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Diagonal and transition magnetic moments of the negative parity, spin-1/2 heavy baryons are studied in framework of the light cone QCD sum rules. By constructing the sum rules for different Lorentz structures, the unwanted contributions…

High Energy Physics - Phenomenology · Physics 2015-09-02 T. M. Aliev , K. Azizi , T. Barakat , M. Savcı

The transition magnetic moments between negative parity, spin-1/2 heavy baryons are studied in framework of the light cone QCD sum rules. By constructing the sum rules for different Lorentz structures, the unwanted contributions coming from…

High Energy Physics - Phenomenology · Physics 2015-05-01 T. M. Aliev , T. Barakat , M. Savci

The magnetic moments of the low lying, negative parity, spin-3/2 baryons are calculated within the light cone QCD sum rules method. The contributions coming from the positive parity, spin-3/2 baryons, as well as from the positive and…

High Energy Physics - Phenomenology · Physics 2015-06-22 T. M. Aliev , M. Savci

Using the most general form of the interpolating current for the octet baryons, the magnetic moments of the negative-parity baryons are calculated within the light-cone sum rules. The contributions coming from diagonal transitions of the…

High Energy Physics - Phenomenology · Physics 2015-06-18 T. M. Aliev , M. Savci

The magnetic moment of the $\Lambda \to \Sigma^0$ transition between negative parity, baryons is calculated in framework of the QCD sum rules approach, using the general form of the interpolating currents. The pollution arising from the…

High Energy Physics - Phenomenology · Physics 2016-06-22 T. M. Aliev , M. Savcı

We calculate the mass and residue of the heavy spin--3/2 negative parity baryons with single heavy bottom or charm quark by the help of a two-point correlation function. We use the obtained results to investigate the diagonal radiative…

High Energy Physics - Phenomenology · Physics 2016-12-19 K. Azizi , H. Sundu

Magnetic moments of $S_{11}(1535)$ and $S_{11}(1650)$ baryons are studied in the framework of the relativistic three-quark Hamiltonian derived in the Field Correlation Method. The baryon magnetic moments are expressed via the average…

High Energy Physics - Phenomenology · Physics 2015-06-17 I. M. Narodetskii , M. A. Trusov

Magnetic dipole moments of the negative parity light and heavy tensor mesons are calculated within the light cone QCD sum rules method. The results are compared with the positive parity counterparts of the corresponding tensor mesons. The…

High Energy Physics - Phenomenology · Physics 2016-12-30 T. M. Aliev , T. Barakat , M. Savcı

We report preliminary results for the magnetic moments of negative-parity baryons extracted from mass shifts in the presence of static external magnetic fields. The calculations are done on $24^3\times 48$ quenched lattices using standard…

High Energy Physics - Lattice · Physics 2011-07-08 Frank X. Lee , Andrei Alexandru

The magnetic moments of ground state single, double and triple heavy baryons containing charm or bottom quarks are calculated in a relativistic three-quark model, which, in the heavy quark limit, is consistent with Heavy Quark Effective…

High Energy Physics - Phenomenology · Physics 2008-11-26 Amand Faessler , Th. Gutsche , M. A. Ivanov , J. G. Korner , V. E. Lyubovitskij , D. Nicmorus , K. Pumsa-ard

Magnetic moments of the positive parity 70-plet baryons are estimated within the non relativistic quark model and QCD sum rules method. It is found that the magnetic moments of the 70-plet baryons can be expressed in terms of the D and F…

High Energy Physics - Phenomenology · Physics 2015-06-26 T. M. Aliev , V. S. Zamiralov

The magnetic moments of heavy sextet $J^P = {1\over 2}^+$ baryons are calculated in framework of the light cone QCD sum rules method. Linearly independent relations among the magnetic moments of these baryons are obtained. The results for…

High Energy Physics - Phenomenology · Physics 2015-02-24 T. M. Aliev , T. Barakat , M. Savci

The magnetic moments of heavy $\Xi_{Q}$ baryons containing a single charm or bottom quark are calculated in the framework of light cone QCD sum rules method. A comparison of our results with the predictions of the quark models is presented.

High Energy Physics - Phenomenology · Physics 2008-11-26 T. M. Aliev , K. Azizi , A. Ozpineci

Using the most general form of the interpolating currents of heavy baryons, the magnetic moments of heavy baryons "Lambda_Q (Q=b,c)" are calculated in framework of the light cone QCD sum rules. A comparison of our results on magnetic…

High Energy Physics - Phenomenology · Physics 2009-11-07 T. M. aliev , A. Ozpineci , M. Savci

In this study, the magnetic moments of the spin-1/2 triply-heavy baryons have been calculated using both light-cone QCD sum rules and Quark-diquark model. Theoretical investigations on magnetic moments of the triply-heavy baryons, are…

High Energy Physics - Phenomenology · Physics 2022-04-27 Halil Mutuk , Ulaş Özdem

We calculate the magnetic moments of decuplet baryons containing strange quarks within the framework of light cone QCD sum rules taking into account the SU(3) flavor symmetry breaking effects. It is obtained that magnetic moments of the…

High Energy Physics - Phenomenology · Physics 2009-10-31 T. M. Aliev , A. Ozpineci

Magnetic moments of baryons composed of light and strange quarks are computed for the first time through the only parameter of the model -- string tension $\sigma$. Resulting theoretical values differ from the experimental ones typically by…

High Energy Physics - Phenomenology · Physics 2016-09-06 B. O. Kerbikov , Yu. A. Simonov

Light cone QCD sum rules for the electromagnetic transition form factors among positive and negative parity octet baryons are derived. The unwanted contributions of the diagonal transitions among positive parity octet baryons are eliminated…

High Energy Physics - Phenomenology · Physics 2015-06-18 T. M. Aliev , M. Savci

A light baryon is viewed as $N_c$ valence quarks bound by meson mean fields in the large $N_c$ limit. In much the same way a singly heavy baryon is regarded as $N_c-1$ valence quarks bound by the same mean fields, which makes it possible to…

High Energy Physics - Phenomenology · Physics 2018-05-23 Ghil-Seok Yang , Hyun-Chul Kim

The baryon magnetic and transition magnetic moments are computed in heavy baryon chiral perturbation theory in the large-N_c limit, where N_c is the number of colors. One-loop nonanalytic corrections of orders m_q^{1/2} and m_q ln m_q are…

High Energy Physics - Phenomenology · Physics 2010-01-18 Ruben Flores-Mendieta
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