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Production of exotic tetraquarks QQ(q)over-bar (q)over-bar in heavy-ion collisions at the LHC
(Amer Physical Soc, 2019-05-28)
We investigate the production of exotic tetraquarks, QQ (q) over bar (q) over bar T-QQ (Q = c or b and q = u or d), in relativistic heavy-ion collisions using the quark coalescence model. The T-QQ yield is given by the ...
Description of Heavy Quark Mass by Lippmann-Schwinger Equation
(Springer/plenum Publishers, 2012-09-01)
Quark masses are of great prominence in high-energy physics. In this paper, we have studied the heavy meson systems via solving the Lippmann-Schwinger equation by using the Martin potential for heavy quark masses. We have ...
Description of Heavy Quark Mass by Lippmann-Schwinger Equation
(Springer/plenum Publishers, 2012-09-01)
Quark masses are of great prominence in high-energy physics. In this paper, we have studied the heavy meson systems via solving the Lippmann-Schwinger equation by using the Martin potential for heavy quark masses. We have ...
Description of Heavy Quark Mass by Lippmann-Schwinger Equation
(Springer/plenum Publishers, 2013)
Bmc: a modulating bar for copper electrowinning designed for heavy duty and high reliability
(IEE-INST ELEC ENG, 2014)
Production of doubly heavy baryons via Higgs boson decays
(Springer, 2019-04-15)
We systematically analyzed the production of semi-inclusive doubly heavy baryons (Xi(cc), Xi(bc) and Xi(bb)) for the process H-0 -> Xi(QQ') + (Q) over bar' + (Q) over bar through four main Higgs decay channels within the ...
Production of semi-inclusive doubly heavy baryons via top-quark decays
(Amer Physical Soc, 2018-11-26)
In the paper, we present a detailed discussion on the semi-inclusive production of doubly heavy baryons (Xi(bc) and Xi(bb)) through top-quark decay channel, t -> Xi(bQ ') + (Q ') over bar + W+, within the framework of ...
D(s)D* Molecule as an Axial Meson
(KOREAN PHYSICAL SOC, 2009)
We use QCD sum rules to study the possible existence of a D(s)(D) over bar* - D(s)*(D) over bar molecule with the quantum number J(PC) = 1(++). We consider the contributions of condensates up to dimension eight and work ...