Results 141 to 150 of about 1,362 (179)
String Invention, Viable 3-3-1 Model, Dark Matter Black Holes. [PDF]
Nielsen HB.
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Short- vs. long-distance physics in B → K ( ∗ ) ℓ + ℓ - : a data-driven analysis. [PDF]
Bordone M +3 more
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Evidence of isospin-symmetry violation in high-energy collisions of atomic nuclei. [PDF]
NA61/SHINE Collaboration +4 more
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Strong couplings of scalar heavy mesons with light axial vector and pseudoscalar states in LCSR. [PDF]
Momeni S, Saghebfar M.
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QCD challenges from pp to AA collisions: 4th edition. [PDF]
Altmann J +59 more
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Physics of heavy quarks and their bound states in a quark-gluon plasma
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Reports on Progress in Physics, 1986
The author discusses the physics of the hadrons containing charmed, bottom and top quarks. The emphasis is on the most recent experimental results from the e+e- storage rings in the 3-12 GeV range of centre-of-mass energy: SPEAR at SLAC, DORIS at DESY, and the Cornell Electron Storage Ring CESR.
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The author discusses the physics of the hadrons containing charmed, bottom and top quarks. The emphasis is on the most recent experimental results from the e+e- storage rings in the 3-12 GeV range of centre-of-mass energy: SPEAR at SLAC, DORIS at DESY, and the Cornell Electron Storage Ring CESR.
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Heavy quark physics on the lattice
Nuclear Physics B - Proceedings Supplements, 2002zbMATH Open Web Interface contents unavailable due to conflicting licenses.
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Physics of heavy-quark production in quantum chromodynamics
Physical Review D, 1987For very heavy quark masses, QCD predicts that the inclusive hadronic production of heavy quarks is governed by quark and gluon hard-scattering subprocesses. On general grounds, one expects corrections of order \ensuremath{\mu}/${M}_{Q}$, where \ensuremath{\mu}\ensuremath{\sim}300 MeV and ${M}_{Q}$ is the heavy-quark mass. At the charm mass scale, such
, Brodsky, , Gunion, , Soper
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