Abstract
Considering the nucleon as consisting entirely of its valence quarks confined independently in a scalar-vector harmonic potential; unpolarized structure functions F 1(x, μ 2) and F 2(x, μ 2) are derived in the Bjorken limit under certain simplifying assumptions; from which valence quark distribution functions u v(x, μ 2) and d v(x, μ 2) are appropriately extracted satisfying the normalization constraints. QCD-evolution of these input distributions from a model scale of μ 2=0.07 GeV2 to a higher Q 2 scale of Q 20 =15 GeV2 yields xu v(x, Q 20 ) and xd v(x, Q 20 ) in good agreement with experimental data. The gluon and sea-quark distributions such as G(x, Q 20 ) and q s(x, Q 20 ) are dynamically generated with a reasonable qualitative agreement with the available data; using the leading order renormalization group equations with appropriate valence-quark distributions as the input.
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References
R G Roberts and M R Whalley, J. Phys. G17, D1 (1991)
S R Mishra and F Sciulli, Ann. Rev. Nucl. Part. Sci. 39, 259 (1989) and the references therein
J F Owens and W K Tung, Ann. Rev. Nucl. Part. Sci. 42, 291 (1992)
A Milsztajn et al, Z. Phys. C49, 527 (1991) and the references therein
P Amaudruz et al. Phys. Rev. Lett. 66, 2712 (1991)
T Sloan, G Smadja and R Voss, Phys. Rep. 162, 45 (1988)
J J Aubert et al, Nucl. Phys. B293, 740 (1987) New Muon Collaboration: D Allasia et al, Report No. CERN-PPE/90-103 (1990)
BCDMS collaboration: A C Benvenuti et al, Phys. Lett. B237, 599 (1990)
G Altarelli and G Parisi, Nucl. Phys. B126, 298 (1977)
M Göckler et al, J. Phys. G22, 703 (1996)
R L Jaffe, Phys. Rev. D11, 1953 (1975)
C J Benesh and G A Miller, Phys. Rev. D36, 1344 (1987)
C J Benesh and G A Miller, Phys. Rev. D38, 48 (1988)
X M Wang, X Song and P C Yin, Hadron J. 6, 985 (1983)
X M Wang, Phys. Lett. B140, 413 (1984)
X Song and J S Mc Carthy, Phys. Rev. D49 3169 (1994); C46, 1077 (1992)
H Meyer and P J Mulders, Nucl. Phys. A528, 589 (1991)
M Traini, L Conci and U Moschella, Nucl. Phys. A544, 731 (1992)
A W Schreiber, A I Signal and A W Thomas, Phys. Rev. D44, 2653 (1991)
M R Bate and A I Signal, J. Phys. G18, 1875 (1992)
T N Pham, Phys. Rev. D19, 707 (1979)
A Dhaul, A N Mitra and A Pagnamenta, Z. Phys. C36, 115 (1987)
M V Terentev, Yad. Fiz. Sov. J. Nucl. Phys. 24, 207 (1976); 106 (1976)
Z Dziembowski, C J Martoff and P. Zyla, Phys. Rev. D50, 5613 (1994)
H J Weber, Phys. Rev. D49, 3160 (1994)
R P Bickerstaff and J L Londergan, Phys. Rev. 42, 3621 (1990)
M Stratmann, Z. Phys. C60, 763 (1993)
N Barik, B K Dash and M Das, Phy. Rev. D31, 1652 (1985); D32, 1725 (1985)
N Barik and B K Dash, Phy. Rev. D34, 2092, 2803 (1986), D33, 1925 (1986)
N Barik, B K Dash and P C Dash, Pramana — J. Phys. 29, 543 (1987)
N Barik, P C Dash and A R Panda, Phys. Rev. D46, 3856 (1992); D47, 1001 (1993)
N Barik and P C Dash, Phys. Rev. D47, 2788 (1993); D53, 1366 (1996)
N Barik, S Tripathy, S Kar and P C Dash, Phys. Rev. D56, 4238 (1997)
N Barik, S Kar and P C Dash, Phys. Rev. D57, 405 (1998)
N Barik et al, Phys. Rev. D59, 037301 (1999)
N Barik, B K Dash and A R Panda, Nucl. Phys. A605, 433 (1996)
N Barik and R N Mishra, Phys. Rev. D61, 014002 (2000)
G Parisi and R Petronzio, Phys. Lett. B62, 331 (1976)
V A Novikov, M A Shifman, A I Vainstein and V I Zakharov, JETP Lett. 24, 341 (1976); Ann.Phys. 105, 276 (1977)
M Gluck and E Reya, Nucl. Phys. B130, 76 (1977)
M Gluck, R M Godbole and E Reya, Z. Phys. C41, 667 (1989)
Callen Gross relation is satisfied in the model here, since it can be shown that W (S)00 (x, Q 2) is finite in the Bjorken limit as \(W_{00}^s = \frac{{MN_q^2 r_{0q}^2 }}{8}[(1 + \frac{1}{{\lambda _q^2 r_{0q}^2 }} + \frac{{K_ + ^2 }}{{\lambda _q^2 }} + \frac{{2K_ + }}{{\lambda _q }})e - r_{0q}^2 K_ + ^2 - (K_ + \to K\_)]\)
M R Pennington and G G Ross, Phys. Lett. B86, 371 (1979)
A J Buras, Rev. Mod. Phy. 52, 199 (1980)
Richard D Field, in Application of perturbative-QCD (Addison-Wesley, New York, 1989) p.148
M Arneodo et al, Phys. Rev. D50, R1 (1994)
P Amadruz et al, Phys. Rev. Lett. 66, 2712 (1991)
NA51 Collaboration: A Baldit et al, Phys. Lett. B332, 244 (1994)
Fermilab E866/NuSea Collaboration: E A Hawker, et al. Phys. Rev. Lett. 80, 3715 (1998)
CCFR Collaboration: A O Bazarko et al, Z Phys. C65, 189 (1995)
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Barik, N., Mishra, R. Unpolarized structure functions and the parton distributions for nucleon in an independent quark model. Pramana - J Phys 56, 519–536 (2001). https://doi.org/10.1007/s12043-001-0101-1
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DOI: https://doi.org/10.1007/s12043-001-0101-1