FIZIKA B 11 (2002)  1, 27-48

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PARTON DISTRIBUTIONS IN NUCLEON ON THE BASIS OF A RELATIVISTIC INDEPENDENT QUARK MODEL

N. BARIKa and R. N. MISHRAb

aDepartment of Physics, Utkal University, VaniVihar, Bhubaneswar-751004, India

bDepartment of Physics, Dhenkanal college, Dhenkanal-759001, Orissa, India

Received 15 August 2001; Accepted 25 February 2002
Online 25 May 2002

At a low resolution scale with Q2 = m2 corresponding to the nucleon bound state, deep inelastic unpolarized structure functions F1(x,m2) and F2(x,m2) are derived, with correct support using the symmetric part of the hadronic tensor under some simplifying assumptions in the Bjorken limit. For doing this, the nucleon in its ground state has been represented by a suitably constructed momentum wave packet of its valence quarks in their appropriate SU(6) spin flavour configuration, with the momentum probability amplitude taken phenomenologically in reference to the independent quark model of scalar-vector harmonic potential. The valence quark distribution functions uv(x,m2) and dv(x,m2), extracted from the structure function F1(x,m2) in a parton model interpretation, satisfy normalization constraints as well as the momentum sum-rule requirements at a bound state scale of m2 = 0.1 GeV2. QCD evolution of these distribution functions taken as the inputs, yields at Q02 = 15 GeV2,xuv(x,Q02) and xdv(x,Q02) in good qualitative agreement with the experimental data. The gluon distribution G(x,Q02) and the sea-quark distribution qs(x,Q02), which are dynamically generated using the leading order renormalization group equation, also match reasonably well with the available experimental data.

PACS numbers: 12.39.pn,12.39.ki,13.60.Hb,13.90.+i
UDC 539.126

Keywords: nucleon bound state, deep inelastic unpolarized structure functions, Bjorken limit, independent quark model of scalar-vector harmonic potential, parton model, comparison with experimental data

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