10.9k citations
Counting papers with at most 25 authors, so collaboration author lists do not stand in for the people here.
- Charles UniversityCZ2k papers
- European Organization for Nuclear ResearchCH2k papers
- Boğaziçi UniversityTR2k papers
- National and Kapodistrian University of AthensGR2k papers
- Universidad Autónoma de MadridES2k papers
- University of BelgradeRS2k papers
- Rutherford Appleton LaboratoryGB2k papers
- The Ohio State UniversityUS2k papers
- Centre National de la Recherche ScientifiqueFR1.9k papers
- University of IowaUS1.9k papers
- Institut National de Physique Nucléaire et de Physique des ParticulesFR1.9k papers
- Commissariat à l'Énergie Atomique et aux Énergies AlternativesFR1.9k papers
4 papers · 2 filters
The Spin Structure of the qq Interaction and the Mass Spectra of Bound q\bar q Systems: Different Versions of the 3-Dimensional Reductions of the Bethe-Salpeter Equation
T. Babutsidze, T. Kopaleishvili, A. Rusetsky
Bound q\bar q -systems are considered in the framework of three different versions of the 3-dimensional reduction of the Bethe-Salpeter equation, all having the correct one-body li…
Exclusive Nonleptonic Decays of Bottom and Charm Baryons in a Relativistic Three-Quark Model: Evaluation of Nonfactorizing Diagrams
M. A. Ivanov, J. G. Korner, V. E. Lyubovitskij +1
Exclusive nonleptonic decays of bottom and charm baryons are studied within a relativistic three-quark model with a Gaussian shape for the momentum dependence of the baryon-three-q…
Exclusive nonleptonic bottom to charm baryon decays including nonfactorizable contributions
M. A. Ivanov, J. G. Korner, V. E. Lyubovitskij +1
Exclusive nonleptonic decays of bottom baryons to charm baryons and pseudoscalar light mesons are analyzed within a relativistic three-quark model. We include factorizing as well a…
Towards the Light Front Variables for High Energy Production Processes
N. S. Amaglobeli, S. M. Esakia, V. R. Garsevanishvili +5
Scale invariant presentation of inclusive spectra in terms of light front variables is proposed. The variables introduced go over to the well-known scaling variables x_F = 2p_z/sqr…