By T. Gherghetta
This publication includes articles at the most recent learn in QCD from a few of the prime specialists within the box. those are in response to talks offered on the non-stop Advances in QCD 2004 workshop held on the William I wonderful Theoretical Physics Institute. The ebook might be an invaluable reference resource for graduate scholars and researchers in excessive strength physics.
Read Online or Download Continuous Advances In QCD 2004: Proceedings Of The Conference, William I. Fine Theoretical Physics Institute, Minneapolis, USA, 13 A» 16 May 2004 PDF
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Additional resources for Continuous Advances In QCD 2004: Proceedings Of The Conference, William I. Fine Theoretical Physics Institute, Minneapolis, USA, 13 A» 16 May 2004
Here ~ R ( s ) / Tand - a g 1 ( Q 2 ) ) / nrepresent the entire radiative corrections to Re+,- (s) and the Bjorken sum rule for the gI(x, Q 2 ) structure function measured in spin-dependent deep inelastic scattering, respectively. The relation between s* and Q2 can be computed order by order in perturbation theory, as in the BLM method 15. The ratio of physical scales guarantees that the effect of new quark thresholds is commensurate. Commensurate scale relations are renormalization-scheme independent and satisfy the group properties of the renormalization group.
S. J. Brodsky, J. R. Hiller, D. S. Hwang and V. A. Karmanov, Phys. Rev. D 69, 076001 (2004) [arXiv:hep-ph/0311218]. 53. V. A. V. Smirnov, Nucl. Phys. A 546, 691 (1992). 54. J . M. Maldacena, Adv. Theor. Math. Phys. 2, 231 (1998) [Int. J. Theor. Phys. 38, 1113 (1999)l [arXiv:hep-th/9711200]. 55. J. Polchinski and M. J. Strassler, Phys. Rev. Lett. 88, 031601 (2002) [arXiv:hep- th/O 1091741. 56. R. C. Brower and C. I. Tan, Nucl. Phys. B 662, 393 (2003) [arXiv:hepth/0207144]. 57. 0. Andreev, Phys. Rev.
X can be obtained by integrating the Bethe-Salpeter solutions over the corresponding relative light-front energies. The resulting LFWFs $:(xi, k l i ) are functions of the light-cone momentum fractions xi = ki . w / p ’ w and the invariant mass squared of the constituents M: = (CZ,k f ) 2 = Cy=l and the light-cone momentum fractions xi = k . w / p w each multiplying spinvector and polarization tensor invariants which can involve wp. The resulting LFWFs for bound states are eigenstates of the Karmanov-Smirnov kinematic angular momentum operator 53 and satisfy all of the Lorentz symmetries of the front form, including boost invariance.