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Interpretation of the new \(\Omega _c^{0}\) states via their mass and width

94 , 114016 ( 2016 ) 23. Z. Shah , K. Thakkar , A.K. Rai , P.C. Vinodkumar , Chin. Phys . C 40 , 123102 ( 2016 ) 24. T.M. Aliev , K. Azizi , T. Barakat , M. Savci , Phys. Rev. D 92 , 036004 ( 2015 ) 25 ... . K. Azizi , H. Sundu , Eur. Phys. J. Plus 132 , 22 ( 2017 ) 26. S.L. Zhu , W.Y.P. Hwang , Z.S. Yang , Phys. Rev. D 56 , 7273 ( 1997 ) 27. T.M. Aliev , K. Azizi , A. Ozpineci , Nucl. Phys . B 808 , 137

Open charm-bottom axial-vector tetraquarks and their properties

( 2012 ) 36. S.S. Agaev , K. Azizi , H. Sundu , Phys. Rev. D 95 , 034008 ( 2017 ) 37. M.A. Shifman , A.I. Vainshtein , V.I. Zhakharov , Nucl. Phys . B 147 , 385 ( 1979 ) 38. V.M. Braun , A.V. Kolesnichenko ... , 109 ( 1984 ) 46. V.M. Belyaev , V.M. Braun , A. Khodjamirian , R. Rückl , Phys. Rev. D 51 , 6177 ( 1995 ) 47. S.S. Agaev , K. Azizi , H. Sundu , Phys. Rev. D 93 , 074002 ( 2016 ) 48. S.S. Agaev , K

Radial excitations of the decuplet baryons

. arXiv:0907 . 1901 [nucl-th] 10. K. Azizi , G. Bozk?r , Decuplet baryons in a hot medium . Eur. Phys. J. C 76(10) , 521 ( 2016 ). arXiv: 1606 .05452 [hep-ph] 11. V.M. Belyaev , B.L. Ioffe , Determination

Decuplet baryons in a hot medium

qcd sum rules . Phys. Rev. D 57 , 1801 ( 1998 ). arXiv:hep-ph/9708323 13. K. Azizi , A. Türkan , E. Veli Veliev , H. Sundu , Thermal properties of light tensor mesons via QCD sum rules . Adv. High

Semileptonic \(B_{s} \rightarrow D_{s2}^{*}(2573)\ell \bar{\nu }_{\ell }\) transition in QCD

, 385 ( 1979 ) 23. K. Azizi , H. Sundu , S. Sahin , Investigation of the semileptonic transition of the B into the orbitally excited charmed tensor meson . Phys. Rev. D 88 , 03600 ( 2013 ). arXiv: 1306 ... .4098 [hep-ph] 24. K. Azizi , H. Sundu , J.Y. Sungu , N. Yinelek , Properties of Ds2(2573) charmed-strange tensor meson . Phys. Rev. D 88 , 036005 ( 2013 ) 25. K. Azizi , H. Sundu , J. Y. Sungu , N

Properties of nucleon in nuclear matter: once more

We calculate the mass and residue of the nucleon in nuclear matter in the frame work of QCD sum rules using the nucleon’s interpolating current with an arbitrary mixing parameter. We evaluate the effects of the nuclear medium on these quantities and compare the results obtained with the existing theoretical predictions. The results are also compared with those obtained in vacuum to ...

Radiative \(\Omega _{Q}^{*}\rightarrow \Omega _{Q}\gamma \) and \(\Xi _{Q}^{*}\rightarrow \Xi ^{\prime }_{Q}\gamma \) transitions in light cone QCD

We calculate the magnetic dipole and electric quadrupole moments associated with the radiative \(\Omega _{Q}^{*}\rightarrow \Omega _{Q}\gamma \) and \(\Xi _{Q}^{*}\rightarrow \Xi ^{\prime }_{Q}\gamma \) transitions with \(Q=b\) or \(c\) in the framework of light cone QCD sum rules. It is found that the corresponding quadrupole moments are negligibly small, while the magnetic dipole ...

Analysis of the strong \(D_{2}^{*}(2460)^{0}\rightarrow D^+\pi ^- \) and \(D_{s2}^{*}(2573)^{+}\rightarrow D^{+} K^{0}\) transitions via QCD sum rules

The strong \(D_{2}^{*}(2460)^{0}\rightarrow D^+ \pi ^- \) and \(D_{s2}^{*}(2573)^{+}\rightarrow D^{+} K^{0}\) transitions are analyzed via three-point QCD sum rules. First we calculate the corresponding strong coupling constants \(g_{D_2^*D\pi }\) and \(g_{D_{s2}^*DK}\). Then we use them to calculate the corresponding decay widths and branching ratios. Making use of the existing ...

More about the \(B\) and \(D\) mesons in nuclear matter

We calculate the shifts in decay constants of the pseudoscalar \(B\) and \(D\) mesons in nuclear medium in the frame work of QCD sum rules. We write those shifts in terms of the \(B\)–\(N\) and \(D\)–\(N\) scattering lengths and an extra phenomenological parameter entered to calculations. Computing an appreciate forward scattering correlation function, we derive the QCD sum rules ...