scholarly journals SU(3)-symmetry breaking effects and mass splitting in scalar and pseudoscalarDmesons from QCD sum rules

2010 ◽  
Vol 81 (5) ◽  
Author(s):  
Hong-Ying Jin ◽  
Jin Zhang ◽  
Zhu-Feng Zhang ◽  
T. G. Steele
Keyword(s):  
Symmetry Breaking ◽  
Sum Rules ◽  
Mass Splitting ◽  
Qcd Sum Rules

scholarly journals More about the Mass of the New Charmonium States

2015 ◽  
Vol 2015 ◽  
pp. 1-7 ◽  
Author(s):  
T. M. Aliev ◽  
H. Özşahin ◽  
M. Savcı
Keyword(s):  
Sum Rules ◽  
Critical Role ◽  
Mass Splitting ◽  
Qcd Sum Rules ◽  
Experimental Search ◽  
New States ◽  
Charmonium States

IfX(3872)is described by the picture as a mixture of the charmonium and molecularD*Dstates;Y(3940)as a mixture of theχc0andD*D*states; andY(4260)as a mixture of the tetraquark and charmonium states, their orthogonal combinations should also exist. We estimate the mass and residues of the states within the QCD sum rules method. We find that the mass splitting amongX, Yand their orthogonal states is at most 200 MeV. Experimental search of these new states can play critical role for establishing the nature of the new charmonium states.

scholarly journals SU(2) symmetry breaking from QCD sum rules

1984 ◽  
Vol 135 (5-6) ◽  
pp. 463-467 ◽  
Author(s):  
E. Bagan ◽  
A. Bramon ◽  
S. Narison ◽  
N. Paver
Keyword(s):  
Symmetry Breaking ◽  
Sum Rules ◽  
Qcd Sum Rules

scholarly journals Mass splitting of heavy-baryons from QCD sum rules

2010 ◽  
Vol 3 ◽  
pp. 07011
Author(s):  
R.M. Albuquerque ◽  
S. Narison ◽  
M. Nielsen
Keyword(s):  
Sum Rules ◽  
Mass Splitting ◽  
Qcd Sum Rules ◽  
Heavy Baryons

scholarly journals QCD SUM RULES: INTERCROSSED RELATIONS FOR THE Σ0–Λ MASS SPLITTING

2005 ◽  
Vol 20 (04) ◽  
pp. 243-249 ◽  
Author(s):  
A. ÖZPINECI ◽  
S. B. YAKOVLEV ◽  
V. S. ZAMIRALOV
Keyword(s):  
Sum Rules ◽  
Mass Splitting ◽  
Qcd Sum Rules ◽  
Sum Rule

New relations between QCD Borel sum rules for masses of Σ0 and Λ hyperons are constructed. It is shown that starting from the sum rule for the Σ0 hyperon mass it is straightforward to obtain the corresponding sum rule for the Λ hyperon mass and vice versa.

CHIRAL SYMMETRY BREAKING AND THE GLUON CONDENSATE

1993 ◽  
Vol 08 (04) ◽  
pp. 335-339
Author(s):  
M. FABER ◽  
A.N. IVANOV ◽  
M. NAGY ◽  
N.I. TROITSKAYA
Keyword(s):  
Magnetic Field ◽  
Symmetry Breaking ◽  
Chiral Symmetry ◽  
Sum Rules ◽  
Chiral Symmetry Breaking ◽  
Gluon Condensate ◽  
Quark Condensate ◽  
Low Energy ◽  
Qcd Sum Rules ◽  
Energy Approximation

For the low-energy approximation of QCD, the extended Nambu-Jona-Lasinio model has been used. Quarks interact with an external homogeneous color-magnetic field, simulating the contribution of the gluon condensate. The value of the gluon condensate, needed to reach the correct value of the quark condensate, is determined and agrees well with the value obtained from QCD sum rules.

scholarly journals Identifying the Λb(6146)0 and Λb(6152)0 as D-Wave Bottom Baryons

Universe ◽  
2020 ◽  
Vol 6 (6) ◽  
pp. 86
Author(s):  
Qiang Mao ◽  
Hua-Xing Chen ◽  
Hui-Min Yang
Keyword(s):  
Quantum Chromodynamics ◽  
Heavy Quark ◽  
Light Cone ◽  
Sum Rules ◽  
Mass Splitting ◽  
Effective Theory ◽  
Heavy Quark Effective Theory ◽  
Qcd Sum Rules ◽  
Decay Properties ◽  
D Wave

We study the Λ b ( 6146 ) 0 and Λ b ( 6152 ) 0 recently observed by LHCb using the method of Quantum Chromodynamics (QCD) sum rules within the framework of heavy quark effective theory. Our results suggest that they can be interpreted as D-wave bottom baryons of J P = 3 / 2 + and 5 / 2 + respectively, both of which contain two λ -mode excitations. We also investigate other possible assignments containing ρ -mode excitations. We extract all the parameters that are necessary to study their decay properties when using the method of light-cone sum rules. We predict masses of their strangeness partners to be m Ξ b ( 3 / 2 + ) = 6.26 − 0.14 + 0.11 GeV and m Ξ b ( 5 / 2 + ) = 6.26 − 0.14 + 0.11 GeV with the mass splitting Δ M = m Ξ b ( 5 / 2 + ) − m Ξ b ( 3 / 2 + ) = 4.5 − 1.5 + 1.9 MeV, and propose to search for them in future CMS, EIC, and LHCb experiments.

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