Production of mesons and baryons at high rapidity and high p(T) in proton-proton collisions at square root[s] = 200 GeV.

We present particle spectra for charged hadrons pi(+/-), K(+/-), p, and p[over] from pp collisions at square root[s] = 200 GeV measured for the first time at forward rapidities (2.95 and 3.3). The kinematics of these measurements are skewed in a way that probes the small momentum fraction in one of the protons and large fractions in the other. Large proton to pion ratios are observed at values of transverse momentum that extend up to 4 GeV/c, where protons have momenta up to 35 GeV. Next-to-leading order perturbative QCD calculations describe the production of pions and kaons well at these rapidities, but fail to account for the large proton yields and small p[over]/p ratios.

[1]  R. Debbe,et al.  The BRAHMS ring imaging Cherenkov detector , 2007, physics/0701281.

[2]  Y. Wang,et al.  Identified hadron spectra at large transverse momentum in p+p and d+Au collisions at,root(NN)-N-S=200 GeV , 2006 .

[3]  B. Kniehl,et al.  Fragmentation functions for light charged hadrons with complete quark flavour separation , 2005, hep-ph/0502188.

[4]  R. Debbe,et al.  On the evolution of the nuclear modification factors with rapidity and centrality in d + Au collisions at s(NN)**(1/2) = 200-GeV , 2004, nucl-ex/0403005.

[5]  C. Bourrely,et al.  Do we understand the single-spin asymmetry for $\pi^0$ inclusive production in pp collisions? , 2003, hep-ph/0311110.

[6]  R. Debbe,et al.  Transverse momentum spectra in Au+Au and d+Au collisions at s**(1/2) = 200-GeV and the pseudorapidity dependence of high p(T) suppression. , 2003, nucl-ex/0307003.

[7]  K. J. Foley,et al.  Evidence from d+Au measurements for final-state suppression of high-p(T) hadrons in Au+Au collisions at RHIC. , 2003, Physical review letters.

[8]  E. al.,et al.  Absence of suppression in particle production at large transverse momentum in sqrt[s(NN)]=200 GeV d+Au collisions. , 2003, Physical review letters.

[9]  E. al.,et al.  Midrapidity Neutral-Pion Production in Proton-Proton Collisions at √s = 200 GeV , 2003, hep-ex/0304038.

[10]  B. Jager,et al.  Next-to-leading order QCD corrections to high p(T) pion production in longitudinally polarized pp collisions , 2002, hep-ph/0211007.

[11]  D. Florian Next-to-leading order QCD corrections to one-hadron production in polarizedppcollisions at BNL RHIC , 2002, hep-ph/0210442.

[12]  J. Huston,et al.  New generation of parton distributions with uncertainties from global QCD analysis , 2002, hep-ph/0201195.

[13]  E. Leader,et al.  Fragmentation functions from semi-inclusive DIS pion production and implications for the polarized parton densities , 2001, hep-ph/0108055.

[14]  B. Kniehl,et al.  Testing the universality of fragmentation functions , 2000, hep-ph/0011155.

[15]  S. Mrenna,et al.  High-energy physics event generation with PYTHIA 6.1 , 2000, hep-ph/0010017.

[16]  P. G. Verdini,et al.  Studies of quantum chromodynamics with the ALEPH detector , 1998 .

[17]  M. Deninno,et al.  Inclusive charged particle cross-sections in full phase space from proton proton interactions at ISR energies , 1995 .

[18]  F. Videbæk The BRAHMS experiment at RHIC , 1994 .

[19]  R. Venugopalan,et al.  Computing quark and gluon distribution functions for very large nuclei. , 1993, Physical review. D, Particles and fields.

[20]  R. S. DeWolf,et al.  Inclusive jet cross-section and a search for quark compositeness at the CERN pp Collider , 1991 .

[21]  E. Reya Perturbative Quantum Chromodynamics , 1981 .

[22]  A. G. Frodesen,et al.  Identified charged particles in quark and gluon jets , 2000 .