Results 151 to 160 of about 282,852 (262)

Mass formulas and thermodynamic treatment in the mass-density-dependent model of strange quark matter [PDF]

, 1999
Guang-Xiong Peng, H.C. Chiang, J. Yang, Landong Li, B. Liu   +4 more
openalex   +1 more source

Strangeness, charm, and beauty: Mesons with one heavy quark [PDF]

, 1998
Stephen Godfrey
openalex   +1 more source

Determining the strange quark mass in Cabibbo-suppressed τ lepton decays [PDF]

, 1998
K.G. Chetyrkin, J.H. Kühn, A. A. Pivovarov   +2 more
openalex   +1 more source

On the QCD sum rule determination of the strange quark mass [PDF]

, 1997
Pietro Colangelo, Fulvia De Fazio, G. Nardulli, N. Paver   +3 more
openalex   +1 more source

Strongly interacting matter exhibits deconfined behavior in massive neutron stars. [PDF]

Nat Commun, 2023
Annala E, Gorda T, Hirvonen J, Komoltsev O, Kurkela A, Nättilä J, Vuorinen A.   +6 more
europepmc   +1 more source

Accessing directly the strange quark content of the proton at HERA [PDF]

, 1996
Lu Wei
openalex   +1 more source

In-medium bottomonium properties from lattice NRQCD calculations with extended meson operators

Journal of High Energy Physics
We calculate the temperature dependence of bottomonium correlators in (2+1)-flavor lattice QCD with the aim to constrain in-medium properties of bottomonia at high temperature.
Heng-Tong Ding, Wei-Ping Huang, Rasmus Larsen, Stefan Meinel, Swagato Mukherjee, Peter Petreczky, Zhanduo Tang   +6 more
doaj   +1 more source

Effects of final-state interaction and screening on strange- and heavy-quark production [PDF]

, 1996
Cheuk-Yin Wong, Lali Chatterjee
openalex   +1 more source

A Preliminary Direct Measurement of the Parity Violating Coupling of the Z{sup 0} to Strange Quarks, A{sub s} [PDF]

, 1999
H. Staengle
openalex   +1 more source

Sea-quark dynamics in decuplet ( $$\frac{3}{2}^+$$ 3 2 + ) $$\rightarrow $$ → octet ( $$\frac{1}{2}^+$$ 1 2 + ) transition quadrupole moment

European Physical Journal C: Particles and Fields
We investigated the electromagnetic quadrupole transition of baryon decuplet ( $$J^P= \frac{3}{2}^+$$ J P = 3 2 + ) to octet ( $$J^P= \frac{1}{2}^+$$ J P = 1 2 + ) using the statistical framework together with the principle of detailed balance.
Preeti Bhall, Alka Upadhyay
doaj   +1 more source