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

. 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 ... . Aliev , K. Azizi , M. Savci , Eur. Phys. J. A 47 , 125 ( 2011 ) 34. T.M. Aliev , K. Azizi , M. Savci , Phys. Lett . B 690 , 164 ( 2010 ) 35. S.S. Agaev , K. Azizi , H. Sundu , arXiv: 1703 .07091v2 [hep-ph

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

The ground and first excited states of the decuplet baryons are studied using the two-point QCD sum rule approach. The mass and residue of these states are computed and compared with the existing experimental data and other theoretical predictions. The results for the masses of the ground state particles as well as the excited \( \Delta \) and \( \Sigma ^{*} \) states are in good ...

\( B_c B_c J/\psi \) vertex form factor at finite temperature in the framework of QCD sum rules approach

. Phys. J. A 51, 28 (2015) 6. E. Yazici, E. Veli Veliev, K. Azizi, H. Sundu, Eur. Phys. J. Plus 128, 113 (2013) 7. A. Abbasi, V. Bashiry, Eur. Phys. J. A 49, 103 (2013) 8. Z.G. Wang, Phys. Rev. D 89 ... . Rev. Lett . 82 , 3396 ( 1999 ) 23. K. Morita , S.H. Lee , Phys. Rev. C 77 , 064904 ( 2008 ) 24. K. Morita , S.H. Lee , Phys. Rev. D 82 , 054008 ( 2010 ) 25. E.V. Veliev , H. Sundu , K. Azizi , M. Bayar

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

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 ...