Results 111 to 120 of about 14,424 (194)

Quarkonium production and polarization in pp collisions with the CMS detector

open access: yesEPJ Web of Conferences, 2014
Studies of the production of heavy quarkonium states are very important to improve our understanding of QCD and hadron formation, given that the heavy quark masses allow the application of theoretical tools less sensitive to nonperturbative effects ...
Degano Alessandro
doaj   +1 more source

Two-loop O(ϵ) term of 1/(mr2) heavy quarkonium potential

open access: yesPhysics Letters B
As a straightforward application of the recently calculated two-loop heavy quarkonium Hamiltonian, we evaluate the two-loop O(ϵ) term of the 1/(mr2) heavy quarkonium potential.
Yukinari Sumino
doaj   +1 more source

Universal kinematic scaling as a probe of factorized long-distance effects in high-energy quarkonium production

open access: yesEuropean Physical Journal C: Particles and Fields, 2018
Dimensional analysis reveals general kinematic scaling rules for the momentum, mass, and energy dependence of Drell–Yan and quarkonium cross sections.
Pietro Faccioli   +3 more
doaj   +1 more source

Nucleon-Quarkonium Elastic Scattering and the Gluon Contribution to Nucleon Spin

open access: yes, 1999
It is shown that the amplitude for the scattering of a heavy quarkonium system from a nucleon near threshold is completely determined by the fraction of angular momentum, as well as linear momentum, carried by gluons in the nucleon.
A. B. Kaidalov   +11 more
core   +1 more source

Heavy Quarkonium Production and Polarization

open access: yesPhysical Review Letters, 2012
latex, 11 pages, 4 ...
Kang, Zhong-Bo   +2 more
openaire   +4 more sources

The role of multi-parton interactions in doubly-heavy hadron production. [PDF]

open access: yesEur Phys J C Part Fields, 2022
Egede U   +4 more
europepmc   +1 more source

Production of the $P$-Wave Excited $B_c$-States through the $Z^0$ Boson Decays

open access: yes, 2011
In Ref.[7],we have dealt with the production of the two color-singlet $S$-wave $(c\bar{b})$-quarkonium states $B_c(|(c\bar{b})_{\bf 1}[^1S_0]>)$ and $B^*_c(|(c\bar{b})_{\bf 1}[^3S_1]>)$ through the $Z^0$ boson decays.
A. Martin   +32 more
core   +1 more source

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