Results 111 to 120 of about 14,424 (194)
Quarkonium production and polarization in pp collisions with the CMS detector
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
Machine Learning Approach to Analyze the Heavy Quark Diffusion Coefficient in Relativistic Heavy Ion Collisions. [PDF]
Guo R, Li Y, Chen B.
europepmc +1 more source
Two-loop O(ϵ) term of 1/(mr2) heavy quarkonium potential
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
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
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
Overview of the QCD phase diagram: Recent progress from the lattice. [PDF]
Guenther JN.
europepmc +1 more source
Heavy Quarkonium Production and Polarization
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]
Egede U +4 more
europepmc +1 more source
The exotic behavior of the wave evolution in Lévy crystals within a fractional medium. [PDF]
Zakeri Z +3 more
europepmc +1 more source
Production of the $P$-Wave Excited $B_c$-States through the $Z^0$ Boson Decays
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

