Abstract
The production of protons, antiprotons, neutrons, deuterons and tritons in minimum bias p+C interactions is studied using a sample of 385 734 inelastic events obtained with the NA49 detector at the CERN SPS at 158 GeV/c beam momentum. The data cover a phase space area ranging from 0 to 1.9 GeV/c in transverse momentum and in Feynman x from −0.8 to 0.95 for protons, from −0.2 to 0.3 for antiprotons and from 0.1 to 0.95 for neutrons. Existing data in the far backward hemisphere are used to extend the coverage for protons and light nuclear fragments into the region of intranuclear cascading. The use of corresponding data sets obtained in hadron–proton collisions with the same detector allows for the detailed analysis and modelindependent separation of the three principle components of hadronization in p+C interactions, namely projectile fragmentation, target fragmentation of participant nucleons and intranuclear cascading.
Introduction
Baryon and light ion production in protonnucleus collisions has in the past drawn considerable interest, resulting in an impressive amount of data from a variety of experiments. This interest concentrated in forward direction on the evident transfer of baryon number towards the central region, known under the misleading label of “stopping”, and in the far backward region on the fact that the laboratory momentum distributions of baryons and light fragments reach far beyond the limits expected from the nuclear binding energy alone. A general experimental study covering the complete phase space from the limit of projectile diffraction to the detailed scrutiny of nuclear effects in the target frame is, however, still missing. More recently, renewed interest has been created by the necessity of providing precision reference data for the control of systematic effects in neutrino physics.
In addition to and beyond the motivations mentioned above, the present study is part of a very general survey of elementary and nuclear interactions at the CERN SPS using the NA49 detector, aiming at a straightforward connection between the different reactions in a purely experimentbased way. After a detailed inspection of pion [1], kaon [2] and baryon [3] production in p+p interactions, a similar indepth approach is being carried out for p+C collisions. This has led to the recent publication of two papers concerning pion production [4, 5] and this aim is here being extended to baryons and light ions.
The use of the light, isoscalar Carbon nucleus is to be regarded as a first step towards the study of proton collisions with heavy nuclei using data with controlled centrality available from NA49. It allows the control of the transition from elementary to nuclear interactions for a small number of intranuclear collisions, thus providing an important link between elementary and multiple hadronic reactions. It also allows for the cleancut separation of the three basic components of hadronization in p+A collisions, namely projectile fragmentation, fragmentation of the target nucleons hit by the projectile, and intranuclear cascading. The detailed study of the superposition of these components in a modelindependent way is the main aim of this paper. For this end the possibility of defining net proton densities by measuring antiprotons and thereby getting access to the yield of pair produced baryons, will be essential. As the acceptance of the NA49 detector does not cover the far backward region, the combination of the NA49 results with measurements from other experiments dedicated to this phase space area is mandatory. A survey of the sdependence of backward hadron production in p+C collisions has therefore been carried out and is published in an accompanying paper [6]. This allows the extension of the NA49 data set to full phase space.
As the extraction of hadronic cross sections has been described in detail in the preceding publications [1–5], the present paper will concentrate on those aspects which are specific to baryon and light ion production, particularly in the exploitation of the NA49 acceptance into the backward hemisphere. After a short comment on existing double differential data in the SPS energy range in Sect. 2, a few experimental details will be given in Sect. 3 together with the binning scheme adopted for protons, antiprotons and neutrons. Section 4 will present a comprehensive description of particle identification in the backward hemisphere which is an important new ingredient of the optimized use of the NA49 detector in particular for the asymmetric p+A collisions. Section 5 deals with the extraction of the inclusive cross sections and with the applied corrections. Section 6 contains the data tables and plots of the invariant cross sections as well as some particle ratios and a comparison to the few available double differential yields at SPS energy for comparison. Section 7 describes the use of the extensive complementary data set from the Fermilab experiment [7] for the data extension into the far backward direction together with an interpolation scheme allowing for the first time the complete inspection of the production phase space for protons in the range −2<x _{ F }<+0.95. This combined study is extended to deuterons and tritons in Sect. 8. Baryon ratios are shown in Sect. 9. Quantities integrated over p _{ T } are given in Sect. 10 both for minimum bias trigger conditions and for the dependence on the number of measured “grey” protons [4, 8]. In addition, the measured p _{ T } integrated neutron yields are presented in Sect. 10 together with a comparison to other integrated data in the SPS energy range. Section 12 contains a detailed discussion of the twocomponent mechanism of baryon and baryon pair production in p+p collisions, thus covering the first two components of the hadronization process defined above, including a comment on resonance decay and a comparison to a recent microscopic simulation code. Section 13 contains the corresponding experimental results from p+C interactions. Section 14 gives a detailed discussion of antiproton production including the application of the twocomponent mechanism introduced in Sect. 12 and a study of the p _{ T } dependence. The discussion of p _{ T } integrated proton and net proton yields is presented in Sect. 15 followed by the exploitation of double differential proton and net proton cross sections in Sect. 16. The paper is closed by a summary of conclusions in Sect. 17.
The experimental situation
As already pointed out for pions in [4] there are only two sets of double differential inclusive data, for identified baryons and light fragments in p+C collisions in the SPS energy range. The differential inclusive cross sections are presented in this paper as:
with \(x_{F} = 2p_{L}/\sqrt{s}\) defined in the nucleon–nucleon centerofmass system (cms). A first data set [7, 9] covers the far backward direction for protons and light ions at five fixed laboratory angles between 70 and 160 degrees for total lab momenta between 0.4 and 1.4 GeV/c at a projectile momentum of 400 GeV/c. A second set [10] has been obtained in forward direction for 0.3<x _{ F }<0.88 and 0.15<p _{ T }<0.5 with 100 GeV/c beam momentum. The respective phase space coverage in x _{ F } and p _{ T } is shown in Figs. 1a,b for protons and antiprotons, respectively, with a superposition of the NA49 coverage for protons. This coverage is presented in more detail in Fig. 1c and for the antiprotons in Fig. 1d.
With the NA49 data covering lab angles of up to 40 degrees the combination with [7, 9] into a consistent data set becomes possible. This allows for the first time the complete scrutiny of the proton phase space in the range −2<x _{ F }<+0.95, with only minor inter and extrapolation.
Experimental information and binning scheme
As a detailed description of the NA49 detector and the extraction of inclusive cross sections has been given in [1–4, 8], only some basic informations are repeated here for convenience.
Target, “grey” proton detection, trigger cross section and event sample
The NA49 experiment is using a secondary proton beam of 158 GeV/c momentum at the CERN SPS. A graphite target of 1.5 % interaction length is placed inside a “grey” proton detector [4, 8] which measures low energy protons in the momentum range up to 1.5 GeV/c originating from intranuclear cascading in the carbon target. This detector covers a range from 45 to 315 degrees in polar angle with a granularity of 256 readout pads placed on the inner surface of a cylindrical proportional counter. An interaction trigger is defined by a small scintillator 380 cm downstream of the target in anticoincidence with the beam. This yields a trigger cross section of 210.1±2.1 mb corresponding to 91 % of the measured inelastic cross section of 226.3±4.5 mb. This is in good agreement with the average of 225.8±2.2 mb obtained from a number of previous measurements [4]. A total sample of 385.7k events has been obtained after fiducial cuts on the beam emittance and on the longitudinal vertex position.
Acceptance coverage, binning and statistical errors
The NA49 detector [8] covers a range of polar laboratory angles between ±45 degrees with a set of four Time Projection Chambers combining tracking and particle identification, two of the TPC’s being placed inside superconducting magnets. While for antiprotons the accessible range in x _{ F } and p _{ T } is essentially defined by the limited event statistics, it has been possible to completely exploit the available range of polar angle for protons. The corresponding binning schemes are shown in Fig. 2 in the cms variables x _{ F } and p _{ T }.
A rough indication of the effective statistical errors is given by the shading of the bins. Neutrons have been detected in a forward hadronic calorimeter [3] in combination with proportional chambers vetoing charged hadrons. Due to the limited resolution in transverse momentum only p _{ T } integrated information in 8 bins in x _{ F } (Fig. 2c) could be obtained, after unfolding of the energy resolution. This coverage is identical to the one in p+p interactions [3] and allows for direct yield comparison.
Particle Identification
Due to the forward–backward asymmetry of p+A interactions, the study of the backward hemisphere is of major interest for the understanding of target fragmentation and intranuclear cascading. Particle identification at negative x _{ F } is therefore mandatory; it has to rely for the NA49 detector on the measurement of ionization energy loss in the TPC system. This method has been developed and described in detail for mesons and baryons in p+p collisions in [1–3] for x _{ F }>0. A substantial effort has been invested for the present study in its extension to the far backward direction down to the acceptance limit in x _{ F } imposed by the NA49 detector configuration. With decreasing x _{ F } the baryonic lab momentum decreases below the region of minimum ionization where the ionization energy loss increases like 1/β ^{2} and thereby successively crosses the deposits from kaons, pions and electrons. This is shown in Fig. 3 for the the momentum dependence of the parametrization of the mean truncated energy loss used in this analysis.
In terms of x _{ F } and p _{ T }, this crossover pattern reflects into lines of equal energy loss in the x _{ F }–p _{ T } plane as shown in Fig. 4.
The region above the line p–K allows for the standard multiparameter fits of the truncated energy loss distributions as described in the preceding publications [1–4]. The approximately triangular region below the line p–e permits the direct extraction of baryon yields partially even without fitting. This is exemplified in Fig. 5 for two bins at x _{ F }=−0.5 and −0.6 and small p _{ T }.
It is interesting to note that also the light ions deuteron and triton are here well separable practically without background. For antiprotons, a direct measurement of the \(\overline{\mathrm{p}}\)/p ratio becomes feasible down to values below 10^{−3} in this region.
In order to extract proton yields from the energy loss distributions in the intermediate region between the lines p–e and p–K, Fig. 4, the particle ratios in each studied x _{ F }/p _{ T } bin are of prime importance. If the ratios p/π, K/π and e/π are known, proton yields may be obtained from the total number of tracks even in those bins where the proton energy loss equals the one from electrons, pions or kaons. A twodimensional interpolation of the measured particle ratios over the full accessible phase space has therefore been established. These ratios are obtained without problem in the regions below the line p–e and above the line p–K (Fig. 4) as well as in most intermediate bins where a sufficient separation in dE/dx of the different particle species is present. Near the crossover bins the measured ratios show a sharp increase of the effective statistical fluctuations, an increase which has been described in the discussion of the error matrix involved with the multidimensional fitting procedure in [2]. As this effect is of statistical and not of systematic origin, an interpolation through the critical regions in x _{ F } and p _{ T } is applicable.
It should be stressed here that the obtained particle ratios are nonphysical in the sense that they use different phase space regions for each particle mass. For each x _{ F }/p _{ T } bin the necessary transformation to total lab momentum is performed using the proton mass for each track. This means that electrons, pions and kaons from different effective x _{ F } values enter into the proton bin, with an asymmetry that increases with decreasing x _{ F } and p _{ T }. This is quantified in Fig. 6 where the effective mean x _{ F } for electrons, pions and kaons is shown as a function of proton \(x_{F}^{p}\) for two values of p _{ T }.
The lighter particles at small p _{ T } are thus effectively collected from the neighbourhood of x _{ F }=0 with decreasing baryonic x _{ F }. For antiprotons this purely kinematic effect is unfavourable for fitting as the effective \(\overline{\mathrm{p}}\)/π ^{−} ratios quickly decrease below the percent level at low p _{ T }, whereas the p/π ^{+} ratios stay always above about 10 %, increasing rapidly with p _{ T } due to the rather flat number distribution dn/dx _{ F }. Proton and antiproton extraction are therefore regarded separately in the following Sects. 4.1 and 4.2, respectively.
Proton extraction
The problematics of the extraction of the yields of the four particle species e, π, K and p from the measured overall truncated ionization energy loss distributions has been described in detail in the preceding publications [1–5]. In particular the estimation of the corresponding systematic and statistical errors has been treated in Refs. [2, 3]. The following sections describe the extraction of the different particle ratios as they are needed for the determination of the proton and antiproton yields. The statistical errors of the particle ratios shown in the following figures are given by the number of extracted particles per bin and do not contain the additional terms due to the fitting process, see [2, 3] for a detailed explanation. The few percent of data points which exceed the quoted error margins with respect to the twodimensional interpolation are due to these additional, purely statistical fluctuations. They do not influence the quality of the ratio interpolation.
e^{+}/\(\mathbf{\pi}^{+}\) ratio
The crossing of the proton dE/dx through the practically constant electron energy loss at p _{lab}∼1 GeV/c is the least critical effect as the momentum dependence of the proton dE/dx is a steep function of lab momentum in this p _{lab} range and as the e/π ratio quickly decreases with increasing p _{ T }, reaching the 1 % level already at p _{ T }>0.3 GeV/c. The e^{+}/π ^{+} ratio is shown in Fig. 7 as a function of x _{ F } for four values of p _{ T } together with the twodimensional interpolation used.
The hatched area indicates the position of the dE/dx crossover for each p _{ T } value and evidently the ratios may be well interpolated through the small affected x _{ F } regions.
p/\(\mathbf{\pi}^{+}\) ratio
Fitted p/π ^{+} ratios are presented in Fig. 8 for four x _{ F } values together with their twodimensional interpolation as a function of p _{ T }. While the fit results yield stable p _{ T } dependences within their statistical errors in the uncritical regions at x _{ F }=0 and −0.6, the intermediate x _{ F } values at −0.2 and −0.4 show some additional fluctuation in the crossover regions indicated by the hatched areas which combine the p–π and p–K ambiguities.
Evidently the data interpolation describes the ratio properly through the ambiguous p _{ T } areas.
A complete picture over the full available backward phase space is given in Fig. 9 where the fitted p/π ^{+} ratios are shown as functions of x _{ F } for different p _{ T } values together with the interpolations (full lines). The ratios at successive p _{ T } values are shifted by a factor of 2 for clarity of presentation.
The complete situation for the data interpolation is finally presented in Fig. 10 with fixed vertical scale as a function of x _{ F } at different p _{ T } values. Here the acceptance limit of the NA49 detector is given as the broken line together with the region of p–π and p–K ambiguity as hatched area.
This plot again clarifies the way in which the critical crossover areas may be bridged by twodimensional interpolation.
K^{+}/\(\mathbf{\pi}^{+}\) ratio
A situation quite similar to the p/π ^{+} ratio exists for the K^{+}/π ^{+} ratio. Again, there are regions of ambiguity against protons and pions, but the influence of eventual systematic deviations on the extraction of protons is small as the K^{+}/π ^{+} ratios are smaller than the p/π ^{+} ratio by factors between 3 and 10. Figure 11 shows K^{+}/π ^{+} ratios as functions of p _{ T } for four x _{ F } values, where the lowest and highest x _{ F } at −0.6 and 0 allow for unambiguous fits over the full x _{ F } range, whereas the x _{ F } values at −0.2 and −0.4 suffer from p–K and K–π ambiguities in the hatched areas of p _{ T }, with resulting increased statistical fluctuations. The twodimensional interpolation is superimposed as full lines.
All fitted values of K^{+}/π ^{+} are plotted in Fig. 12 as a function of x _{ F } for fixed p _{ T }. As in Fig. 9 the ratios at successive p _{ T } values are shifted by 3 in order to sufficiently separate the measurements.
Figure 13 presents the overview of the interpolated K^{+}/π ^{+} ratios at fixed vertical scale as a function of x _{ F } for fixed values of p _{ T } [GeV/c]. The broken line represents the acceptance limits and the hatched area the region of p–K and K–π ambiguity.
Proton extraction in the far forward region
Due to the gap between the TPC detectors imposed by the operation with heavy ion beams [8], charged particles progressively leave the TPC acceptance region at low p _{ T } for x _{ F }>0.55. Here, tracking is achieved by the combination of a small “gap” TPC (GTPC) in conjunction with two forward proportional chambers (VPC). The performance of this detector combination is described in detail in [3]. In the absence of particle identification in this area one has to rely on external information concerning the combined fraction of K^{+} and π ^{+} in the total charged particle yield. Several considerations help to establish reference values for the (K^{+}+π ^{+})/p ratios:

The (K^{+} + π ^{+})/p ratios decrease very rapidly with increasing x _{ F } at all p _{ T }, from about 10 % at x _{ F }=0.6 to less than 1 % at x _{ F }=0.9. Possible deviations from the used external reference data therefore introduce only small systematic effects in the extracted proton yield.

Existing data may be used to come to a consistent estimation of the particle ratio. Direct measurements from Barton et al. [10] in p+C interactions cover the region from x _{ F }=0.2 to 0.8 for p _{ T }=0.3 and 0.5 GeV/c. Although the published invariant cross sections show sizeable deviations from the NA49 results, see Sect. 6.5, the particle ratios of the two experiments compare well.

The ratios also comply with measurements in p+p collisions, both from NA49 [1–3] and from Brenner et al. [11] at 100 and 175 GeV/c beam momentum.
An overview of the experimental situation is given in Fig. 14 which shows the available measurements of the (K^{+}+π ^{+})/p ratio as a function of x _{ F } for eight values of p _{ T } between 0.1 and 1.3 GeV/c. The full lines give the combination of the NA49 data with Fermilab and ISR data in p+p interactions as interpolated in [3], the open squares the p+p data of [11]. An impressive consistency on an about 10 % level between the experimental results from the two different reactions is apparent. This allows for a safe extrapolation into the region above x _{ F }=0.6 where particle identification via dE/dx is not available.
The interpolated (K^{+}+π ^{+})/p ratios are again presented in Fig. 15, here as a function of p _{ T } for several values of x _{ F } between 0.3 and 0.9. The limits of dE/dx identification and NA49 acceptance are given by the broken and dotted lines, respectively.
This figure demonstrates that the (K^{+}+π ^{+})/p ratios show only a small dependence on p _{ T }. They are of order 10 % at the limit of the dE/dx identification and decrease rapidly to the 1 % level at x _{ F }=0.9. This implies that possible systematic differences between p+p and the p+C interactions in the extrapolated region should have effects on the percent level and below concerning the extracted proton yields.
The equality of the meson/baryon ratio between p+p and the p+C interactions may be taken as a first physics result of this paper. It has two aspects: Firstly, 60 % of the minimum bias p+C interactions correspond to single projectile collisions inside the nucleus [5]. These collisions should indeed produce particle ratios equivalent to p+p interactions. Secondly, the phenomenon of “stopping”, that is of the transfer of particle yields in multiple interactions towards the central region, is not limited to baryons but applies also to mesons [4, 5]. Hence again an expected similarity in the meson/baryon ratios.
Antiproton extraction
As stated above the extension of the determination of antiproton yields into the backward hemisphere suffers from the fact that the \(\overline{\mathrm{p}}\)/π ^{−} and \(\overline{\mathrm{p}}\)/K^{−} ratios decrease with decreasing x _{ F }. This is shown by the energy loss distributions of two typical bins in x _{ F } and p _{ T } in Fig. 16.
This effect is largely due to the asymmetry between the effective x _{ F } for light particles and antiprotons due to the transformation to the lab momentum using proton mass, see Fig. 6. Thus at \(x_{F}^{\overline{\mathrm{p}}}=0.2\) pions are sampled close to maximum yield whereas the antiproton cross section is steeply decreasing.
While the extraction of pion yields therefore presents no problem in this phase space region, the fits of kaon and antiproton densities become strongly correlated with sizeable uncertainties in their relative position on the energy loss scale. The combined (\(\mathrm{K}^{} +\overline{\mathrm{p}}\)) yields however stay well defined with respect to the pions. This is shown by the fitted (\(\mathrm{K}^{} +\overline{\mathrm{p}}\))/π ^{−} ratios of Fig. 17.
In order to resolve the K^{−}–\(\overline{\mathrm{p}}\) ambiguity, the high statistics data on \(\overline{\mathrm{p}}\) production in p+p interactions [3] in order to fix the position of the K^{−} and \(\overline{\mathrm{p}}\) peaks in the corresponding dE/dx distributions. In this symmetric configuration, the measured \(\overline{\mathrm{p}}\) cross sections may be reflected into the backward hemisphere and thereby the correlation between the positions of the K^{−} and \(\overline{\mathrm{p}}\) peaks extracted. The positions of these peaks is expressed as their systematic deviations in the dE/dx variable from the Bethe–Bloch parametrization, \(\delta_{\overline{\mathrm{p}}}\) and \(\delta_{\mathrm{K}^{}}\), in units of minimum ionization. As shown in Refs. [2, 3] these shifts are experimentally determined with an accuracy of about 0.001 in the scale of minimum ionization. The correlation is shown in Fig. 18 for an example at x _{ F }=−0.1 for fixed values of p _{ T } between 0.3 and 0.9 GeV/c, also indicating the corresponding \(\overline{\mathrm{p}}\)/π ^{−} ratios.
Using the same correlation for the p+C data, effective \(\overline{\mathrm{p}}\)/π ^{−} ratios are obtained. The observed stability of these ratios over the full range of the correlations is a strong test of the validity of the method.
Figure 19 presents the obtained \(\overline{\mathrm{p}}\)/π ^{−} ratios as a function of p _{ T } for x _{ F }=−0.05, −0.1 and −0.15, together with the directly fitted values at x _{ F }=0. Full lines: twodimensional interpolation of the ratios.
A complete picture of the \(\overline{\mathrm{p}}\)/π ^{−} ratios used in this analysis is given in Fig. 20 as a function of x _{ F } which combines the directly fitted ratios in the forward hemisphere with the ones obtained using the reflection method described above in the backward hemisphere.
Note that the values at x _{ F }=−0.2 are obtained by extrapolation following the broken lines. Note also that the applied method allows the extraction of the ratios in the percent and subpercent region.
Evaluation of invariant cross sections and corrections
The invariant cross section,
is experimentally determined by the measured quantity [1]
where Δp ^{3} is the finite phase space element defined by the bin width with x _{ F } and p _{ T } being defined in the bin center.
As described in [1] several steps of normalization and correction are necessary in order to make f _{meas}(x _{ F },p _{ T },Δp ^{3}) approach f(x _{ F },p _{ T }). The determination of the trigger cross section and its deviation from the total inelastic p+C cross section have been discussed in [4]. The following corrections for baryons have been applied and will be discussed below:

treatment of the empty target contribution

effect of the interaction trigger

feeddown from weak decays of strange particles

reinteraction in the target volume

absorption in the detector material

effects of final bin width
Empty target contribution
This correction has been determined experimentally using the available empty target data sample, as described in [4]. The resulting correction is essentially determined by the different amounts of empty events in full and empty target condition. It is within errors p _{ T } independent and equal for protons and antiprotons. It increases from about 2 % in in the far forward direction to about 7 % in the most backward region as shown in Fig. 21.
Effect of the interaction trigger
Due to the high trigger efficiency of 93 % [4] this correction is small compared to p+p interactions [1]. It has been determined experimentally by increasing the diameter of the trigger counter using the accumulated data. Within its statistical uncertainty it is independent of p _{ T } and similar for protons and antiprotons. Its x _{ F } dependence as shown in Fig. 22 is following the expected trend [3] where the fast decrease in forward direction as compared to p+p collisions is due to the lower particle yields at high x _{ F }. Note that the slope of the x _{ F } dependence for antiprotons corresponds to the one for protons. Both corrections have to increase in backward direction due to the effects of hadronic factorisation, see also [1].
Feeddown correction
The hyperon cross sections relative to p+p collisions established in [4] for x _{ F }>0 have been used. These cross section ratios approach at x _{ F }<0 the expected factor of 1.6 corresponding to the number of intranuclear projectile collisions, in account of the fact that for Λ and \(\overline{\varLambda}\) there is no isospin effect [12]. For the contribution from target fragmentation this ratio should be constant into the backward hemisphere. For the determination of the feeddown correction the corresponding yields have to be folded with the onvertex baryon reconstruction efficiency which reaches large values in the far backward hemisphere. The resulting correction in percent of the total proton yield drops however quickly below x _{ F }<−0.2 due to the decrease of the Λ cross section relative to protons and due to the fact that the important baryon contribution from intranuclear cascading has no hyperon content. The numerical values in percent of the baryon yields are shown in Fig. 23 as a function of x _{ F }.
In comparison to the pion data [4] this correction reaches considerable values of up to 20 % for the antiprotons and therefore constitutes, together with the absolute normalization, the most important source of systematic uncertainty.
Reinteraction in the target
The carbon target has an interaction length of 1.5 %, which corresponds to about half of the length of the hydrogen target used in p+p collisions. The expected reinteraction correction is therefore smaller than +0.5 % in the forward and −2 % in the backward hemisphere. The values obtained in [3] have therefore been downscaled accordingly.
Absorption in the detector material
The absorption losses in the detector material are equal to the ones obtained in [3]. Baryons in the newly exploited region in the far backward direction feature short track lengths in the first NA49 TPC detector only and are not affected by any support structures; hence the corresponding corrections are below the 1 % level as shown in Fig. 24.
Binning correction
The correction for finite bin width follows the scheme developed in [1] using the local second derivative of the particle density distribution. This correction stays, despite of the rather sizeable bins used in some areas of the p+C data, generally below the ±2 % level, being negligible in the x _{ F } coordinate for protons due to their rather flat dn/dx _{ F } distribution. Two typical distributions of the p _{ T } correction for protons and for the x _{ F } correction for antiprotons are shown in Fig. 25 both for the nominal bin width of 0.1 GeV/c in p _{ T } and 0.05 in x _{ F } and for the actually used bin widths.
Systematic errors
An estimation of the systematic errors induced by the absolute normalization and the applied corrections is given in Table 1. For the proton and antiproton extraction in the newly exploited backward regions an additional systematic error due to particle identification is indicated. An upper limit of 7.0 % (8.5 %) for protons (antiprotons) results from the linear addition of the error sources, increasing to 10 % (14.5 %) in the backward region. Quadratic summation results in the corresponding values of 3.7 % (4.2 %) and 4.7 % (7.3 %). Note that even the upper error limits given by the extreme and improbable case of linear addition stay below a ten percent margin for the charged baryons. The distribution of the numerical values of the corrections in all measured bins is shown in Fig. 26 for protons.
Results on doubledifferential cross sections for p and \(\overline{\mathrm{p}}\)
Data tables
The binning scheme presented in Sect. 3 results in 491 and 121 data values for protons and antiprotons, respectively. These are presented in Tables 2 and 3.
Data interpolation
As in the preceding publications concerning p+p [1–3] and p+C [4] interactions, a twodimensional interpolation is applied to the data. This interpolation has several aims:

It should reduce the local statistical data fluctuations by correlating several data points in the neighbourhood of each measured cross section, imposing the physics constraints of smoothness and continuity.

It should ensure stability at the boundaries of the covered phase space regions.

It should allow for an eventual slight extrapolation beyond the measured regions taking full account of the corresponding physics constraints. As an example the extrapolation to p _{ T }=0 is strongly constrained by the fact that the invariant cross sections should approach this point with slope zero.

It should allow the creation of a fine grid of interpolated values that may serve as a reference for the comparison of the yields of different particle species in the same hadronic collision or for the comparison of different types of hadronic interactions.
The problem of analytic representation
A look at Figs. 28, 29 and 30 shows that on the level of precision and completeness achieved by the present experiment, the measured cross sections show complex shapes both in their p _{ T } and in their x _{ F } dependences. These shapes exclude the description of the data with straightforward analytic functions unless a complex array of rapidly varying fit parameters would be established, with heavy constraints in order to fulfil the physics boundary conditions. There is a vast literature using simple parametrizations like single or double exponential fits or transverse mass (m _{ T }, see Sect. 6.4) fits for hadronic p _{ T } distributions, and power law distributions of the type (1−x _{ F })^{n} for the x _{ F } dependences. Although these approaches have been claimed to carry physics relevance in terms of the concept of a fixed “hadronic temperature” in the case of transverse momentum or “counting rules” for the x _{ F } distributions in a purported connection to quark or even gluon structure functions, their impact on the understanding of soft hadronic physics has been doubtful to say the least. In the preceding publications [1–5] it has been shown that the shape of transverse momentum distributions against transverse mass disproves the concept of a constant hadronic “temperature” both in p+p and in p+C interactions, see also Sect. 6.4 below. In particular in Ref. [2] a detailed confrontation with the effects of the decay of known resonances, in contrast to the assumption of a “thermodynamic” behaviour, has been discussed.
In view of this problematics, an alternative arithmetic approach to the twodimensional interpolation is eventually given by cubic spline fits. These fits would of course, in terms of an analytic description, at best offer a vast matrix of parameters concerning the locally used thirdorder polynomials. In addition, the necessary introduction of the physics constraints and boundary conditions would weigh heavily against the practicability of such an approach. The human eye, on the other hand, offers a welcome capability to perform interpolation which is easily guided by the physics constraints mentioned above. This approach is described below.
Multistep recursive eyeball fits
The data shown in Tables 2 and 3 have statistical errors between 2 % and about 30 % with distributions shown in Fig. 27a for p and in Fig. 27b for \(\overline{\mathrm{p}}\). The corresponding mean values are 8 % and 12 %, respectively. With these error margins it is no problem to produce interpolations via eyeball fits with a precision of a fraction of the error bars, using an appropriate scale for the invariant cross sections. These interpolations have to describe the data simultaneously both in the p _{ T } and x _{ F } variables. An iterative, recursive method is therefore applied in both dimensions. The quality of this eye fit procedure may be judged by plotting the distribution of the differences between the data points and the interpolation, normalized by the statistical errors (normalized residuals). These distributions should be Gaussians centred close to zero, as unlike in algebraic fits the center at zero is not enforced, and with a variance close to unity if the statistical errors are correctly estimated and no additional systematics is introduced by the fit procedure.
Statistical and correlated errors
As described above in Sect. 4, an interpolation of particle ratios has been used in part of the backward phase space in order to allow for the extraction of proton and antiproton yields in regions where particle identification via fits to the ionization energy loss distributions are not reliable. In these regions the statistical errors become correlated and are in principle not any more directly related to the number of extracted particles in each bin. The regions of direct dE/dx analysis and of the interpolation of particle ratios have therefore been separated and the normalized residuals are shown in Fig. 27 in corresponding separate number distributions.
The uncorrelated residual distributions, Figs. 27c and d, are described by Gaussian fits with means of 0.01±0.07 for protons and 0.23±0.12 for antiprotons, corresponding with respect to the mean statistical errors to less than 1 % for protons and 2.7 % for antiprotons. Both values are within two standard deviations with respect to the fit errors. The variances of 1.14±0.06 and 0.73±0.14 are also within about two standard deviations from the expected values of unity. The correlated residual distributions, Figs. 27e and f, are centred within 2.7 standard deviations or 2 % for the protons and less than one standard deviation or 0.5 % for the antiprotons. In both cases, however, the variances are smaller than in the uncorrelated samples. While this difference is only on the one standard deviation level for the protons, it is statistically significant for the antiprotons. It should be mentioned here that in the multiparameter fits applied to the truncated energy loss distributions for the extraction of particle yields, additional error sources of statistical origin appear which depend on the relative particle yields in each bin as well as on the position of each particle on the overall BetheBloch parametrization. This effect has been elaborated in detail in Refs. [2, 3] where it has been demonstrated that an increase of the effective statistical errors over the \(1/\sqrt{N}\) estimator, where N is the number of extracted particles per bin, by several tens of percent is to be expected in certain cases. The deviations observed in Figs. 27c and d are therefore within reasonable error margins.
Concerning the reduced variance of Fig. 27f it has been decided to keep the errors given in Table 3 at the level of the estimator \(1/\sqrt{N}\) in order to absorb eventual systematic effects originating in the particle ratio interpolation.
Tabulation of the interpolated cross sections
A complete set of interpolated cross sections can be found on the web page “spshadrons” [13] in steps of 0.05 GeV/c in p _{ T } and for all x _{ F } values used in this publication. Comparable sets of cross sections are given in [13] for all other investigated particle types and interactions. As an example Table 4 gives a limited list of interpolated proton cross sections for the 22 x _{ F } values at x _{ F }≥0 established in this paper. The lines through the data points corresponding to the interpolation are obtained using the smoothed interpolation procedure described in the ROOT program package [14]. It should be mentioned here that the region below p _{ T }=0.05–0.1 GeV/c covered by the data has been extended to p _{ T }=0 GeV/c by extrapolation using the physics constraint of zero slope at this point. A slight extrapolation in the high p _{ T } region has also been applied using the basically exponential behaviour of the cross sections in this area. As far as the coverage of the high x _{ F } region at low p _{ T } which is outside the NA49 acceptance is concerned, see the argumentation given in Sect. 6.3.
Dependence of the invariant cross sections on p _{ T } and x _{ F }
The distribution of the invariant cross section as a function of p _{ T } is shown in Fig. 28 for protons and antiprotons at negative x _{ F } and in Fig. 29 at positive x _{ F }, indicating the data interpolation by full lines. For better visibility successive values in x _{ F } have been multiplied by a factor 0.5.
Corresponding x _{ F } distributions are presented in Fig. 30 for protons and in Fig. 31 for antiprotons.
The shape of the p _{ T } distributions resembles, for x _{ F }≥0 (Fig. 29), the one measured in p+p interactions [3] including details of the deviation from either exponential or Gaussian shape. In backward direction, Fig. 28, a more complex behaviour develops with a steepening up at x _{ F }<−0.4. The basic asymmetry of the p+C interaction is more directly visible in the x _{ F } distributions of Figs. 30 and 31. While at high p _{ T } factors of 1.6–2 are typical between the backward and forward proton yields at x _{ F }=0.5–0.7, these factors grow to about 3–5 at p _{ T }=0.1 GeV/c. This allows a first view at the composition of p+A collisions from projectile fragmentation in forward direction and target fragmentation as well as intranuclear cascading in backward direction. A quantification and separation of these three basic ingredients will be performed in Sects. 14, 15 and 16 below. For antiprotons the x _{ F } distributions clearly peak at negative x _{ F }. The forward–backward asymmetry is, at x _{ F }=0.2, to first order p _{ T } independent and on the order of 1.6–1.9 which is well above the asymmetry of protons at this x _{ F } indicating important effects from isospin and baryon number transfer.
A remark concerning the behaviour of the proton cross sections at x _{ F }>0.8 is in place here. In this region a clear diffractive peak becomes visible which is in shape equal to the one observed in p+p interactions [3]. This peak is to be expected from single projectile collisions in the target nucleus which amount to about 60 % of all inelastic p+C interactions [5]. In the absence of comparable measurements in the low p _{ T } region the relative shape of the extrapolated lines in the inaccessible area of phase space has been adjusted, after renormalization, to the one extracted in [3] from existing p+p data. This extrapolation is indicated by the broken line segments in Fig. 30.
Rapidity and transverse mass distributions
The rapidity distribution for protons at fixed p _{ T } presented in Fig. 32 extends to the kinematic limit in forward direction and to −2.6 units in the target hemisphere. Again a clear view of the asymmetry of the p+C interactions increasing with decreasing p _{ T } is evident.
The rapidity range of antiprotons is limited by statistics to −1.4 to +1.8 units. The corresponding distribution as a function of y for fixed p _{ T } is shown in Fig. 33.
Transverse mass distributions at y=0, with \(m_{T} = \sqrt{m_{p}^{2} + p_{T}^{2}}\), are presented in Fig. 34 together with the local inverse slopes obtained by exponential fits to three subsequent points. A situation very similar to p+p collisions emerges with a nonexponential behaviour and inverse slope parameters varying systematically by up to 60 MeV with the transverse mass.
Comparison to other experiments
As stated in Sect. 2 there are only two experiments providing double differential data in the SPS energy range. The data set [7] which is disjoint from the NA49 phase space coverage will be discussed in detail in the next Sect. 7. As far as the Fermilab data of Barton et al. [10] are concerned there are 10 data points for protons and 4 data points for antiprotons available in overlapping phase space ranges. The situation for protons is shown in Fig. 35 where the invariant cross sections [10] (full circles) at p _{ T }=0.3 and 0.5 GeV/c are shown together with the measurements (open circles) and data interpolation (full lines) of the NA49 experiment as a function of x _{ F }.
The comparison between the two experiments reveals very sizeable systematic offsets with an average of +21 % or +6 standard deviations averaged over all data points. This complies with the comparison of pion yields [4] with an average of +25 % or +3.6 standard deviations. The good agreement between the particle ratios (K^{+}+π ^{+})/p demonstrated in Sect. 4.1.4 over the full comparable range of x _{ F } and p _{ T } speaks indeed for a normalization problem as the origin of the discrepancies which are not visible in the results of p+p interactions [3].
For antiprotons the situation is considerably less clear due to the very large statistical errors of the data [10] indicating only upper limits for some of the measurements. Figure 36 gives the x _{ F } dependence of these data for p _{ T }=0.3 GeV/c together with the NA49 interpolation (full line) which has been partially extrapolated using an exponential shape. The large upward shift of the Fermilab data of about a factor of 2 (dashed line in Fig. 36) is compounded by the fact that due to the lower beam momentum of 100 GeV/c these data should be expected to be about 30–40 % below the NA49 cross sections [3].
In this context it should be mentioned that already in p+p collisions the Fermilab data [11] were high by about +25 % for antiprotons.
Data extension into the far backward direction
As the backward acceptance of the NA49 detector is limited to the ranges of x _{ F }>−0.8 to x _{ F }<−0.5 at low and high p _{ T }, respectively, it is desirable to extend this coverage into the far backward region to x _{ F } values down to and below −1. A detailed survey of existing experiments in the backward direction of p+C interactions has therefore been undertaken and is being published in an accompanying paper [6]. This survey establishes the detailed sdependence of measured cross sections for beam momenta between 1 and 400 GeV/c, for lab angles between 10 and 180 degrees, and for lab momenta between 0.2 and 1.2 GeV/c. It shows in particular that the baryon cross sections in the SPS energy range from about 100 to 400 GeV/c beam momentum may be regarded as sindependent within tight systematic limits of less than two percent [6]. This allows the combination of the extensive data set of the Fermilab experiment [7] at 400 GeV/c beam momentum and lab angles between 70 and 160 degrees with the NA49 data which span the angular range up to 40 degrees.
The relevant kinematic situation is presented in Fig. 37 where lines of constant p _{lab} and Θ _{lab} are shown in the x _{ F }/p _{ T } plane.
In the necessary transformation between the lab and cms frames involved in Fig. 37 there is very little difference between the beam momenta of 158 and 400 GeV/c. This is shown in Fig. 38 which gives the difference in x _{ F } as a function of p _{lab} for the angular range between 70 and 160 degrees.
One example of the apparent sindependence of the backward baryon yields is shown in Fig. 39 which compares data at Θ _{lab}=162 and 160 degrees for 8.5 [15] and 400 GeV/c beam momentum [7].
Due to the flat angular distribution at Θ _{lab} around 160 degrees, see Fig. 41, the small angular difference in angle between the two measurements has negligible influence on the cross sections comparison. Also the SPS measurements of “grey” protons by Braune et al. [16] show no dependence on beam momentum in the range from 50 to 150 GeV/c over the complete Θ _{lab} range from 10 to 159 degrees.
NA49 results at fixed Θ _{lab} and p _{lab} combined with the data from [7]
The kinematic situation presented in Fig. 37 shows that the NA49 acceptance allows the measurement of proton yields as a function of p _{lab} up to Θ _{lab}=40 degrees. The corresponding data values are tabulated in Table 5. These data are shown in Fig. 40 together with the Fermilab data [7] as a function of p _{lab}.
Evidently the two data sets are complementary and offer for the first time an almost complete angular coverage of the backward proton production with double differential cross sections.
A twodimensional data interpolation has been performed as shown by the full lines in Fig. 40. This allows to produce the combined angular distribution as a function of cos(Θ _{lab}) for fixed values of p _{lab} presented in Fig. 41.
The proton density distributions dn _{ p }/dp _{lab} derived from the interpolated invariant cross sections are shown as a function of p _{lab} in Fig. 42, normalized to unit area.
These distributions are closely similar for 160>Θ _{lab}>118 degrees and develop a tail to large p _{lab} values for angles smaller than 90 degrees indicating increasing contributions from the fragmentation of the participant nucleons hit by the projectile. The “grey” proton momentum distribution measured in the EHS rapid cycling bubble chamber [17], interpolated in steps of p _{lab} of 0.1 GeV/c, are shown as full circles in Fig. 42. It is closely tracing the result at Θ _{lab}=90 degrees. In this case a strong momentum cut is introduced by requesting bubble densities at 1.3 minimum ionizing rejecting most of the faster forward region.
The dn _{ p }/dp _{lab} distributions shown in Fig. 42 may be integrated over p _{lab} resulting in the proton densities dn/dΩ shown in Fig. 43 as a function of cos(Θ _{lab}). Here the integration has been limited to 0<p _{lab}<1.6 GeV/c as at low angles the target fragmentation contribution will create a divergent behaviour and since the comparison data do not contain this component.
The direct measurements from [16] also presented in Fig. 43 show systematic deviations both at forward and at backward angles. As this experiment uses an energy loss measurement with variable threshold it is not clear to which extent it represents identified proton yields. The authors in fact explain that a contribution from “evaporation” particles (“black tracks” in emulsion work) cannot be excluded. Such a contribution would typically be characterized by a flatter angular distribution as compared to protons, see also the discussion on light ions in Sect. 8 showing very sizeable d/p ratios. As the d/p and t/p ratios decrease steeply with increasing x _{ F }, see Fig. 45, the yield measured by [16] would increase at Θ _{lab}>90^{∘} and decrease towards small angles with respect to the one of identified protons. In addition, a dE/dx cutoff in the detector of [16] at p _{lab}∼0.2 GeV/c will reduce the measured yields as a function of angle, see Fig. 42.
Double differential cross section f(x _{ F },p _{ T }) as a function of x _{ F }
The invariant cross sections measured in p _{lab} and Θ _{lab} may be transformed into the x _{ F }/p _{ T } variables following the kinematics shown in Fig. 37. The corresponding x _{ F } distributions at fixed p _{ T } are presented in Fig. 44 which shows the x _{ F } range down to −2.0. Both the NA49 data (full circles) and the Fermilab results (open circles) are plotted. The full lines in Fig. 44 represent the interpolation of the two data sets also covering the nonmeasured angular region between 40 and 70 degrees, see Fig. 41. The thin lines indicate the position of the lab angles of 10, 30, and 50 degrees as well as the five angles measured by [7].
Figure 44 represents one of the main results of this paper. It shows for the first time a complete coverage of the baryonic phase space in p+A collisions, from x _{ F }=−2 up to the kinematic limit for the projectile fragmentation at x _{ F }∼+1. Several features merit comment:

The invariant proton cross sections extend far below the kinematic limit for target fragmentation at x _{ F }=−1.

There is no indication of a diffractive structure with a peak at x _{ F }∼−1 as it would be expected from the prompt fragmentation of the hit target nucleons—on the other hand, at x _{ F }>+0.9 there is a diffractive peak in the projectile fragmentation region, see [3] for comparison with p+p interactions.

The backward cross sections peak at x _{ F }∼−0.9, not at x _{ F }∼−1 indicating a sizeable longitudinal momentum transfer in the nuclear fragmentation region.

At low p _{ T } or low transverse momentum transfer however, the lines of constant lab angle are compatible as expected with a convergence towards x _{ F }=−1.
A detailed discussion of these features including the decomposition of the measured proton yields into the basic components of projectile, target and nuclear fragmentation, is presented in Sects. 15 and 16.
Light ions: deuterons and tritons
As shown in Sect. 4, Fig. 5, the particle identification via energy loss measurement in the NA49 TPC system also allows the extraction of deuteron and triton yields. The accessible kinematic region covers lab momenta from the detector acceptance limit at about 0.25 GeV/c up to the crossing of the energy loss distributions with the ones for electrons, Fig. 3, at about p _{lab}=2 GeV/c for deuterons and 3 GeV/c for tritons.
As for the proton cross sections, this range is complementary to the Fermilab experiment [9] which gives light ion cross sections in the lab angular range from 70 to 160 degrees, at p _{lab} from 0.5 to 1.3 GeV/c for deuterons and from 0.7 to 1.3 GeV/c for tritons. The NA49 data offer the advantage of reaching low p _{ T } down to 0.1 GeV/c and of covering the forward region from Θ _{lab}=40 degrees down to about 3 degrees. This allows for the first time to trace the extension of nuclear fragmentation into light ions towards the central region of particle production.
Ion to proton ratios
In order to clearly bring out the last aspect mentioned above the deuteron and triton yields are given here as ratios to the proton yields in each bin of p _{lab} and Θ _{lab},
These density ratios are given as functions of x _{ F } and p _{ T } using the proton mass in the transformation from lab to cms variables. They thus give directly the relative contribution of the light ions with respect to protons in the x _{ F }/p _{ T } bins shown in Fig. 2 and Table 2. In forming the ion/proton density ratios, most of the data corrections, Sect. 5, drop out with the exception of absorption which is small but increased for ions, and of hyperon feeddown which is of course only applicable to protons. The resulting ratios are shown as functions of x _{ F } and p _{ T } in Table 6 for deuterons and in Table 7 for tritons. Most of the systematic errors cancel in the ratios of Tables 6 and 7, with the exception of the feeddown (only for protons) and the detector and target absorption. The resulting systematic uncertainty has been estimated to less than 3 % for deuterons and less than 5 % for tritons which is small compared to the given statistical errors.
In these data tables the cutoffs imposed by the NA49 acceptance at Θ _{lab}∼40 degrees below x _{ F }∼−0.5 and by the upper limit on p _{lab} imposed by the energy loss measurement at x _{ F }≳−0.5 are discernible. In addition the fast decrease of the ratios towards higher x _{ F } limits the extraction of tritons due to the low overall event statistics.
Comparison to the Fermilab data [9]
The density ratios R _{ d }(x _{ F },p _{ T }) and R _{ t }(x _{ F },p _{ T }) are presented in Fig. 45 as a function of x _{ F } in comparison to the Fermilab data which are available above p _{ T }∼0.3 GeV/c.
As for the proton data, the good consistency with the Fermilab data in the p _{ T } range above 0.3 GeV/c is confirmed for R _{ d } by the twodimensional data interpolation performed by eyeball fits and shown as the full lines in Fig. 45. The density ratio R _{ t } shows a similar consistency with [9] over the smaller available region of comparison due to the higher p _{lab} cutoff in the Fermilab data. With respect to R _{ d }, R _{ t } is suppressed by a factor of 0.1 to 0.2 depending on p _{ T } but within statistics independent of x _{ F }. This is demonstrated by the broken lines in Fig. 45 which represent the interpolation of R _{ d } with the ratio R _{ t }/\(R_{d}^{\mathrm{interpol}}\), assumed x _{ F } independent, given as a function of p _{ T } in Fig. 46.
x _{ F } and p _{ T } dependences
The x _{ F } dependences of the density ratios presented in Fig. 45 show a rather complex behaviour. Evidently deuterons and tritons, if seen as nuclear fragments as opposed to coalescing from produced baryons, reach far towards central production. In consequence the separation of nuclear fragmentation and coalescence is not an easy especially as fragmentation products, as shown by the tentative extrapolation of the data interpolation towards x _{ F }=−0.1, might well represent a contribution in the subpercent range even at x _{ F }=0 and already for the light Carbon nuclei at SPS energy. The p _{ T } dependence of R _{ d } at fixed x _{ F } is as well nontrivial, as shown in Fig. 47.
Evidently R _{ d } tends to decrease with increasing p _{ T } for x _{ F }>−0.8 and with an inverted tendency for x _{ F }<−0.8. The R _{ t }/R _{ d } ratio on the other hand clearly increases with p _{ T } at all available x _{ F } values, see Fig. 46.
Particle ratios
The already published data on p+C [4, 5] and p+p [1–3] interactions allow for a very detailed study of particle ratios. In a first overview baryonic ratios will be investigated in this section, both concerning antiproton/proton ratios in elementary and nuclear collisions,
and baryon density ratios directly comparing p+C and p+p reactions,
Figure 48 shows \(R_{\overline{\mathrm{p}}\mathrm{p}}^{\mathrm{pC}}\) (closed circles) and \(R_{\overline{\mathrm{p}}\mathrm{p}}^{\mathrm{pp}}\) (open circles) together with the corresponding ratios of the data interpolation (full and broken lines) as a function of x _{ F } for several bins of p _{ T }.
This comparison reveals that the ratios are within errors equal in the projectile hemisphere x _{ F }≳0.1 with the exception of the two highest p _{ T } bins. This means that the transfer of projectile baryon number (“stopping”) towards the central region is equal for protons and for antiprotons. In the backward hemisphere there are distinct differences between p+C and p+p interactions at low to medium p _{ T }. This is a result of isospin effects between the isoscalar C and the p targets. In fact it is known that the antiproton yields increase and the proton yields decrease in neutron fragmentation [12] with both effects increasing \(R_{\overline{\mathrm{p}}\mathrm{p}}^{\mathrm{pC}}\) compared to \(R_{\overline{\mathrm{p}}\mathrm{p}}^{\mathrm{pp}}\). The clean extraction of \(\overline{\mathrm{p}}\) and p yields in the far backward direction, x _{ F }<−0.4, see Sect. 4 and Fig. 5, allows the extension of \(R_{\overline{\mathrm{p}}\mathrm{p}}^{\mathrm{pC}}\) to the x _{ F } range −0.7<x _{ F }<−0.5. This is presented in Fig. 49 in the p _{ T } interval 0.1<p _{ T }<0.4 GeV/c.
The broken line represents \(R_{\overline{\mathrm{p}}\mathrm{p}}^{\mathrm{pp}}\) [3], the full line the measured \(R_{\overline{\mathrm{p}}\mathrm{p}}^{\mathrm{pC}}\). The expected increase of the \(\overline{\mathrm{p}}\) yield by a factor of 1.7 (\(\overline{\mathrm{p}}\) increase by a factor of 1.33 [12] and p decrease by a factor of 1.3 [3]) is indicated by a hatched area assuming a 5 % uncertainty in the respective factors. The fact that the measured backward ratio follows closely the expectation from target fragmentation shows that there is no \(\overline{\mathrm{p}}\) production from nuclear cascading. This is in agreement with the upper limit of \(R_{\overline{\mathrm{p}}\mathrm{p}}^{\mathrm{pC}}\) of 10^{−4} to 10^{−5} given in [18] for p+^{181}Ta at 90 degrees laboratory angle.
In contrast to the \(\overline{\mathrm{p}}\)/p ratios discussed above, the baryon yields proper exhibit an important evolution when passing from p+p to p+C interactions. This is presented as functions of x _{ F } for fixed values of p _{ T } in Fig. 50 for R _{p} and in Fig. 51 for \(R_{\overline{\mathrm{p}}}\).
Looking first at R _{p}, Fig. 50, where the data give access to a very wide range of x _{ F }, three distinct zones may be distinguished.
A first area is governed by the projectile fragmentation, x _{ F }≳0.1. Here the transfer of baryon number from the forward to the central region is clearly evident, with a suppression of the far forward yield by a factor of 0.6 at low to medium p _{ T } followed by a steady increase of proton density with increasing p _{ T } until the densities exceed the p+p values at all x _{ F } for p _{ T }>1 GeV/c.
A second area is characterized by the fragmentation of the target nucleons hit by the projectile, −0.5<x _{ F }<0. Here the pileup of produced hadrons in the central area due to the 1.6 mean projectile collisions in the C nucleus is visible, followed by a steady decrease of proton density in the backward direction due to the contribution of neutron fragmentation.
A third component is characterized by the steep increase of proton density for x _{ F }<−0.2, at low to medium p _{ T }. This region is governed by the intranuclear cascading of baryons (“grey” protons) in the lab momentum range up to about 2 GeV/c. This component dies out as expected with increasing transverse momentum.
Due to the smaller x _{ F } range experimentally available for the antiprotons, the corresponding ratio \(R_{\overline{\mathrm{p}}}\) is more restricted. It has however been demonstrated (Fig. 49) that here no cascading component exists. As argued above, the evolution of the projectile fragmentation (x _{ F }≳0.1) follows closely the one for protons including the increase with transverse momentum. As far as the target fragmentation is concerned, the increase of antiproton density beyond the pileup from the 1.6 average projectile collisions to about a factor of 2 is expected from isospin symmetry.
A further, more detailed argumentation concerning this phenomenology can be found in the discussion Sect. 14 below.
Integrated data
p _{ T } integrated distributions
The p _{ T } integrated noninvariant and invariant yields are defined by:
with f=E⋅d ^{3} σ/dp ^{3}, the invariant double differential cross section. The integrations are performed numerically using the twodimensional data interpolation (Sect. 6.2) in the range 0<p _{ T }<1.9 GeV/c. Tables 8 and 9 give the numerical values and the first and second moments of the p _{ T } distributions as functions of x _{ F } and rapidity for protons and antiprotons, respectively. The relative errors quoted are given in percent using the full statistical errors of the measured points. They thus present upper limits as the data interpolation in x _{ F } will reduce the statistical fluctuations for the p _{ T } integrated quantities.
Concerning the extension of the kinematic coverage into the far backward direction for protons, x _{ F }<−0.8, see Sect. 7, additional integrated quantities are given in Table 10 for −2.0≤x _{ F }≤−0.9. Again, the data interpolation is used to obtain the numerical values.
In this region the estimation of the statistical uncertainties is nontrivial as the measured data have been transformed from the laboratory coordinates (p _{lab},Θ _{lab}) to the cms quantities (x _{ F },p _{ T }) using a twodimensional interpolation. The given errors have been obtained from the total number of measured protons at each lab angle [9] which varies from about 1100 to 3600. The values given in Table 10 are therefore to be regarded as upper limits.
The corresponding distributions for dn/dx _{ F }, F and dn/dy are shown in Fig. 52 for protons and in Fig. 53 for antiprotons.
The ratio of p _{ T } integrated \(\overline{\mathrm{p}}\) and p yields as a function of x _{ F } are shown in Fig. 54. The first and second moments 〈p _{ T }〉 and \(\langle p_{T}^{2} \rangle\) are presented as a function of x _{ F } in Fig. 55 for protons and in Fig. 56 for antiprotons.
Centrality dependence
The detection of “grey” protons in the centrality detector of NA49 [8] allows the study of particle densities as a function of the number n _{grey} of protons in the lab momentum range of approximately 0.15 to 1.2 GeV/c in the backward hemisphere. The number distribution dN/dn _{grey} has been shown in [4] to be a steep function of n _{grey} with only 20 % and 5 % of all events at n _{grey}=1 and 2, respectively. The determination of double differential cross sections is therefore not feasible in this experiment. As already shown in [4] for pions, the extraction of p _{ T } integrated yields as a function of x _{ F } by fitting the dE/dx distributions over the complete range of p _{ T } is however feasible in a limited range of x _{ F }. This range is determined by the variation of total momentum with p _{ T } and extends from x _{ F }=−0.2 to +0.65 for protons, the upper limit being imposed by the progressive loss of acceptance at low p _{ T }. Two samples with n _{grey}≥1 and n _{grey}≥2 have been selected. The resulting proton density distributions dn/dx _{ F } are given after correction in Table 11, with the additional use of the complete data sample (see also [4]) which allows for a precise control of eventual systematic effects. It should be realized that the measurement of “grey” protons is confined to the region x _{ F }<−0.2 [4] and does therefore not interfere with the results presented in Table 11.
As shown in Fig. 57, the results for the total data sample are compatible within errors with the integration of the data interpolation, Table 8 and Fig. 52.
As seen from Fig. 57, a systematic and smooth variation of the proton density distributions is evident when passing from p+p to minimum bias p+C and to centrality enhanced p+C interactions. A well defined crossover with equal number density is visible at x _{ F }=0.25–0.3. Above this value the densities decrease progressively with increasing number of projectile collisions by up to a factor of 0.5 at the experimentally accessible limit of x _{ F }=0.6. Below x _{ F }=0.3 this trend is inverted with a density increase of up to factors of 2.5 at negative x _{ F }.
A similar behaviour is also seen for antiprotons, although here only a reduced range in x _{ F } is accessible due to the limiting statistical uncertainties. This is shown in Fig. 58 where the relative difference in baryon density between the n _{grey} selected and minimum bias samples is given in % as a function of x _{ F } for protons (panel a) and antiprotons (panel b).
The interplay between baryon number transfer from the projectile hemisphere and pileup of baryons from the target fragmentation, including isospin effects, will be discussed in more detail in Sect. 12 of this paper.
Neutron data
The detection of forward neutrons in the Ring Calorimeter of NA49 [8] has been introduced and described in detail in [3]. The neutron analysis concerning the separation of electromagnetic and hadronic deposits, the veto against charged particles, the calorimeter calibration and the energy resolution unfolding may be directly applied to the p+C interactions. The x _{ F }/p _{ T } acceptance of the calorimeter is shown in Fig. 2. For the total neutron yields at x _{ F }≤0.3 an extrapolation beyond the available p _{ T } window has been performed using corresponding proton p _{ T } distributions, see also [3] for this procedure. This extrapolation concerns p _{ T } values in the ranges 0.8<p _{ T }<2 GeV/c at x _{ F }=0.1 up to 1.6<p _{ T }<2 GeV/c at x _{ F }=0.3. The corrections for feeddown from weak decays are shown in Fig. 23. The empty target, trigger bias and reinteraction corrections are equal to the ones for protons [3]. The contributions from \(K^{0}_{L}\) decay and antineutron production are obtained from the charged kaon data which are available from NA49 [19] and from the isospin argumentation using the antiproton data explained in [3].
The resulting neutron densities dn/dx _{ F } are listed in Table 12 together with their ratio to the results from p+p collisions [3].
The p _{ T } integrated neutron density distribution dn/dx _{ F } as a function of x _{ F } is presented in Fig. 59a together with a data interpolation (full line). Due to the absence of charge exchange processes in hadronic interactions at SPS energy [6] this interpolation is constrained to density zero at x _{ F }=1. Of particular interest in this context is the ratio between neutron densities in p+C and p+p interactions in comparison to the same ratio for protons as shown in Fig. 59b.
Evidently protons and neutrons show within errors the same behaviour when passing from p+p to p+C collisions. The density ratio is equal to 1 at x _{ F }=0.3, increasing to 1.3 at x _{ F }=0.1 and decreasing to 0.6 at x _{ F } towards +1. The latter value corresponds to the expected fraction of single projectile collisions in p+C interactions derived from the nuclear density distribution [5].
Comparison to other data
Two data sets are available for comparison with the NA49 integrated data in the SPS energy range. The first set from the ACCMOR collaboration [20] gives the density distribution dn/dx _{ F } of protons for p+A collisions from Be to U nuclei at 120 GeV/c beam momentum. A second, very recent publication from the MIPP collaboration [21] provides neutron densities dn/dx _{ F } for p+C interactions again at 120 GeV/c beam momentum at the FERMILAB Main Injector.
ACCMOR data [20]
The ACCMOR collaboration [20] measured proton densities dn/dx _{ F } with a proton beam at 120 GeV/c momentum at the CERN SPS for five different nuclei (Be, Cu, Ag, W, U) in the x _{ F } range from 0.07 to 0.6. These data may be interpolated from Be to C. This is demonstrated in Fig. 60 which gives the proton density as a function of mass number A for five x _{ F } values from 0.1 to 0.6.
The data interpolation of dn/dx _{ F } to p+C interactions is shown in Fig. 61 as a function of x _{ F } in comparison to the NA49 results, Table 8 and Fig. 52 above.
The ACCMOR data show an upward deviation which increases from about 0 at x _{ F }=0.6 to about 20 % at the lower data limit of x _{ F }=0.07. This deviation looks similar to the feeddown correction for protons from weak hyperon decays used for the NA49 data, Sect. 5.3, which reaches 15 % at small x _{ F } and decreases rapidly to 0 at x _{ F }∼0.7. As such a correction is not mentioned in [20] and as the geometrical layout of the experiment is similar to the one of NA49 as far as the position of the tracking elements is concerned (∼3 m distance between target and first tracking station) it has been tentatively assumed that the onvertex reconstruction efficiency of decay products might be similar in both experiments. Subtracting the feeddown correction from NA49 results in the broken line in Fig. 52. This line is about 8 % above the NA49 results for x _{ F }<0.4. At this point a look at the total inelastic cross sections as a function of A from different references [20, 22], Fig. 62, shows that the cross section for p+Be given in [20] falls low by about 6 % compared to the interpolation of other available data [22]. A corresponding correction of the cross section is shown as dotted line in Fig. 61
In conclusion it may be stated that the ACCMOR results are compatible with the NA49 results within the quoted systematic uncertainties.
MIPP data [21]
Very recently new data on neutron densities dn/dx _{ F } have become available from the MIPP collaboration at the FERMILAB Main Injector for p+p and p+A interactions [21]. The MIPP neutron densities dn/dx _{ F } for p+C interactions at 120 GeV/c beam momentum are compared to the NA49 results in Fig. 63a, the densities for p+p collisions at 84 GeV/c beam momentum in Fig. 63b.
Important deviations are visible between the two experiments both for p+C and p+p collisions. This is quantified in Fig. 64 where the ratio
between the two respective interpolations is shown as a function of x _{ F }.
The density ratios show a remarkable similarity between p+C and p+p interactions, varying systematically from 1.4–1.6 at the lower x _{ F } limit to a maximum of 1.9–2.0 at x _{ F }∼0.4 and decreasing to 0.5–1.0 at the upper kinematic limit. The total neutron yields in the forward hemisphere obtained by an extrapolation of the measured densities towards x _{ F }=0 as shown in Fig. 63 deviate by about 60 % for both reactions, with the integrated MIPP neutron yield resulting in 1 neutron per event for p+p collisions at 84 GeV/c beam momentum.
These large deviations pose a problem for baryon number conservation which may be verified for p+p interactions using published total yields for protons, neutrons, hyperons, pair produced protons and pair produced hyperons. The available data are plotted in Fig. 65 as a function of \(\sqrt{s}\) from [23, 24] at 12 and 24 GeV/c beam momentum, [25, 26] at 32 GeV/c beam momentum, [27–29] at 69 GeV/c beam momentum and from NA49.
The large neutron yields published by MIPP are clearly out of proportion with respect to the available data and are incompatible with baryon number conservation.
A phenomenological study of baryon and antibaryon production in p+C interactions over the complete phase space
In the following sections a detailed phenomenological analysis of the experimental results presented above will be carried out. In this context it may be useful to recall some basic ingredients of p+A interactions and their relation to the elementary nucleon–nucleon collisions. The following short subsections should be regarded as a recollection of known facts as well as an introduction to the more detailed and quantitative studies described in the subsequent sections.
The three components contributing to p+A collisions
There is today no doubt that the final state of p+A collisions is built up from three basic components:

The fragmentation of the projectile particle.

The fragmentation of those target nucleons which are hit by the projectile.

The nuclear component which is created by the momentum transfer from the projectile via the hit target nucleons into the nucleus.
It is important to realize that different time scales are acting in the hadronization of the mentioned components: the fragmentation time scales are short with respect to the nuclear cascading processes. In consequence, as will be shown in detail below, only those secondaries from the target fragmentation which have small momenta in the target rest frame are involved in the cascading process.
A schematic view of this situation is shown in Fig. 66 for final state protons which gives, in addition to the total measured proton yield (full line), its separation into the three basic components of p+A interactions: the projectile fragmentation (broken line), target fragmentation (dotted line), and nuclear component (dashdotted line).
The separation and extraction of the three components will be described below in a largely modelindependent way that essentially only relies on experimental input. The term “modelindependent” will be explained and become clear in the course of the following argumentation. The asymmetric character of the p+A interactions is in this context to be seen as an asset and not as a complication, as it permits—in contrast to the symmetric A+A collisions—a straightforward, parameterfree experimental separation of the components with only one single assumption concerning the target contribution.
Intranuclear collisions
The projectile undergoes subsequent collisions on its way through the target nucleus. The number of these collisions is given by the variable ν with mean value 〈ν〉. In the past, quite a number of assumptions have been made about this multiple collision process, ranging from the splittingup of the projectile into quarks upon the first collision to the constancy of the total interaction cross section through the subsequent collisions. In the latter hypothesis, the variable ν is calculable on an eventbyevent basis using the measured density distribution of nucleons inside the nucleus [5]. Its mean value is then also accessible from the total inelastic p+A interaction cross section in its relation to the p+p cross section [5],
In this case, it stands to reason to assume the hadronization of the hit target nucleons to be equivalent to the hadronization of the elementary nucleon–nucleon interaction, of course up to intranuclear cascading of the low momentum secondaries evoked above, and taking full account of isospin symmetry. This hypothesis allows the straightforward prediction of particle densities in the target fragmentation region (Fig. 66) which is directly amenable to experimental verification. It is the only assumption made in the following analysis and it will be tested quantitatively using the available experimental results both from p+p [3] and p+C interactions.
Net baryons and baryon/antibaryon pairs
Final state baryon production appears in two categories: “net” baryons which are linked to the presence of a projectile baryon and have to obey baryon number conservation, and baryon/antibaryon pairs. Experimentally the “net” baryon yield may be defined by the difference between the total yield of a baryon species and the corresponding yield of pairproduced baryons of the same species. Whereas the sum of all net baryon yields is constrained by baryon number conservation, there is no limit to the production of baryon/antibaryon pairs which rises sharply from the threshold at about \(\sqrt{s}=6~\mbox{GeV}\) through the SPS energy range and flattens towards collider energies in a way characteristic of the production of heavy hadronic systems.
In the case of protons, it has to be realized that the baryon/antibaryon yield is not only given by proton/antiproton pair production, but has also additional components containing neutrons and antineutrons. In the following, protons and neutrons which are produced as baryon/antibaryon pairs are therefore denoted by:
In general these pairs form isospin triplets with the isospin3 components shown in Table 13.
This phenomenology has been studied by NA49 using the comparison of p+p and n+p interactions [12]. Here it has been shown that the antiproton yield increases by about a factor of 1.6 when exchanging the I _{3}=+1/2 against an I _{3}=−1/2 projectile, thereby enhancing the I _{3}=−1 against the I _{3}=+1 combination in Table 13.
As the central \(\overline{\mathrm{p}}\)/p ratio reaches about 23 % for minimum bias p+C interactions, the definition of net protons needs a careful analysis of the corresponding isospin factors, as shown below.
Overlap between the components of fragmentation
In the separation of the different components of final state hadronization characterized for example by the target and the projectile hemispheres, the eventual overlap between these hemispheres, Fig. 66, plays an important role. For any quantitative work the exact extent and shape of the respective overlap functions has to be known and it will be shown below that this is indeed possible in a completely modelindependent way, using basic conservation rules. In the case of final state pions this has been achieved in Ref. [5] using charge conservation and isospin symmetry, using also π+p interactions. For net protons, baryon number conservation may be invoked, and for antiprotons the internal isospin structure of the fragmentation process has been used. In both cases this is discussed in detail below.
Several wellknown experimental findings present sharp constraints to the phenomenon of component overlap, in particular at SPS energy:

The absence, at SPS energy, of charge and flavour exchange.

The absence of longrange correlations between the target and projectile hemispheres, for x _{ F }>0.2.

The independence of the target fragmentation on the nature of the projectile particle and vice versa (hadronic factorization).

The presence of shortrange forward–backward multiplicity correlations at x _{ F }<0.2
Within the experimental uncertainties, a common overlap function which is limited to 0.2 units of x _{ F } has been measured for net protons and antiprotons.
Extraction of the projectile and nuclear components
Given the hypothesis for the target fragmentation described above, and given the fact that this hypothesis may be tested against the experimental results, the projectile and nuclear components follow, without additional assumptions, from the subtraction of the target fragmentation from the measured total proton or antiproton yields. For the protons it is useful to extract the net proton projectile component as in this case a direct crosscheck of baryon number conservation becomes possible. The extraction will be performed both for the p _{ T } integrated and for the doubledifferential yields. With respect to the interplay of the target fragmentation and nuclear components in the far backward direction, the modification and extent in x _{ F } of the diffractive target component will be determined.
Error estimation
The present analysis makes use of experimental results both from p+p and from p+C interactions. In both cases the results from the twodimensional data interpolation and of its integration over transverse momentum are exploited. With mean statistical errors of 8 % (12 %) in p+C and 5 % (11 %) in p+p for protons and antiprotons, respectively, the local fluctuations of the data interpolation are about a factor of 3 lower. For the p _{ T } integration, the statistical errors have an upper limit of order 1 %.The systematic uncertainties are estimated to 3.7 % (4.5 %) in p+C and 2.5 % (3.3 %) in p+p, where a part of these quantities is of common origin. In the data comparison between the two reactions, a systematic error of about 5 % is therefore estimated.
Two component mechanism of baryon and baryon pair production
In preparation of the separation of the different components contributing to the overall baryon and antibaryon yields in p+C interactions, a modelindependent study of the target and projectile components in p+p collisions will be performed in this section. This study allows the extraction of the baryonic overlap functions introduced in Sect. 11.4 above. The section will also contain a detailed comparison to the results from a microscopic simulation code.
A large sample of 4.8 million inelastic events is available from NA49 [1–3] with both proton/antiproton and neutron identification in the final state. This allows for the selection of subsamples of events with defined net baryon number either in the projectile or in the target hemisphere by tagging baryons at sufficiently large x _{ F }. Sufficiently large means in this context x _{ F } values where the yield of pair produced baryons is low enough to ensure negligible background. For protons this condition is fulfilled for x _{ F }>0.35 where the \(\overline{\mathrm{p}}\)/p ratio is less than 0.5 % [3]. The following ranges of x _{ F } have been used for net proton and neutron selection:
These ranges are given by the constraints of acceptance and proton identification via dE/dx, see Sect. 4, and by the limited energy resolution of the hadron calorimetry for neutrons. In the following the measured baryonic double and single differential densities obtained with net baryon constraint,
will be described by their ratio to the corresponding inclusive yields,
by
The ratio \(R^{c}_{\mathrm{int}}(x_{F})\) is obtained by direct yield extraction over the complete p _{ T } range from 0 to 1.9 GeV/c, while R ^{c}(x _{ F },p _{ T }) extracts the ratios in distinct x _{ F }/p _{ T } bins. This allows for the study of eventual p _{ T } dependences. The double differential cross sections are obtained, due to limited statistics, in the range 0.1<p _{ T }<0.7 GeV/c, and the resulting ratios are averaged over this p _{ T } range resulting in the ratios:
In a first subsection the production of antiprotons in these samples will be studied, as the determination of the net proton yields has to rely on the estimation of the cross sections of pairproduced protons.
Antiprotons with finalstate net baryon constraint
The ratios \(R^{c}_{\mathrm{av}}(x_{F})\) and \(R^{c}_{\mathrm{int}}(x_{F})\) for antiprotons are presented in Fig. 67 for forward (14) and backward (16) proton selection.
For both net proton selections, a distinct correlation between the antiproton yields and the presence of a tagged proton in the respective hemisphere is evident. The yield ratios reach values of 1.6 in the far backward and forward directions, respectively. The excess over 1 is halved at x _{ F }=0 and the ratio goes to 1 in the respective opposite x _{ F } regions. It has been verified that this correlation is not induced by asymmetries in the azimuthal acceptance of the detector. It is therefore due to an isospin effect as expected from the isotriplet nature of baryon pair production, Table 13. Indeed the presence of a net proton will unbalance the isospin structure present in the inclusive event sample towards the I _{3}=−1 component of the corresponding heavy mesonic state and thereby enhance the \(\overline{\mathrm{p}}\,\widetilde{\mathrm{n}}\) yield in the selected hemisphere. From this argument follows a strict prediction for the tagging with net neutrons: in this case the I _{3}=+1 component, hence the \(\overline{\mathrm{n}}\,\widetilde{\mathrm{p}}\) combination, should be favoured, and the antiproton yield should be reduced accordingly with respect to the inclusive sample. This is indeed the case as shown in Fig. 68 for forward neutron tagging, see (15).
This finding has two interesting consequences: it allows for the first time the establishment of the range and shape of the antiproton overlap function in a completely modelindependent way. Secondly it has direct consequences for the possible production mechanism of baryon pairs in hadronic interactions.
The hand interpolated lines given in Figs. 67 and 68 may be redefined as the antiproton overlap function \(F^{o}_{\overline{\mathrm{p}}}\) which is normalized in the ordinate to the range 0 \(\leq F^{o}_{\overline{\mathrm{p}}} \leq1\), as shown in Fig. 69 and tabulated in Table 14. This function is strongly constrained by the forward–backward symmetry in p+p interactions. It has to pass through 0.5 at x _{ F }=0 and it should reach the values of 0 or 1 at x _{ F }∼0.2 as imposed by the absence of long range hadronic correlations beyond this limit [5]. In addition, the constraint \(F^{o}_{\overline{\mathrm{p}}}(+x_{F}) = 1  F^{o}_{\overline{\mathrm{p}}}(x_{F})\) has to be fulfilled. This leaves, regarding the experimental error bars, in particular those for the net proton yields (Fig. 72) resulting in the same x _{ F } dependence, an error margin of about 5 % for the intermediate x _{ F } values.
A remark concerning the choice of the longitudinal variable might be in place here. Throughout this paper the Feynman x _{ F } variable has been chosen to describe the longitudinal momentum dependences. This choice has several reasons:

x _{ F } describes, at least to first order, the observed scaling of the hadronic cross section with cms energy.

It is orthogonal with respect to the transverse momentum.

The range of the forward–backward correlations, as for example the forward–backward multiplicity correlations [5] has been shown to be sindependent in the x _{ F } variable.

If changing from x _{ F } to the rapidity variable y, the energy scaling of the results as well as the orthogonality to p _{ T } is lost. As shown in detail in Ref. [5] different rapidity limits for each interaction energy have to be introduced to describe the multiplicity correlations. In addition and of course, seeing rapidity as basically an angular variable, strong correlations with p _{ T } of all physics phenomena depending on longitudinal momentum are introduced.
Concerning the production mechanism of baryon pairs, the strong isospin correlation both with the final state net baryons and with the hadronic projectile in the initial state speaks against the central production from the quarkgluon sea, as for instance gluon fusion. Concerning current hadronization models using string fragmentation, the adhoc introduction of diquark systems in the colliding baryons is necessary in order to describe the net baryon production. In addition quark/antiquark and diquark/antidiquark pickup processes have to be introduced for baryon pair production, in close resemblance to the description of hadronization in e^{+}+e^{−} annihilation, with a multitude of adjustable parameters and doubtful predictive power, see Sect. 12.5.
On the other hand the presence of heavy, high spin mesonic states in the early stage of hadronization of the highly excited baryonic systems in the p+p interaction presents a natural explanation for the observed correlations. In fact most observed heavy meson resonances have a \(\overline{\mathrm{p}}\,\widetilde{\mathrm{p}}\) decay branching fraction, or have been discovered in the inverse \(\overline{\mathrm{p}}+\mathrm{p}\) annihilation process. It is interesting to note that baryon pair production, via the high effective mass involved, probes a rather primordial phase of hadronization as compared to the lighter final state hadrons. This again favours the observed strong isospin correlations. In this context it should be recalled that a high mass mesonic origin of baryon pairs was indeed proposed as early as 35 years ago by Bourquin and Gaillard [30] in order to describe the observed inclusive yields.
Pairproduced protons
Following the isospin structure of baryon pair production, see Table 13, antiprotons (\(\overline{\mathrm{p}}\)) and pair produced protons (\(\widetilde{\mathrm{p}}\)) are coupled in their yields by isospin symmetry with the I _{3} component of either the projectile or the trigger net baryon in the respective hemisphere. This is shown schematically in Fig. 70 where the \(\overline{\mathrm{p}}\) and \(\widetilde{\mathrm{p}}\) yields are presented with respect to the inclusive antiproton level in p+p interactions.
Evidently the definition of “net” protons, which needs the knowledge of pairproduced proton yields, is linked to the measured \(\overline{\mathrm{p}}\) yields in a nontrivial fashion. As far as the overlap function between the forward and backward hemispheres is concerned, it is of course the same for \(\overline{\mathrm{p}}\) and \(\widetilde{\mathrm{p}}\) and has to be referred to the yield levels indicated in Fig. 70.
Net proton feedover
With the above clarification of the yields of pair produced baryons, the inclusive net proton yield may now be defined as:
As \(\rho^{\mathrm{incl}}_{\widetilde{\mathrm{p}}}\) is 1.6 times higher than \(\rho^{\mathrm{incl}}_{\overline{\mathrm{p}}}\), Fig. 70, this means a substantial decrease of the central net proton density with respect to the simple subtraction of the \(\overline{\mathrm{p}}\) yield. The consequence of this for the evolution of \(\rho^{\mathrm{net}}_{\mathrm{p}}\) with \(\sqrt{s}\) has been demonstrated in [12] where it has been shown that the central net invariant proton cross section approaches zero in the ISR energy range.
The net proton feedover and the corresponding overlap function may be determined, as for the antiproton case Sect. 12.1 above, by fixing a net proton in the projectile or target hemisphere following the selection criteria, (14) and (16) above, respectively. This ensures the absence of net protons in the corresponding hemisphere and results in the constrained net proton density:
These density distributions may be normalized by dividing by the inclusive yield, (21), resulting in the ratio
In a first instance, it can be shown that \(R^{c,\mathrm{net}}_{\mathrm{p}}(x_{F},p_{T})\) is independent on p _{ T } in the range 0.1<p _{ T }<0.7 GeV/c, see Fig. 71.
The x _{ F } dependence for the p _{ T } integrated ratio \(R^{c,\mathrm{net}}_{\mathrm{p}}(x_{F})\) and the p _{ T } averaged ratio \(\langle R^{c,\mathrm{net}}_{\mathrm{p}}(x_{F},p_{T}) \rangle\) are shown in Fig. 72. The full lines in this Figure represent the same overlap function as extracted for antiprotons, Fig. 69. In addition and due to the higher statistics available for protons, the independence of the overlap function on transverse momentum has been demonstrated, Fig. 71. This gives an interesting connection to the origin of proton yields from the decay of heavy resonances, which predicts p _{ T } independence in contrast to pions as decay products of the same resonances, see Ref. [5].
A remark concerning resonance decay
The modelindependent extraction of the baryonic feedover and the experimental determination of the corresponding overlap functions, as described in the preceding sections, may be extended to resonance decay. As in fact most if not all final state baryons stem from resonance decay it is of interest to investigate the consequences of the hadronic twocomponent mechanism observed for the final state baryons also for the parent generation of resonances. This will be demonstrated below using as examples the well measured Δ^{++} resonance for the proton and a mesonic resonance approximated by measured tensor meson characteristics for the antiproton feedover.
Protons from Δ^{++} decay
The p _{ T } integrated density distribution dn/dx _{ F }(x _{ F }) of the Δ^{++}(1232) resonance has been rather precisely measured by a number of experiments in the SPS and ISR energy ranges as shown by two examples [31, 32] in Fig. 73a. In both cases the full p _{ T } range from 0 to 2 GeV/c was available. The integration of the interpolated full line yields a total inclusive cross section of 7 mb. The corresponding decay proton distribution from Δ^{++}→p+π ^{+} (100 % branching fraction) is presented in Fig. 73b together with the measured total inclusive proton yield as measured by NA49 [3], multiplied by the factor 0.27.
This plot demonstrates several important features:

The shape of the decay proton distribution from Δ^{++} follows, for x _{ F }<0.6, very closely (to within about 5 %) the total inclusive proton distribution renormalized by a factor 0.27. This means that 27 % of all protons in this x _{ F } range stem from Δ^{++} decay alone.

The difference between the decay and inclusive distributions at x _{ F }>0 is well described by a \(1/M_{x}^{2}\) form typical of single diffraction with \(M_{x}^{2} \sim s(1x_{F})\), dashdotted line in panel (b).

Taking account of the other Δ states Δ^{+}(1232) and Δ^{0}(1232) with branching fractions of 66 % and 33 % into protons, respectively, this means that more than 40 % of all nondiffractive protons cascade down from Δ resonances.

The shape difference between the dn/dx _{ F } distributions of the mother resonance and the daughter protons exemplifies the very effective baryon number transfer towards the central x _{ F } region in resonance decay even for lowQ resonances like the Δ.
A number of further comments are due in this context. The absence of charge and flavour exchange in inelastic p+p interactions at SPS energy implies that the observed Δ resonances are not directly produced at least in the primordial phase of target and projectile excitation. They rather turn up as decay products of N^{∗} resonances. This fact has been experimentally proven in a number of high precision studies of single and double diffraction into pπ ^{+} π ^{−} states from PS to ISR energies [33–36]. In these final states which cover an x _{ F } range from 1 to about 0.6 [36], the initial I, I _{3} state is 1/2, +1/2. Although the subchannels pπ ^{+} and pπ ^{−} show clear Δ(1232) signals, those are completely contained in the decay mass spectra of a series of N^{∗} resonances (N^{∗}(1440), N^{∗}(1520), N^{∗}(1680)). In the more central area of hadronization, this clear isospin signature will become diluted and contain 1/2, −1/2 states, see also the isospin correlations discussed above. Nevertheless the production and decay of N^{∗} resonances without intermediate Δ states will provide another important source of final state nucleons.
The twocomponent mechanism of hadronization should therefore also be considered for baryon resonances with the constraint to reproduce the measured overlap function for final state protons. This is fulfilled for Δ^{++} by the separation of the production cross section into a target and a projectile component as indicated in Fig. 74a. The corresponding x _{ F } distributions for the decay protons are given in Fig. 74b.
This choice results in the ratios R=(dn/dx _{ F })_{proj}/(dn/dx _{ F })^{incl} between projectile component and inclusive distribution shown in Fig. 75.
Evidently the measured proton feedover is precisely reproduced, Fig. 75b, if the overlap function of the mother resonance is chosen slightly wider in x _{ F }, Fig. 75a, indicating a certain mass dependence in the x _{ F } scale. In this context the dependence on decay particle mass exhibited by the much reduced feedover for the decay pions from Δ^{++}, as elaborated in [5], should be recalled here.
Antiprotons from heavy meson decay
A complementary approach may be used for the production of antiprotons from heavy mesonic states [30]. In fact a sizeable number of states above the p\(\overline{\mathrm{p}}\) mass threshold at 1.88 GeV/c^{2} have been observed [37] both in hadronic interactions and in the inverse p\(\overline{\mathrm{p}}\) annihilation into final state hadrons. While due to the large width and density of these states their direct experimental detection in mass spectra is difficult, the application of Partial Wave Analysis permits their localization and determination of quantum numbers. In the following a hypothetical state at 2.5 GeV mass with a Breit–Wigner width of 0.25 GeV and a twobody decay into p\(\overline{\mathrm{p}}\) is used in order to study the corresponding daughter x _{ F } distributions and overlap functions. An invariant x _{ F } distribution consistent with the one for vector and tensor mesons published by Suzuki et al. [38] yields the inclusive density distribution dn/dx _{ F } for the decay antiprotons shown in Fig. 76.
Evidently this choice reproduces perfectly the measured inclusive antiproton yields measured by NA49 [3]. Imposing the targetprojectile decomposition for the yield distribution of the heavy meson as shown in Fig. 77a, the overlap function for the decay baryons reproduces closely the measured feedover for antiprotons, Fig. 77b.
As far as the normalization of the resulting inclusive yields is concerned, it may be stated that—compared to the \(\overline{\mathrm{p}}\) cross section of 1.2 mb [3]—the measurement of [38] indicates 1.6 mb for the f_{4}(2050) state alone, and the mass dependence of the tensor meson production given in [39] an f_{4}(2050) cross section in excess of 5 mb at ISR energy. There are, however, almost no measurements of the branching fraction into baryon pairs, and if so, they vary by large factors, for the f_{4}(2050) for instance from 50 % [40] to 0.2 % [41]. The amount to which antiprotons cascade from heavy meson decay has therefore to stay an open question.
Comparison to a microscopic simulation code
In the preceding NA49 publications concerning p+p and p+C interactions [1–5] a strictly modelindependent approach to the interpretation of these extensive and precise data sets has been followed. Comparison to the multitude of existing microscopic simulation codes has therefore been avoided in clear appreciation of the fact that the actual understanding (or, better, lack of understanding) of the theoretical foundations of the soft sector of QCD calls for improved experimental information rather than ad hoc parametrizations. Given the detailed data concerning baryons both on the inclusive level and on the level of baryonic correlations contained in [3] and in the above discussion, it might however be useful to confront the obtained results with one specific microscopic simulation in order to obtain some idea of the precision and predictive power reached in such approaches.
The relatively recent code named JAM [42] has been chosen for this comparison. This code is supposed to describe hadronization in elementary and nuclear interactions over the complete cms energy range from 1 GeV up to collider energies. It uses, in the SPS energy range, soft string excitation following the HIJING [43] approach which in turn relies on the string fragmentation mechanism developed in the PYTHIA/LUND [44] environment.
Inclusive baryon and antibaryon density distributions dn/dx _{ F }
The measured proton and neutron density distributions dn/dx _{ F } in p+p interactions are confronted in Fig. 78 with the predictions from JAM.
Large systematic deviations between prediction and data are visible at low x _{ F } (−40 %), at medium x _{ F }∼0.25 (+50 %) and at high x _{ F } (−30 %) for the protons. Systematic deviations of similar or bigger size are also seen for the HSD and UrQMD codes [45].
The neutron yields are evidently obtained from the proton densities by a constant multiplicative factor of 0.69 with the exception of the large x _{ F } region where a diffractive component with a \(1/M_{x}^{2}\) behaviour, see Sect. 12.4.1, is added to the protons. The deviations are +60 % at medium x _{ F } and more than −100 % at large x _{ F } for the neutrons. A look at the density distributions for n+p interactions, Fig. 79, shows only approximate isospin symmetry which would impose that neutrons from proton fragmentation should be equal to protons from neutrons in the x _{ F } regions beyond the targetprojectile overlap. The same should of course be true for neutrons from neutron beam and protons from proton beam.
The antibaryon densities shown in Fig. 80 show an interesting pattern, the antiproton and antineutron yields being identical for both projectiletarget combinations.
This means that only the I _{3}=0 combinations p\(\overline{\mathrm{p}}\) and n\(\overline{\mathrm{n}}\) are allowed which are produced with equal yields. The comparison with the measured antiproton density in p+p collisions shows a sizeable underestimation of the yield by 35 % at x _{ F }=0 and an equally large overestimation at x _{ F }∼0.3. Invoking the isospin effect measured in n+p interactions [12] this difference will increase to 50 % in this reaction.
Baryonic correlations
While it might be a straightforward possibility to remedy the observed discrepancies between the prediction and the inclusive data by modifying some of the many parameters involved in the simulation codes, the correlation data will probe the “physics” input on a deeper level. This applies especially to the measured isospin effects.
A first comparison concerns the net proton density correlated with a trigger baryon in the projectile hemisphere resulting in the overlap function \(R^{c,\mathrm{net}}_{\mathrm{p}}\), (23), as shown in Fig. 81 for the two trigger x _{ F } bins defined in Sect. 12, Eqs. (14) and (15).
The microscopic simulation results in a feedover behaviour which only reaches to about ±0.06 in x _{ F }. This is considerably sharper than the measured behaviour (full lines in Fig. 81) and corresponds to the pionic feedover extracted in [5]. In addition there is an asymmetric long range tail that extends up to and beyond x _{ F }∼0.3 and is different both for proton and neutron trigger and for the two trigger x _{ F } bins in contrast to the data.
The antiproton feedover behaviour characterized by the ratio \(R^{c}_{\overline{\mathrm{p}}}(x_{F})\) of correlated to inclusive densities, Eq. (19), is presented in Fig. 82 again for the two available trigger x _{ F } bins and for proton and neutron trigger.
A rather complicated pattern concerning the simulation emerges. Evidently the symmetric isospin effect observed experimentally between proton and neutron triggers is not reproduced although there is a general reduction of the density ratio in the trigger hemisphere with neutron triggers. As only isospin singlet baryon pairs are generated, see Sect. 12.5.1, any isospin effect is not really expected. The strong suppression of the density ratio in the highx _{ F } trigger bin already starting at x _{ F }∼0.2 indicates an effect of energymomentum conservation in the baryon pair simulation which is probably the result of the details of string fragmentation.
In conclusion the microscopic simulation results in major deviations from the data both on the level of the inclusive and of the correlated yields. The absence of a proper treatment of isospin effects both concerning the I _{3} component of the projectile and of the final state baryons is flagrant. This puts into doubt the application of this approach to p+A and especially A+A interactions where the neutron component is preponderant.
Proton and antiproton feedover in p+C interactions
The study presented above for p+p collisions may be repeated for p+C interactions, albeit with reduced statistical significance due to the smaller available data sample. The density ratio for antiprotons, \(R^{c}_{\overline{\mathrm{p}}}(x_{F})\) with forward proton tagging is presented in Fig. 83 where the full line represents the feedover function measured in p+p interactions, see Fig. 67.
Evidently the measurement reproduces the shape and extent of the \(\overline{\mathrm{p}}\) overlap in p+p collisions.
Net proton tagging in the backward hemisphere is not possible for p+A interactions as protons from intranuclear cascading (“grey” protons) which prevail in this area dilute the correlation.
For the net proton density \(\rho^{c,\mathrm{net}}_{\mathrm{p}}(x_{F})\) with tagging in the projectile hemisphere, a result which might look surprising at first view is found as shown in Fig. 84.
Indeed the constrained net proton density reproduces the one found in p+p interactions down to x _{ F }=−0.2. This reveals an additional internal correlation effect generally present in minimum bias p+A interactions. By selecting a rather forward proton, see (14), single collisions corresponding to peripheral interactions are enhanced. In fact 60 % of the minimum bias p+C events correspond to single interactions of the projectile proton with nuclear participants [5]. The situation is clarified by Fig. 85 which presents the inclusive proton yield dn/dx _{ F }(x _{ F }) in p+C collisions (full line), 0.6×dn/dx _{ F }(x _{ F }) from p+p (broken line), and their difference (dotted line). It is evident that the bulk of protons in the tagging region (hatched area) comes from single collisions, with the fraction of multiple collisions in addition biased against very inelastic interactions which would favour lowx _{ F } protons by enhanced baryon number transfer. It may however be stated that also for p+C interactions with forward proton tagging the constrained net proton density dies out at x _{ F }>0.2.
Hadronization in p+C collisions: antiprotons
The twocomponent hadronization mechanism studied experimentally in the preceding section allows, in conjunction with the precision data on antiproton production in p+p interactions published by NA49 [3], the confrontation of the measured \(\overline{\mathrm{p}}\) yields in p+C collisions with a straightforward prediction based on elementary reactions. This is simplified in the case of antiprotons by the fact that there is, in contrast to proton and pion production, no contribution from nuclear cascading (see Sect. 9 above). In consequence the superposition of target and projectile fragmentation should suffice to completely describe the observed cross sections. In a first step it may be assumed that the projectile contribution corresponds exactly to the one in p+p interactions. For the target contribution the same basic assumption may be made with two important additional constraints taking account, firstly, of the multiple intranuclear collisions of the projectile, and secondly, of the isospin factor involved in the fragmentation of the neutrons contained in the nucleus.
The mean number of projectile collisions 〈ν〉 in minimum bias p+C collisions has been investigated in [5] using three different methods:

A Monte Carlo simulation using the measured nuclear density profile as input with the result 〈ν〉=1.6

The measured p+C inelastic cross section which gives, via the relation
$$ \langle\nu\rangle = \frac{A\cdot\sigma(pp)}{\sigma(pA)} $$(24)an estimation of 〈ν〉 under the assumption that the intranuclear inelastic interaction cross section stays constant for all subsequent projectile collisions, resulting in 〈ν〉=1.68

The measured increase of pion yields in the backward hemisphere using the fact that the contribution from intranuclear cascading as well as the one from projectile fragmentation die out at x _{ F }∼−0.1, yielding 〈ν〉=1.6.
The isospin factor for \(\overline{\mathrm{p}}\) production from the isoscalar C nucleus may be calculated, using the measured increase of \(\overline{\mathrm{p}}\) yields in n+p collisions \(g^{n}_{\overline{\mathrm{p}}}\) [12] as
with \(g^{n}_{\overline{\mathrm{p}}}=1.6\). The combined overall factor to be applied to the target component is 1.6×1.3=2.08.
p _{ T } integrated density dn/dx _{ F }(x _{ F })
The evolution of the p _{ T } integrated antiproton density dn/dx _{ F }(x _{ F }) from the elementary p+p to the p+C interactions using the superposition of target and projectile components discussed above is presented in Fig. 86. The p _{ T } integration was performed both for the p+p and p+C data in the range 0<p _{ T }<1.7 GeV/c.
This most straightforward superposition picture evidently reproduces the measured \(\overline{\mathrm{p}}\) densities quite closely, overestimating them by about 10 % in the target area and underestimating them by the same amount in the projectile region. This can be remedied by decreasing the target multiplication factor by 12 % from 2.08 to 1.84 and by increasing the projectile contribution by 10 % resulting in a reasonable fit of the experimental data compatible with their statistical errors as shown in Fig. 87.
The increase of the \(\overline{\mathrm{p}}\) yield by 10 % in the projectile hemisphere with respect to the direct estimation from p+p collisions is a first interesting consequence of this study. It is equal to the increase of the pion yields deduced in [5].
The reduction of the target contribution by about 12 % with respect to the simple superposition of elementary hadronization processes as characterized by the mean number of collisions 〈ν〉 and isospin symmetry, is a second important result. The magnitude of this reduction being relatively small it is nevertheless on the limit allowed by the experimental determination both of 〈ν〉 [5] and of the isospin effect on antiproton production from neutrons [12].
Regarding the excitation mechanism of colliding hadrons by the exchange of gluons or gluonic (charge and flavourless) objects, the observed effects are however to be expected. The projectile interacts in its multiple collisions subsequently with “fresh” nucleons which did not undergo previous exchanges. Hence its effective excitation level will increase with 〈ν〉. The projectile on the other hand suffers in each collision a loss of its gluonic component such that less excitation energy with the target nucleons can be exchanged in subsequent interactions. In this sense the nucleus may be regarded as a gluon filter, the description of this phenomenology by the term of “energy loss” giving only a very general and somewhat misleading impression.
The antiproton yields regarded here are especially sensitive to this notion as at SPS energy the sdependence of the production cross section is still rather steep with about 10 % per GeV in \(\sqrt{s}\) [30]. This is in contrast to the production of mesons, with 5 % per GeV for mean kaons [2] and only 3 % per GeV for mean pions [46]. In this sense the study of pion yields in the target hemisphere approaches a precise measure of 〈ν〉 [5] whereas the observed antiproton cross section indicates an effective loss in \(\sqrt{s}\) of about 1 GeV in target fragmentation for p+C collisions. Evidently the extension of this study to heavier nuclei is of considerable interest in this respect. The data on p+Pb collisions with controlled centrality available from NA49 will illuminate this point, as is already visible in the preliminary results shown in [47].
Double differential invariant densities f(x _{ F },p _{ T })/σ _{inel}
Further details of the twocomponent hadronization mechanism detailed above become visible if comparing the double differential invariant densities to the optimized prediction from target and projectile fragmentation obtained from the p _{ T } integrated yields, see Fig. 87. This is shown in Fig. 88 where the invariant cross sections f(x _{ F },p _{ T }) per inelastic event (open circles) are presented together with the predicted densities (full line).
Three main features may be extracted from these plots:

The target component reproduces, within the experimental errors, the densities predicted from elementary interactions for p _{ T }<1 GeV/c.

The projectile component reveals a definite p _{ T } dependence. The measurements fall below the prediction for p _{ T }≲0.5 GeV/c and increase smoothly above the prediction above this value.

In the range of p _{ T }>1 GeV/c the excess of the projectile component starts to extend well into the target hemisphere down to x _{ F }∼−0.2.
This behaviour is detailed in Fig. 89 which presents the ratio R between measurement and prediction for the p _{ T } values shown in Fig. 88.
The same ratio is plotted against p _{ T } for different values of x _{ F } in Fig. 90.
It should be stressed here that these experimental results are in strong support of the independent targetprojectile fragmentation in p+C interactions. The modification of the p _{ T } distribution of the projectile component which superimposes itself to the 10 % increase in total yield, indicates that the Cronin effect, whose onset is visible here, is limited to the projectile hadronization. The increase of yields at higher p _{ T } which extends well into the target hemisphere might be due to an extension of the feedover range with p _{ T } (see also [5] for pions), although the limited statistics does not allow for quantitative statements. The increase of R in the projectile hemisphere may be parametrized as
Its modification in the transition to the target hemisphere is then predicted by the projectile overlap function \(F^{o}_{\overline{\mathrm{p}}}\) (Fig. 69) resulting in the full lines indicated in Figs. 89 and 90.
Further information is contained in the detailed comparison of the average p _{ T } values to p+p interactions given in Fig. 91.
The convergence of the difference in 〈p _{ T }〉 towards zero in the backward hemisphere, Fig. 91b, and its description by the overlap function \(F^{o}_{\overline{\mathrm{p}}}\), Fig. 69, is to be regarded as yet another manifestation of the twocomponent mechanism of hadronization as discussed in Sect. 12.
Proton production in p+C collisions: p _{ T } integrated yields
As in the preceding section on antiprotons, proton production will be first discussed using the p _{ T } integrated yields dn/dx _{ F } in order to clearly visualize and separate the three basic contributions to the overall proton cross section. After establishing the net proton density by subtracting the yield of pair produced protons, the fragmentation of the hit target nucleons, the projectile fragmentation and the contribution from intranuclear cascading will be treated in turn. The p _{ T } integrations used in this section were performed both for the p+p and p+C data in the range 0<p _{ T }<1.7 GeV/c.
Pair produced protons and net proton density
It has been shown above that the isotriplet nature of baryon pair production imposes a detailed followup of isospin effects all through the hadronization process. This means of course that the yield of antiprotons is in general not identical to the yield of pairproduced protons. It is therefore not sufficient to subtract the antiproton density as established in the preceding section from the proton yield in order to obtain the net proton density. In the case of the asymmetric p+C interaction, the equality of antiproton and pairproduced proton yields is only valid for the target part of the overall cross section due to isoscalar carbon nucleus, invoking isospin symmetry. For the projectile component on the other hand this does not apply. In the absence of precision data for antiproton production in n+C collisions it may be assumed that the same enhancement of pairproduced protons over antiprotons as in p+p interactions applies where a factor of 1.6 has been established [12]. This modifies the superposition scheme for antiprotons described in Sect. 14 by increasing the projectile contribution from 1.1 to 1.76 with respect to the input p+p densities. The resulting p _{ T } integrated density distribution for pair produced protons (hereafter denoted as \(\widetilde{\mathrm{p}}\)) is shown in Fig. 92.
This distribution is in contrast to Fig. 78 almost symmetric and the comparison to the measured antiproton densities demonstrates that this isospin effect is by no means negligible.
The corresponding net proton density distribution results from the subtraction of the pair produced protons from the total proton density distribution, Table 8 and Fig. 52. It is presented in Fig. 93 in the x _{ F } range influenced by pair production, −0.4<x _{ F }<+0.4.
The net proton density shows, in contrast to the total proton yield, a smooth behaviour around x _{ F }=0.
Target and projectile components in net proton production
The fragmentation of those nucleons in the carbon nucleus which are hit by the throughgoing projectile, here called the “target component”, is a quantity which should be closely related to the proper superposition of net proton production in the elementary p+p and p+n interactions, multiplied by the number of projectile interactions. Such a superposition has been shown to describe the target component of the antiproton yields, Sect. 14, up to a loss of about 12 % specific to multiple collisions and related to the strong sdependence of baryon pair production. For baryons this loss should be negligible as the baryon density is to first order sindependent at SPS energy.
For the prediction of the target component, knowledge about the two basic contributions from
is needed. The latter process may be related, via isospin symmetry, to the reaction
which is measured by the NA49 experiment [3]. The resulting prediction for the isospin averaged net proton density from p+p collisions is described in the following section.
Isospin averaged net proton density from p+p collisions
The p _{ T } integrated proton and neutron densities dn/dx _{ F } as measured by the NA49 experiment are shown in Fig. 94 as dotted and broken lines. The corresponding net proton yield is obtained by subtracting 1.6 times the measured antiproton yield. For the net neutron yield, the subtraction of the measured antiproton yield is indicated by the isospin symmetry of baryon pair production. In the case of the isoscalar carbon nucleus, a simple average of the two distributions is to be performed as indicated by the full line in Fig. 94.
Predicted target component of net proton production
In order to obtain the predicted target component of net proton production in p+C interaction, the predicted yield from p+p collisions has to be multiplied by the number of projectile collisions 〈ν〉=1.6 and by the target overlap function, Sect. 13. The resulting distribution is shown in Fig. 95 together with the total net proton yield, Sect. 15.1.
As a first result it may be seen that the target component nearly saturates the total yield at x _{ F }∼−0.2.
The projectile component of net proton production
The subtraction of the predicted target component from the overall net proton density, Fig. 95, allows now for the extraction of the projectile component of the p+C interaction. This is demonstrated in Fig. 96 which shows the net projectile component (full line) in comparison with the net projectile component in p+p collisions (broken line, Sect. 13).
Several features of these distributions are noteworthy:

This study allows for the first time the isolation of the net proton projectile component in p+A collisions over the full phase space.

In principle this net proton component is strongly constrained by baryon number conservation in comparison to p+p collisions, to the extent that the surface under the two distributions should be equal up to second order effects like a relative increase of neutron or hyperon production.

In fact the integrated yields are 0.547 and 0.52 net protons per inelastic event for p+p and p+C interactions, respectively. In view of the multistep methodology involved in extracting this experimental result, the agreement to within about 5 % is certainly compatible with the systematic uncertainties.

A relative increase of the net neutron yield, which is in principle not excluded in multiple hadronic interactions, is improbable as it has been shown, see Sect. 10.3, that the baryon number transfer is identical for neutrons and protons.

A relative increase of hyperon production can as well only have limited influence as an increase of Λ and Σ production by 50 % would only reduce the observed difference from 5 % to 4 %.

The shapes of the two distributions are rather similar, with a downward shift of about 0.15 units in x _{ F } in p+C except for the diffractive region which is governed by single projectile collisions

At x _{ F }<−0.2 there is a steep increase of the targetsubtracted density (shaded region in Fig. 96) which is due to the tail of protons from intranuclear cascading. This contribution will be discussed in detail below (Sect. 15.4). It is however to be noted that a clean separation of the projectile component from both the target and the nuclear cascading contributions is being achieved at SPS energy. At lower cms energies, the nuclear component will extend into higher x _{ F } ranges, covering x _{ F }=0 at AGS energy, as it scales in p _{lab} rather than x _{ F }.
It is interesting to extract the projectile overlap function from the ratio \(R^{c,\mathrm{net}}_{\mathrm{p}}\), see (23), between the projectile component and the symmetrized total density. This is shown in Fig. 97 in comparison with the corresponding function in p+p collisions.
As a further important result of this study it may be stated that in multiple collisions the width of the proton feedover from the projectile to the target hemisphere widens. In view of the discussion of resonance decay in Sect. 12.4 above, this would be compatible with an increase of the effective mass in the process of projectile excitation.
The nuclear component of net proton production
If the subtraction of the target component from the total net proton density distribution reveals the projectile component at x _{ F }>−0.2, it also should allow for the extraction of the nuclear component at x _{ F }≲−0.2. Here the nuclear component is defined as the retarded proton density produced by the intranuclear cascading of nucleons following the momentum transfer from the projectile to the nucleus, as opposed to the prompt fragmentation of those nucleons which are hit by the projectile.
The situation is clarified in Fig. 98 which shows the total net proton density dn/dx _{ F } for x _{ F }<−0.2 (full line) together with the target component discussed in the preceding section (broken line), Fig. 95.
The subtraction of the target component from the total yield, Fig. 99 (full line), results in a rather particular pattern.
This pattern features two distinct regions in x _{ F }. For the region of ±0.2 units around x _{ F }=−1, an abrupt bipolar instability arises from the presence of a diffractive peak in the predicted target component, whereas for the regions −1.6<x _{ F }<−1.2 and −0.8<x _{ F }<−0.2 a smooth x _{ F } distribution results which is well fitted by a Gaussian of the form
centered at x _{ F }=−0.92 with an rms of 0.265 as shown by the broken line in Fig. 99.
The diffractive component of the predicted target density should show up in any measurement of the total proton density in the region around x _{ F }=−1 if the nuclear component would have as expected a smooth behaviour across this region. Assuming the Gaussian fit to describe this smooth behaviour one may tentatively subtract the Gaussian shape from the total proton density as shown in Fig. 100.
This results in a modified target component (dotted line in Fig. 100) which reaches down to x _{ F } values at ∼−1.2 and goes smoothly through x _{ F }=−1. The difference between the modified and predicted target component is bipolar around x _{ F }=−1 and conserves, to first order, the total integrated density, as shown in Fig. 101.
In this context the action of the Fermi motion of the hit nucleons on the momentum distribution of protons in the diffractive peak should be recalled. Fermi motion may be approximated by a Gaussian momentum distribution of about 75 MeV/c rms width in the nuclear rest system. This translates at SPS energy to an rms width of about 0.085 in x _{ F }. Low momentum transfer processes like quasielastic scattering or diffraction convolute with this momentum distribution. This leads to a smearing of the peak structure characterized by a base width of ±2–3 times the Fermi rms around x _{ F }=−1. This is quantified by the Gaussian x _{ F } distribution with rms 0.085 in Fig. 101b which covers exactly the range of the observed deviation from the predicted diffractive peak. This convolution has been studied in quasielastic alpha–alpha scattering at the CERN ISR [48] where it was shown that low momentum transfer rescattering processes have only small influence on the longitudinal width in contrast to a substantial broadening of the transverse momentum distribution, see Sect. 14 below.
The extracted width of the nuclear component in longitudinal momentum with an rms of 0.265 units in x _{ F } is much larger than the spread expected from Fermi motion. This feature is known from quite a number of experiments since some decades [6] but is shown here for the first time to be symmetric, however not around x _{ F }=−1 but around x _{ F }=−0.92. This substantial transfer of baryon number needs comment. One effective mechanism contributing to the transfer of nucleons in longitudinal momentum is certainly the production of pions in the intranuclear cascade. In the excitation of I=3/2 states at pion threshold, the decay products are located at x _{ F }=−0.85 and x _{ F }=−0.15, respectively, for protons and pions, and for isobars at x _{ F }∼−1. For isobar masses above threshold the x _{ F } values of the decay baryons will shift further up.
The production of pions in the nuclear cascade has indeed been studied in the accompanying publication [6]. The backward pion yields have been separated into the two components of target fragmentation which may be predicted from elementary hadronic collisions, and of nuclear cascading, in close similarity to the argumentation carried out here for baryons. As a result the total number of pions in the nuclear component has been determined to 0.3 per inelastic event.
The Gaussian distribution of the nuclear component, Fig. 100, integrates to 0.6 protons per inelastic event, see Sect. 15.6 below. Isospin symmetry and the absence of charge exchange in the primary p+C interaction at SPS energy ask for an equal number of neutrons to be produced. This means that every fourth proton in the nuclear cascade produces a pion. In the decay of the isospin 3/2 isobars involved with pion production, the decay protons are transferred to x _{ F }=−0.85 at pion threshold with the decay pions being centred at x _{ F }=−0.15 for low lab momenta. Integrating over the pion transverse momentum distribution this center shifts down to about −0.2 [6] with a rather long tail towards lower x _{ F }. The corresponding nucleons will be placed at x _{ F }=−0.8 and above. The center of the nuclear component at x _{ F }=−0.92 is therefore compatible with pion production in the nuclear cascade via isobar excitation near threshold and the subsequent decay into baryons and pions. The symmetry of the nuclear component would however ask for a bigger pion yield at about one pion for every second proton. Here deexcitation processes without pion emission like final state isobarnucleon rescattering could be involved to reduce the pion yield.
In conclusion of the preceding sections on p _{ T } integrated proton distributions it may be stated that a threecomponent mechanism of convincing internal consistency has been established in a quantitative and precise way. These three components are defined by

The fragmentation of the projectile which obeys baryon number conservation and shows a transfer in longitudinal momentum corresponding to 0.15 units in Feynman x _{ F }.

The prompt fragmentation of the nucleons hit by the projectile. This component has been predicted from elementary proton–nucleon interactions invoking isospin symmetry and the mean number of projectile collisions.

The nuclear component which arises from intranuclear cascading and is partially accompanied by pion production.
At SPS energy the nuclear component extends up to x _{ F }=−0.2. It is well separated from the projectile fragmentation which feeds over into the target hemisphere down to the same value of x _{ F }=−0.2. The target fragmentation in turn reaches from x _{ F }=+0.2 down to x _{ F }=−1.2. The latter range is well beyond the kinematic limit of elementary fragmentation with a diffractive peak close to and above x _{ F }=−1. This sharp diffractive structure is evidently diluted and smoothed by quasielastic rescattering of its lowmomentum nucleons in accordance with experimental results from other experiments.
A remark about sdependence
Even if the SPS energy range is, as shown above, a well suited region for the separation of the three components contributing to the measured net baryon density, it is interesting to look at the expected evolution with \(\sqrt{s}\).
The nuclear component
The study [6] of backward proton production in p+C interactions shows that only small changes in the momentum distributions are to be expected by increasing \(\sqrt{s}\) to RHIC energy and beyond, or by decreasing it into the AGS energy region. Indeed one has to move down to \(\sqrt{s}\) below about 3 GeV in order to see threshold effects drastically reducing the proton density. In terms of the range in x _{ F } covered by the nuclear component, however, kinematics will extend the upper limit of ∼−0.25 at SPS energy to higher values until x _{ F }=0 is reached at \(\sqrt{s} \sim4~\mbox{GeV}\). This purely kinematic effect is presented in Fig. 102 where x _{ F } is plotted as a function of 1/\(\sqrt{s}\) for two values of p _{lab} and three values of p _{ T }.
This behaviour means that for given x _{ F } (or rapidity) the nuclear contribution will increase with decreasing beam momentum. This effect is of course also to be expected for peripheral heavy ion collisions where the separation of prompt baryons from the delayed nuclear cascade will become more important but also more difficult with decreasing interaction energy.
The target fragmentation
As shown above prompt net baryons from target fragmentation are well described by the superposition of elementary proton–nucleon collisions. With increasing \(\sqrt{s}\) this means that this contribution will move back in x _{ F } due to increasing transparency until at the highest ISR and at RHIC energies the central region around x _{ F }=0 will be only populated by pair produced baryons. In the x _{ F } region below ∼−0.3 the yields will not change appreciably due to the approximate scaling behaviour. Towards lower \(\sqrt{s}\) the feedover of the target fragmentation into the projectile hemisphere will accordingly increase. Together with the increasing nuclear component a clear separation will therefore become more involved.
The projectile component
The evolution of the projectile component with collision energy is of considerable interest as it carries unique information about multiple hadronic collisions. Since its diffractive part is connected—for minimum bias p+A collisions—to the fraction of single projectile collisions which is as discussed above on a level of 60 % for p+C interactions, there should be approximative energy scaling with a progressive widening of the peak towards lower energies as measured in p+p interactions. For the nondiffractive part the situation is however much less clear, in particular as there is no theoretical understanding of the observed baryon number transfer and as there is only very limited experimental information available on the required level of precision. It has been shown above that the net baryon density distribution shifts downward by 0.15 units of x _{ F } in p+C collisions, the same shift being observed for the neutrons. It has also been shown that this baryon number transfer increases with centrality as indicated by the dependence on the number of “grey” protons. It has also in addition been indicated that resonance production and decay presents a very effective source of baryon transfer. If with increasing interaction energy the excitation of the projectile proton in its multiple collisions also increases and therefore the spectrum of produced resonances extends to higher masses, the reduction of central net baryon density via transparency should be reduced or even compensated. At lower \(\sqrt{s}\) the situation should become, as for the two other contributions, more obscure due to the increased mutual overlap of the different components.
Proton and net proton multiplicities
Using the p _{ T } integrated density distributions dn/dx _{ F } extracted above for the inclusive p+C interaction as well as for the different subcomponents, the corresponding baryonic multiplicities may now be determined by integration over x _{ F }. In view of the statistical errors of the dn/dx _{ F }, Tables 8 and 9, which are of order 1 % and 3 % for p and \(\overline{\mathrm{p}}\), respectively, the statistical uncertainties of the total integration are negligible with respect to the systematic errors given below in percent of the yields. The integration limits in x _{ F } reach from −0.2 to 1 (projectile component, Fig. 96), from −1.2 to 0.2 (target component, Figs. 95 and 100), and from −1.7 to −0.2 (nuclear component, Fig. 100). This results in the following numbers:
There are two predictions respectively for the net projectile component and for the expected net target component established from the elementary p+p collisions [3]:
This assumes baryon number conservation and a negligible increase in neutron and hyperon production.
This uses isospin invariance and the measured number of 1.6 projectile collisions.
Subtracting the predicted target component from the total net proton density in the projectile fragmentation region, the multiplicity of net projectile protons is measured as
which reproduces the expected multiplicity to within 5.5 % and leaves room for some increase of the hyperon yields in p+C collisions.
Subtracting the predicted target component from the total net proton density in the backward region, the nuclear component is measured as
A Gauss fit to the nuclear component in the symmetric regions of the targetsubtracted proton density yields the multiplicity
which complies to within 3.6 % with the straightforward subtraction.
Finally there is the modified target component obtained by subtraction of the Gaussian nuclear component from the overall proton density which smooths the diffractive peak in accordance with the Fermi motion of the hit nucleons. This modified target component results in the multiplicity
which reproduces the predicted multiplicity (35) to within 2.9 %.
In conclusion it may be stated that the total measured net proton multiplicity made up by the superposition of three components of comparable magnitude, namely a projectile multiplicity of 0.52, a target multiplicity of 0.67 and a nuclear component of 0.65 units. These yields add up to 1.84 which is within 1 % equal to the direct integration (33). The multiplicities of antiprotons and pair produced protons are 0.052 and 0.065, respectively, corresponding to 2.9 % and 3.6 % of the total net proton yield.
Proton production in p+C collisions: p _{ T } dependence
Following the study of p _{ T } integrated yields in the preceding section, the doubledifferential proton cross sections will now be studied for the three components of projectile fragmentation, target fragmentation, and nuclear cascading, thus adding the transverse dimension to the experimental scrutiny. In order to comply with the discussion of the integrated proton yields dn/dx _{ F }, Sect. 15, the double differential cross sections will be used in their noninvariant form
see also (10). In a first step, the net proton cross sections will be defined using the results on antiprotons, Sect. 14. A detailed comparison of the overall backward cross sections with the predicted contribution from target fragmentation will reveal a necessary p _{ T } dependent modification of this component which will then be employed to extract in turn the projectile and nuclear components in their p _{ T } dependence.
Pair produced protons and net proton density
Using the results of the discussion of the double differential antiproton yields and their separation into target and projectile components in Sect. 14.2, the yield of pair produced protons may be estimated by multiplying the projectile component by the isospin factor 1.6, maintaining the p _{ T } enhancement as parametrized in (26). The target component stays equal to the antiproton yield due to isospin symmetry. The total and the resulting net proton densities are shown in Fig. 103 as a function of x _{ F } for different values of p _{ T }.
Target component
As discussed in Sect. 15.2.2 the target component of net proton production in p+C interactions may be predicted from p+p collisions using the number of projectile collisions 〈ν〉=1.6, the target overlap function \(R^{c,\mathrm{net}}_{\mathrm{p}}\) (see (23) and Fig. 72), and the measured proton and neutron cross sections [3]. The only additional assumption to be made for the double differential yield is the equality of the p _{ T } distributions for neutrons and protons, see [3] for experimental evidence. The result for the target component and its subtraction from the overall proton yield is shown in Fig. 104.
Compared to the same prediction and subtraction for the p _{ T } integrated densities, Figs. 95 and 96, a p _{ T } dependence becomes visible. It is the region of x _{ F } between −0.2 and −0.3 which is extremely sensitive to the predicted target yield. At transverse momenta below the mean p _{ T } (Fig. 55) the prediction overshoots the total density by about 20 %, whereas for higher p _{ T } it falls low by up to 40 % at p _{ T }=1 GeV/c. In this x _{ F } region neither the possible projectile feedover nor the nuclear component may explain, by their limited x _{ F } range, the observed p _{ T } dependence. Instead a yield suppression at low p _{ T } followed by an enhancement at high p _{ T } similar to the one found for antiprotons, Sect. 14.2, has to be invoked also for the target contribution. This pattern of yield suppression and enhancement is quantified in Fig. 105a as a function of x _{ F } for the p _{ T } values shown in Fig. 104. Given the estimated systematic error margins, Fig. 105b, the effect is significant for p _{ T }> 0.7 GeV/c. It should be noted that baryon number conservation imposes, for a yield increase in this p _{ T } range, a corresponding yield suppression at low p _{ T }.
This phenomenon is also borne out by a comparison of the mean p _{ T } values between p+C and p+p interactions shown in Fig. 106.
If the target component showed a p _{ T } dependence equivalent to p+p interactions, the mean p _{ T } values should approach the ones for p+p at x _{ F } around −0.2 to −0.3 where target fragmentation prevails. The observed difference of 50 MeV/c in 〈p _{ T }〉 is significant with respect to the statistical errors of less than 1 %. The systematic errors are of the same order as most error sources, or for certain the normalization error, cancel in the mean value.
Applying this enhancement, the target component and its subtraction from the total measured yield take the pattern shown in Fig. 107.
This subtraction leaves clearly defined and separated projectile and nuclear components which will be discussed in the subsequent sections.
The projectile component
The hadronization of the projectile is already clearly visible in the dotted line of Fig. 107. It saturates the total yield at x _{ F }>0.2 and comes down to zero at x _{ F }∼−0.2 due to the limited range of the baryonic overlap function. In order to put this behaviour in perspective as far as the x _{ F } distributions for different transverse momenta are concerned, the projectile components normalized to their maximum densities are presented in Fig. 108.
Compared to the p _{ T } integrated distribution, Fig. 96, there is a clear dependence of baryon number transfer on p _{ T }. The maximum density shifts from x _{ F }=0.3 at low p _{ T } to x _{ F }=0.1 at 1 GeV/c. The density at x _{ F }≳0.6 corresponding to low mass excitation is strongly reduced with increasing p _{ T } whereas the transfer function is successively extending further into the backward hemisphere.
Further information concerning the p _{ T } dependence comes from a direct comparison to p+p interactions. Extracting the projectile component from the symmetric p+p collision using the baryonic overlap function determined in Sect. 12 the ratio
may be obtained as shown in Fig. 109 as a function of p _{ T } for different values of x _{ F }.
A clear increase with p _{ T } of the net proton yields is visible for all values of x _{ F }. The overall increase of the cross sections with decreasing x _{ F } is due to the general baryon number transfer in p+C interactions visible in the p _{ T } integrated distributions of Fig. 57 (“minimum bias” compared to p+p). This can be normalized out by multiplying R ^{proj} by the integrated density ratio between p+p and p+C collisions:
The resulting ratio \(R^{\mathrm{proj}}_{\mathrm{norm}}\) is shown in Fig. 110 again as a function of p _{ T } for different values of x _{ F }.
The wide spread observed in Fig. 109 reduces to a narrow band of p _{ T } enhancements which are about independent on x _{ F } except for the x _{ F } range approaching diffraction. Again, as for \(\overline{\mathrm{p}}\) in Sect. 14.2 and for the target component in the preceding section, the normalized densities are reduced by 10–20 % at low p _{ T } and enhanced to factors of about 1.5 at p _{ T }=1.5 GeV/c.
The nuclear component
The onset of the contribution from nuclear cascading is already visible in Fig. 107 by the dotted lines at x _{ F }<−0.25. This range is extended to the far backward hemisphere down to x _{ F }=−1.6 in Fig. 111. In this figure the total proton density, the predicted target contribution and the target subtracted yield are shown as a function of x _{ F } for five values of p _{ T } between 0.2 and 1 GeV/c.
As already discussed for the p _{ T } integrated densities in Sect. 15.4 (Figs. 98 and 99), the presence of the diffractive peak from proton fragmentation in the predicted target contribution creates a sharp spike between x _{ F }∼−0.9 and x _{ F }=−1.0 which should be visible in the total proton density distribution in this area. The absence of such structure in the measured yield indicates, as argued in Sect. 15.4, a smoothing of the predicted structure via quasielastic rescattering of the diffrative protons inside the Carbon nucleus. This rescattering extends typically up to ±0.2 units of x _{ F } around x _{ F }=−1 [48]. Beyond this range the target subtracted yield shows a Gaussian behaviour as presented in Fig. 112.
The fit parameters show, within tight errors, a stable mean value in x _{ F } between −0.92 and −0.93 in agreement with the p _{ T } integrated fit (29). The rms deviation increases with p _{ T } from 0.22 to 0.3 units of x _{ F }. The p _{ T } dependences of the maximum density and of the yield integrated over x _{ F } are shown in Fig. 113.
It is interesting to observe that the p _{ T } dependence of the nuclear component is not Gaussian and corresponds to the one measured in the diffractive region of p+p interactions [3].
Using the Gaussian fits as an estimator of the nuclear component a modified target component may be obtained by subtracting these fitted densities from the total proton yield as shown in Fig. 114.
The resulting modified target component extends now to x _{ F } values below −1.0 and shows a smooth behaviour through the region of proton diffraction in accordance with the p _{ T } integrated yield, Sect. 15.4.
Conclusion
As part of a comprehensive study of hadronic production in elementary and nuclear collisions at the SPS, new data from the NA49 experiment on proton, antiproton, neutron and light ion production in minimum bias p+C interactions are presented. Making full use of the acceptance coverage and the particle identification capabilities of the NA49 detector, a wide phase space area from the far forward direction at Feynman x _{ F } of 0.95 to the far backward direction down to x _{ F }=−0.8 has been exploited. Using available data from a Fermilab experiment the data coverage could be further extended into the nuclear fragmentation region down to x _{ F }∼−2.0. In addition, deuteron and triton production have been studied in the lab momentum range from 0.25 to 3 GeV/c making available there for the first time cross sections in the low to medium p _{ T } region. In addition a limited amount of data with “grey” proton detection allows for a first look at the centrality dependence of baryon number transfer.
Given the complete phase space coverage of the combined data set, the main aim of this publication is the separation and isolation of the three components of hadronization in p+C collisions, namely projectile fragmentation, target fragmentation and nuclear cascading. This study has been conducted both for p _{ T } integrated quantities and using double differential cross sections to obtain a complete view of the p _{ T } dependence. For this aim, the baryonic overlap functions from the projectile to the target regions and vice versa have been determined experimentally using both the elementary p+p and the asymmetric p+C interactions. This has been achieved in a completely modelindependent way relying essentially on baryon number conservation and isospin symmetry. For antiproton production the absence of a nuclear contribution has been shown and the superposition of the target and the projectile fragmentation has been established using the known number of projectile collisions inside the Carbon nucleus. This allows for the definition of the yield of pair produced protons and thereby of net proton densities.
In contrast to the a priory unknown projectile and nuclear components, the target fragmentation occupies a special place as it should at least to first order be describable by a superposition of single nucleon fragmentations taking of course into account the number of projectile collisions and isospin effects. This approach works out well for p _{ T } integrated proton densities with the exception of the diffractive contribution contained in the elementary interactions. This contribution is evidently smeared out by secondary, quasielastic interactions of the corresponding low momentum protons in the nuclear rest system. The subtraction of the thus predicted target component yields both the projectile and the nuclear components. The former is proven to preserve baryon number combined with a sizeable amount of baryon transfer of order 0.15 units of x _{ F }. The latter turns out to have a Gaussian shape in x _{ F } centred at x _{ F }=−0.92 with a substantial FWHM of 0.6 units far in excess of the narrow x _{ F } distribution centred close to −1.0 which might be expected from Fermi motion alone. In the case of the p+C collisions studied here, the three components have comparable total yields of 0.52, 0.67 and 0.65 net protons respectively for the projectile, target and nuclear contributions. This sums up to 1.84 net protons in total, comparing to within 1 % with the independent direct yield integration of 1.82 net protons (33).
The study of double differential cross sections gives access to the additional dimension of transverse momentum. All three components show a distinct transverse activity which goes beyond the naive expectation from elementary collisions or nuclear binding. The projectile component features, both for protons and antiprotons, a suppression by 10–20 % at low p _{ T } followed by an enhancement of about 50 % at p _{ T }=1.5 GeV/c. This pattern is rather x _{ F } independent in the forward hemisphere. The target component shows a similar behaviour, however with a distinct x _{ F } dependence centred at x _{ F }∼−0.3. The nuclear component finally has a wide, nonGaussian p _{ T } dependence which goes far beyond the one expected from Fermi motion and which is shown to be comparable to the one measured in the diffractive region of p+p interactions.
As for the previous publications [1–4] the measured cross sections and twodimensional interpolation values are available on the Web Site [13].
References
 1.
C. Alt et al., Eur. Phys. J. C 45, 343 (2006)
 2.
T. Anticic et al., Eur. Phys. J. C 68, 1 (2010)
 3.
T. Anticic et al., Eur. Phys. J. C 65, 9 (2010)
 4.
C. Alt et al., Eur. Phys. J. C 49, 897 (2007)
 5.
G. Barr et al., Eur. Phys. J. C 49, 919 (2007)
 6.
O. Chvala et al. arXiv:1210.6775 [nuclex]
 7.
Y.D. Bayukov et al., Phys. Rev. C 20, 764 (1979)
 8.
S. Afanasiev et al., Nucl. Instrum. Methods Phys. Res., Sect. A 430, 210 (1999)
 9.
S. Frankel et al., Phys. Rev. C 20, 2257 (1979)
 10.
D. Barton et al., Phys. Rev. D 27, 2580 (1983)
 11.
A.E. Brenner et al., Phys. Rev. D 26, 1497 (1982)
 12.
H.G. Fischer et al., Heavy Ion Phys. 17, 369 (2003)
 13.
 14.
 15.
N.A. Burgov et al., Sov. J. Nucl. Phys. 30, 371 (1979). Yad. Fiz., 30, 720 (1979)
 16.
K. Braune et al., Z. Phys. C 13, 191 (1982)
 17.
J.L. Bailly et al., Z. Phys. C 35, 301 (1987)
 18.
N.A. Nikiforov et al., Phys. Rev. C 22, 700 (1980)
 19.
NA49 collaboration, Inclusive charged kaon production in p+C interactions. To be published
 20.
R. Bailey et al., Z. Phys. C 29, 1 (1985)
 21.
T.S. Nigmanov et al., Phys. Rev. D 83, 012002 (2011)
 22.
A.S. Carroll et al., Phys. Lett. B 80, 319 (1979)
 23.
V. Blobel et al., Nucl. Phys. B 69, 454 (1974)
 24.
V. Blobel et al., Nucl. Phys. B 135, 379 (1978)
 25.
E.E. Zabrodin et al., Phys. Rev. D 52, 1316 (1995)
 26.
M.Yu. Bogolyubsky et al., Sov. J. Nucl. Phys. 50, 424 (1989). Yad. Fiz. 50, 683 (1989)
 27.
V.V. Ammosov et al., Nuovo Cimento A 40, 237 (1977)
 28.
V.V. Ammosov et al., Nucl. Phys. B 115, 269 (1976)
 29.
V.V. Abramov et al., Nucl. Phys. B 173, 348 (1980)
 30.
M. Bourquin, J.M. Gaillard, Nucl. Phys. B 114, 334 (1976)
 31.
A. Breakstone et al., Z. Phys. C 21, 321 (1984)
 32.
M. AguilarBenitez et al., Z. Phys. C 50, 405 (1991)
 33.
U. Idschok et al., Nucl. Phys. B 140, 365 (1978)
 34.
D. Denegri et al., Nucl. Phys. B 114, 413 (1976)
 35.
L. Baksay et al., Phys. Lett. 53B, 484 (1975)
 36.
C. Conta et al., Nucl. Phys. B 175, 97 (1980)
 37.
C. Amsler et al., Phys. Lett. B 667, 1 (2008)
 38.
A. Suzuki et al., Nucl. Phys. B 172, 327 (1980)
 39.
D. Drijard et al., Z. Phys. C 9, 293 (1981)
 40.
J.W. Lamsa et al., Phys. Rev. D 26, 1769 (1982)
 41.
M. Rozanska et al., Nucl. Phys. B 162, 505 (1980)
 42.
 43.
 44.
 45.
T. Anticic et al., Phys. Rev. C 83, 014901 (2011)
 46.
A.M. Rossi et al., Nucl. Phys. B 84, 269 (1975)
 47.
G.I. Veres et al., Nucl. Phys. A 661, 383c (1999)
 48.
W. Bell et al., Nucl. Phys. B 254, 475 (1985)
Acknowledgements
This work was supported by the Polish State Committee for Scientific Research (P03B00630), the Polish National Science Centre (on the basis of decision no. DEC2011/03/B/ST2/02634) the Bulgarian National Science Fund (Ph09/05), the EU FP6 HRM Marie Curie IntraEuropean Fellowship Program, the Hungarian Scientific Research Fund OTKA (T68506) and the Hungarian OTKA/NKTH A0877719 and A0877815 grants.
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Baatar, B., Barr, G., Bartke, J. et al. Inclusive production of protons, antiprotons, neutrons, deuterons and tritons in p+C collisions at 158 GeV/c beam momentum. Eur. Phys. J. C 73, 2364 (2013). https://doi.org/10.1140/epjc/s1005201323643
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