Collinearity approximations and kinematic shifts in partonic shower algorithms
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We study kinematic effects due to the approximation of on-shell, collinear partons in shower Monte Carlo event generators. We observe that the collinearity approximation, combined with the requirements of energy-momentum conservation, gives rise to a kinematic shift, event by event, in longitudinal momentum distributions. We present numerical results in the case of jet and heavy-flavor production processes measured at the LHC.
KeywordsLarge Hadron Collider Transverse Momentum Parton Showering Parton Distribution Function Longitudinal Momentum
Phenomenological analyses of complex final states produced by hard processes at the Large Hadron Collider (LHC) rely on event simulation by parton shower Monte Carlo generators . These are used both to supplement finite-order perturbative calculations with all-order, leading-logarithmic QCD radiative terms and to incorporate nonperturbative effects from hadronization, multiple parton interactions, underlying events [2, 3, 4].
The shower Monte Carlo generators [2, 3, 4] treat QCD multi-parton radiation within collinear ordering approximations. These approximations have proved to be very successful for Monte Carlo simulation of final states at LEP and Tevatron. On the other hand at the LHC, unlike previous collider experiments, the phase space opens up for events with multiple hard scales and multiple jets to occur with sizeable rates, while the angular and rapidity coverage of detectors extends over a much wider range. In this case corrections to collinear ordering can significantly affect the structure of multi-jet final states [5, 6, 7]. This, for instance, will influence uncertainties  of NLO-matched shower calculations  for jet observables.
In this letter we investigate effects of kinematic origin arising from collinearity approximations in the parton showering algorithms. While the dynamical corrections studied in [5, 6, 7] come from terms beyond NLO in QCD perturbation theory (possibly enhanced in certain regions of phase space), the contributions studied in this paper are not obviously suppressed by powers of the strong coupling. Rather, they correspond to approximations made by showering algorithms in the parton kinematics. They can be discussed already at the level of leading-order and next-to-leading-order [8, 9] shower calculations.
We find that the collinearity approximation, combined with the requirements of energy-momentum conservation, gives rise to a kinematic shift, event by event, in longitudinal momentum distributions. The size of this shift depends on the observable and on the phase space region, but becomes in general non-negligible with increasing rapidities. In Sect. 2 we discuss the physical origin of this effect. In Sect. 3 we present numerical illustrations for jet production and b-flavor production based on NLO event generators. We give concluding remarks in Sect. 4.
2 Longitudinal momentum shifts in parton showers
Consider inclusive jet hadro-production. LHC experiments have measured one-jet cross sections [10, 11, 12] over a kinematic range in transverse momentum and rapidity much larger than in any previous collider experiment. Two kinds of comparison of experimental data with standard model theoretical predictions have been carried out. The first is based on NLO calculations  supplemented by nonperturbative (NP) corrections estimated from shower Monte Carlo generators [10, 11, 12]. This shows that the NLO calculation agrees with data at central rapidities, while increasing deviations are seen with increasing rapidity at large transverse momentum p T .
A second comparison  is based on Powheg calculations , in which NLO matrix elements are matched with parton showers [2, 3, 4]. This data comparison shows large differences in the high-rapidity region between results obtained by interfacing Powheg with different shower models [2, 3, 4] and different model tunes .
The dependence of high-rapidity jet distributions on parton showering effects is discussed in [16, 17, 18] based on results  from high-energy factorization [19, 20, 21]. These results are valid to single-logarithmic accuracy in the jet rapidity and the jet transverse momentum, and resum terms to all orders in the strong coupling α s . In the approach [7, 16, 17, 18] forward jet production is dominated by the scattering of a highly off-shell, low-x parton off a nearly on-shell, high-x parton. As noted in [16, 17, 18], this leads to a sizeable fraction of reconstructed jets receiving contribution from final-state partons produced by showering rather than just partons from hard matrix elements.
In the next section we illustrate the longitudinal momentum shifts numerically for jet and heavy-flavor production using Powheg.
3 Numerical results
We see from the upper plots in Fig. 1 that the kinematical reshuffling in the longitudinal momentum fraction is negligible for high-x partons but it is significant for low-x partons. This effect characterizes the highly asymmetric parton kinematics [16, 17, 18]. We note that in NLO shower calculations, since the perturbative weight for each event is determined by the initial Powheg simulation, predictions for observables sensitive to this asymmetric region can be affected significantly by the kinematical shift in Fig. 1. Similarly, since the momentum reshuffling is done after evaluation of the parton distribution functions, the kinematical shift can affect predictions also through the pdfs. It will be of interest to examine the impact of this phase space region on total cross sections as well.
The lower plots in Fig. 1 illustrate the distribution of transverse momenta in the initial state as a result of parton showering. We see that this distribution falls off rapidly for the low-k t initial-state parton, while the distribution for the high-k t initial-state parton has a significant large-k t tail. This provides an illustration, at the next-to-leading order, of the physical picture described in Sect. 2 based on the single-logarithmic, resummed results of [7, 16, 17, 18].
The longitudinal momentum shifts computed in this section may affect parton distribution functions in parton shower calculations. Although we have illustrated the shifts using the event generator Powheg, the effect is common to other calculation methods using collinear shower algorithms. Further studies of this effect will be reported elsewhere.
In this letter we have observed that, in the particular phase space regions for which inclusive jets and b-jets are measured at the LHC, QCD parton showers are sensitive to kinematic corrections associated with approximations of on-shellness and collinearity on the partonic states to which branching algorithms are applied.
Kinematic reshuffling in the longitudinal momentum fractions comes from the implementation of energy-momentum conservation in collinearly ordered showering algorithms. It depends on the emitted transverse momenta, and is present at leading order as well as at next-to-leading order. We have illustrated this effect quantitatively using NLO-matched event generators.
While the effect is generally small for central production if the center-of-mass energy is not too high, we have found that it becomes sizeable in kinematic regions probed by hard production processes at the LHC, for instance jet and heavy-flavor production at high rapidity. These regions have not been accessed experimentally before at previous colliders (e.g., at the Tevatron).
The event-by-event shift in longitudinal momentum distributions affects predictions through both perturbative weights and parton distribution functions. It contributes in particular to the uncertainty on predictions which incorporate results of collinearly ordered showering algorithms.
Formulations that keep track of non-collinear (i.e., transverse and/or anti-collinear) momentum components using unintegrated parton distributions [27, 28, 29, 30, 31, 32, 33] will be helpful to take account of the kinematic effect of longitudinal momentum shifts. It will also be of interest to investigate the relative size of the kinematic contribution studied in this article with respect to high-energy dynamical [5, 6, 7] effects on jet final states which can be included by unintegrated formalisms.
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