References
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The r.h.s. of eq. (11) is energy-independent, but no scaling property is required. At least form=1, equation (11) is satisfied by a wide class of models including recent ones which predict large cross-sections at high transverse momenta:D. Amati, L. Caneschi andM. Testa:Phys. Lett.,43 B, 186 (1973);M. Greco andY. N. Srivastava:Inclusive production at large mass and large transverse momentum, CERN TH-1616 (1973). In the casem>1, we assume no violation of eq. (11) from the long-range correlations between the particlec m and the particlesc t (i<m) whens→∞.
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No error bars are shown in Fig. 1 and 2, because here the statistical errors are less important than the systematical ones due to 1) the reading of the single-particle distributions from plots, 2) the construction of the neutron spectra in Fig. 2b) (see ref. (5), andA. L. M. Mihul andT. Besliu:Average quantum numbers per particle. What are they good for?, JINR E1-6745, Dubna (1972)), 30 the normalization of the distributions from different experiments (seeE. Flaminio, J. D. Hansen, D. R. O. Morrison andN. Tovey:Compilation of cross-sections, CERN-HERA 70-2, 70-5, 70-7 (1970);V. Barger andR. J. N. Phillips:Nucl. Phys.,32 B, 93 (1971)).
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Berceanu, S., Besliu, T., Gheorghe, A. et al. Asymptotic properties of charge distributions. Lett. Nuovo Cimento 8, 345–352 (1973). https://doi.org/10.1007/BF02724593
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DOI: https://doi.org/10.1007/BF02724593