The inclusive single-particle spectra of π−, KS0 and Λ in proton-proton collisions at 19 GeV/c

V0 production in p+A collisions at $\sqrt{s}=41.6$ GeV

“…The curves correspond to parameterizations of the present measurements as explained in the text Fig. 9 A compilation of total cross section measurements from references [6][7][8][9][10][11][12][13][14][15][16][17][18][19][20][21][22][23][24] and HERA-B for (a) K 0 S and (b) Λ andΛ production vs. squared CM energy (s). The recalculated data from Erhan et al [22] are indicated by diamonds and stars y = 0 measurements of [49] are also about a factor of two higher than the present measurement.…”

“…Numerous studies have been made (see [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17][18][19][20], and references therein) including fixed-target experiments at Center-of-Mass (CM) energies up to 40 GeV, mainly with bubble chambers, as well as at CERN's Intersecting Storage Ring in the 1970s and early 1980s (see [21][22][23][24]) and later at the SPS Collider [25]. More recently, studies of strangeness production at a CM energy of 200 GeV in both proton-proton and deuterongold collisions at RHIC have been published [26,27].…”

Performance of Monte Carlo event generators of pp collisions at NICA energies

“…Early data on hadron production mostly come from 60s and 70s from fixed-target experiments on accelerator facilities in Brookhaven (BNL, fix target, incident proton energies: 2.4, 2.85, 5, 6.9 8 GeV, [19][20][21][22][23][24]), Princeton (PPA, i. e. Princeton-Pensilvania Accelerator, incident beam energies: 2.54, 2.88, 3.03 GeV [25]) in Princeton, CERN (PS, i. e. Proton Synchrotron Saclay 81-cm hydrogen bubble chamber, incident proton energy: 5.5 GeV, 19 GeV, 12, 24 GeV [26][27][28][29][30]; SPS, i. e. Super Proton Synchrotron, 200, 360 GeV [31,32]), Argonne National Laboratory (ANL, incident beam momentum 6, 102 GeV [33,34], ZGS, i. e Zero Gradient Synchrotron, incident proton momentum 12, 12.4 GeV/c [35,36]), Serpukhov (Serpukhov accelerator, incident beam momentum 32, 69 GeV/c [37,38]), Fermilab (Main Ring, incident beam momentum: 100, 147, 200, 205, 300, 400 GeV/c [39][40][41][42][43][44]). Particle identification in early experiments was done by the means of bubble chambers [19, 21-24, 26, 27, 29, 30, 33-35, 37-39, 41-44] or using either time of flight cameras, Cherenkov detectors or both [20,25,28,36] in counter-based experiments.…”