نتایج جستجو برای: who questionnaire

تعداد نتایج: 943089  

2017
T. Affolder Kenneth A. Bloom H. Akimoto A. Akopian M. G. Albrow P. Amaral D. Amidei K. Anikeev J. Antos G. Apollinari T. Arisawa T. Asakawa W. Ashmanskas F. Azfar P. Azzi-Bacchetta N. Bacchetta M. W. Bailey S. Bailey P. de Barbaro A. Barbaro-Galtieri V. E. Barnes B. A. Barnett S. Baroiant M. Barone G. Bauer F. Bedeschi S. Belforte W. H. Bell G. Bellettini J. Bellinger D. Benjamin J. Bensinger A. Beretvas J. P. Berge J. Berryhill B. Bevensee A. Bhatti M. Binkley D. Bisello M. Bishai R. E. Blair C. Blocker K. Bloom B. Blumenfeld S. R. Blusk A. Bocci A. Bodek W. Bokhari G. Bolla Y. Bonushkin D. Bortoletto K. L. Byrum P. Calafiura A. Cerri A. W. Chan P. S. Chang P. T. Chang M. L. Chu Y. S. Chung C. I. Ciobanu A. G. Clark

2008
Sh Mamedov

The motion of quark is studied in a confining bag having central color field. The Dirac equation is solved for a quark in such bag and its energy spectrum is found. It is pointed out the possibility to identify the external color field with the background field of gluon condensation. This makes the received energy spectrum of quark useful for comparison with the energy spectrum of hadrons.

1993
MAKOTO OKA

A realistic hyperon (Y )-nucleon (N) interaction based on the quark model and the oneboson-exchange potential is constructed. The Nijmegen potential model D with the SU(3) flavor symmetry is modified with a quark exchange interaction at the short-distance, which replaces the short-range repulsive core in the original model. The flavor-spin dependences of the short-range repulsion are qualitativ...

2008
Néstor Armesto Carlos Pajares

We study the modification of the multiplicity distributions in MLLA due to the presence of a QCD medium. The medium is introduced though a multiplicative constant (fmed) in the soft infrared parts of the kernels of QCD evolution equations. Using the asymptotic ansatz for quark and gluons mean multiplicities 〈nG〉 = e γy and 〈nQ〉 = r e respectively, we study two cases: fixed γ as previously consi...

2000
S. W. Hong B. K. Jennings

We considered the quark-meson coupling model for a nucleon. The model describes a nucleon as an MIT bag, in which quarks are coupled to the scalar and the vector mesons. A set of coupled equations for the quark and the meson fields are obtained and are solved in a self-consistent manner. We show that the mass of a dressed MIT bag interacting with σand ω-meson fields differs considerably from th...

2010
B. U. Musch J. W. Negele A. Schäfer

We study transverse momentum dependent parton distribution functions (TMDs) with non-local operators in lattice QCD, using MILC/LHPC lattices. We discuss the basic concepts of the method, including renormalization of the gauge link. Results obtained with a simplified operator geometry show visible dipole deformations of spin-dependent quark momentum densities.

2001
V. S. Fadin R. Fiore

The method of calculation of effective vertices of interaction of the Reggeized gluon and quark with particles in QCD in the next-to-leading order is developed. The method is demonstrated in the case of already known vertices of both gluon-gluon and quark-quark transitions in the scattering of gluons and quarks on the Reggeized gluon. It is used for the calculation of the gluon-quark transition...

2008
Nobuhito Maru Motoi Tachibana

In this talk, a supersymmetric (SUSY) composite model of color superconductivity is discussed. In this model, quark and diquark supermultiplets are dynamically generated as massless composites by a newly introduced confining gauge dynamics. It is analytically shown that the scalar component of diquark supermultiplets develops vacuum expectation value (VEV) at a certain critical chemical potenti...

1993
V. Barger J. Ohnemus R. J. N. Phillips

Single-lepton plus jets signals from t ¯ t production at hadron colliders generally give more spherically symmetrical events than the principal backgrounds from W production. We show that sphericity and aplanarity criteria, applied to lepton plus neutrino plus four jet final states at the Fermilab Tevatron p¯ p collider, help to discriminate; they can be used either to validate an eventual top ...

1997
Henning Genz

Partial conservation of the nine axial currents Aμ for β = 0, 1, ..., 8 applied to the vacuum expectation values of the equal-time commutators of the nine axial charges QA(x0) for α = 0, 1, ..., 8 with the corresponding axial current divergences ∂Aμ implies that the non-vanishing current quark masses mu, md, ms of the light quarks u, d, s have the same sign. Under the more realistic assumption ...

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