2020
DOI: 10.1103/physrevd.101.056002
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Bc meson spectrum via Dyson-Schwinger equation and Bethe-Salpeter equation approach

Abstract: We predict the masses of the lowlying Bc mesons with J P = 0 − , 1 − , 0 + , 1 + , 2 + , using a flavor dependent interaction pattern which gives an unified successful description of the light, heavy-light and heavy mesons and is also appliable to the radial excited heavy mesons. The errors are controlled carefully. With the errors from the RL approximation subduced, our predictions are consistent with the lQCD and quark model results, which supports strongly that the flavor dependent interaction pattern is re… Show more

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Cited by 29 publications
(17 citation statements)
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“…Let us now consider the BS equation in the MRL truncation, Eq. (12). Supplemented by the effective gluon in the CI model, Eq.…”
Section: B Contact Interaction In Modified Rlmentioning
confidence: 99%
See 1 more Smart Citation
“…Let us now consider the BS equation in the MRL truncation, Eq. (12). Supplemented by the effective gluon in the CI model, Eq.…”
Section: B Contact Interaction In Modified Rlmentioning
confidence: 99%
“…The derivation of QCD's DSEs do not require any assumptions on the running coupling, therefore, both perturbative and nonperturbative facets of the strong interactions can be addressed within this formalism. At the same time, the DSE approach is not restricted to a certain domain of current quark masses [9][10][11][12]. Moreover, hadron observables can be traced down to fundamental pieces, namely propagators and vertices, hence maintaining a clear connection to QCD's fundamental degrees of freedom, quarks and gluons [13][14][15][16].…”
Section: Introductionmentioning
confidence: 99%
“…The thresholds for the charmonium and bottomunium systems are approximately 3.71 and 10.50 GeV, respectively [2]. Many charmonium and bottomonium states below thresholds have been experimentally observed and theoretically studied through various relativistic and non-relativistic potential models [3][4][5][6][7][8][9][10][11][12][13][14][15][16][17][18][19] and approaches like chiral perturbation theory [20], heavy quark effective field theory, lattice QCD [21][22][23][24][25][26][27][28][29][30][31], QCD sum rules [32][33][34][35][36][37][38], NRQCD [39][40][41], and dynamical equations based approaches like Bethe Salpeter and Dyson-Schwinger equations [41][42][43][44]. The heavy quarkonia were observed so far, still have many puzzles [17].…”
Section: Introductionmentioning
confidence: 99%
“…The derivation of QCD's DSEs do not require any assumptions on the running coupling, therefore, both perturbative and non-perturbative facets of the strong interactions can be addressed within this formalism. At the same time, the DSE approach is not restricted to a certain domain of current quark masses [9][10][11][12]. Moreover, hadron observables can be traced down to fundamental pieces, namely propagators and vertices, hence maintaining a clear connection to QCD's fundamental degrees of freedom, quarks and gluons [13][14][15][16].…”
Section: Introductionmentioning
confidence: 99%