S-Wave Single Heavy Baryons with Spin-3/2 at Finite Temperature
arXiv:1910.11538 · doi:10.1140/epjc/s10052-020-7931-9
Abstract
The thermal behavior of the spectroscopic parameters of the S-wave single heavy baryons and with spin-3/2 are investigated in QCD at finite temperature. We analyze the variations of the mass and residue of these baryons taking into consideration the contributions of QCD thermal condensates up to dimension eight in Wilson expansion. At finite temperature, due to the breakdown of the Lorentz invariance by the choice of reference frame and presence of an extra symmetry, some new four-dimensional operators come out in the form of the fermionic and gluonic parts of the energy momentum tensor that are taken into account in the calculations. Our analyses show that at lower temperatures, the parameters of baryons under consideration are not affected by the medium. These parameters, however, show rapid variations with respect to temperature at higher temperatures near to a pseudo-critical temperature, after which the baryons are melted. The results of the masses and residues at limit are compatible with the available experimental data and predictions of other theoretical studies.
arXiv comment14 Pages, 4 Figures and 3 Tables
References in corpus (46)
- The order of the quantum chromodynamics transition predicted by the standard model of particle physics
- The equation of state in (2+1)-flavor QCD
- Full result for the QCD equation of state with 2+1 flavors
- Heavy Baryons in a Quark Model
- The QCD Equation of State to from Lattice QCD
- QCD at Low Energies
- The QCD phase transition with physical-mass, chiral quarks
- Spectroscopy and Regge trajectories of heavy baryons in the relativistic quark-diquark picture
- The transition temperature in QCD
- Static quark anti-quark free energy and the running coupling at finite temperature
- Towards an understanding of heavy baryon spectroscopy
- PREDICTING THE MASSES OF BARYONS CONTAINING ONE OR TWO HEAVY QUARKS
- Faddeev study of heavy baryon spectroscopy
- Charmed and Bottom Baryons from Lattice NRQCD
- Masses of heavy baryons in the relativistic quark model
- The Quark Model and Baryons
- Heavy Baryon Masses in the and Expansions
- Bottom Baryons
- Recent Progress in QCD Condensate Evaluations and Sum Rules
- Measurement of hadron masses in exclusive decays with the CDF detector
- Analysis of the heavy and doubly heavy baryon states with QCD sum rules
- Heavy baryon spectroscopy in QCD
- Baryonic currents and their correlators in the Heavy Quark Effective Theory
- Critical behavior of charmonia across the phase transition: A QCD sum rule approach
- Bottom baryons from a dynamical lattice QCD simulation
- QCD Sum Rules for Heavy Baryons at Next-to-Leading Order in alpha_s
- 1/m Corrections to Heavy Baryon Masses in the Heavy Quark Effective Theory Sum Rules
- Predicting the Masses of Heavy Hadrons without an Explicit Hamiltonian
- Charmed Baryon Masses in Chiral Perturbation Theory
- Operator product expansion at finite temperature
- Analysis of and with QCD sum rules
- Mass and Magnetic Moments of the Heavy Flavored Baryons with in Light Cone QCD Sum Rules
- Mass spectra of the heavy baryons Lambda_Q and Sigma_Q^(*) from QCD sum rules
- Improved analysis for the baryon masses to order Lambda_{QCD}/m_Q from QCD sum rules
- Mass spectra of singly heavy baryons in a self-consistent chiral quark-soliton model
- Flavor dependence of baryon melting temperature in effective models of QCD
- Electric Quadrupole and Magnetic Octupole Moments of the Light Decuplet Baryons Within Light Cone QCD Sum Rules
- Choice of heavy baryon currents in QCD sum rules
- Decuplet baryons in a hot medium
- S-wave bottom baryons
- Heavy baryon properties with NLO accuracy in perturbative QCD
- Properties of , and heavy baryons in cold nuclear matter
- Chiral perturbation theory analysis of baryon temperature mass shifts
- The temperature dependence of the decuplet baryon masses from thermal QCD sum rules
- Thermal behavior of the mass and residue of hyperons
- Strong Coupling Constants of Decuplet Baryons with Vector Mesons