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TheCharmoftheProtonandthe$Lambda_c^{}$Production
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The Charm of the Proton and the Λ
+
c
Production
1
J. dos Anjos, G. Herrera2, J. Magnin and F.R.A. Sima?o
CBPF, Rua Dr. Xavier Sigaud 150, CEP 22290-180 - Urca RJ, Rio de Janeiro, Brazil
Abstract. We propose a two component model for charmed baryon production
in pp collisions consisting of the conventional parton fusion mechanism and frag-
mentation plus quarks recombination in which a ud valence diquark from the
proton recombines with a c-sea quark to produce a Λ+c . Our two-component
model is compared with the intrinsic charm two-component model and experi-
mental data.
INTRODUCTION
The production mechanism of hadrons containing heavy quarks is not well
understood. Although the fusion reactions gg → QQ? and qq → QQ? are sup-
posed to be the dominant processes, they fail to explain important features of
heavy quark hadro-production like the leading particle effects observed in D±
produced in π?p collisions [1], Λ+c production in pp interactions [2] [3] and in
others baryons containing heavy quarks [4], the J/Ψ cross section at large xF
observed in πp collisions [5], etc.
The above mentioned effects have been explained using a two-component
model [6] consisting of the parton fusion mechanism calculable in perturbative
QCD plus the coalescence of intrinsic charm [7].
In hadron-hadron collisions the recombination of valence spectator quarks
with c-quarks present in the sea of the initial hadron is a possible mechanism
for charmed hadron production. Here we explore that possibility for the Λ+c ’s
production in pp interactions. We will assume that in addition to the usual
parton fusion processes, a ud diquark recombines with c-sea quark both from
the incident proton.
1) This work was partially supported by Centro Latino Americano de F??sica (CLAF).
2) Permanent address: CINVESTAV, Apdo Postal 14-740 Me?xico DF,Me?xico
c? 1995 American Institute of Physics 1
2We compare our results with those of the intrins
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