Electromagnetic properties of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" altimg="si1.svg"><mml:msup><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>D</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy="false">¯</mml:mo></mml:mrow></mml:mover></mml:mrow><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mo>⁎</mml:mo><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:msup><mml:msubsup><mml:mrow><mml:mi mathvariant="normal">Ξ</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><m

Özdem, Ulaş

doi:10.1016/j.physletb.2023.138267

Physics Letters B

2023

DOI: 10.1016/j.physletb.2023.138267

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Electromagnetic properties of D¯(⁎)Ξc

Ulaş Özdem

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2024

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Cited by 10 publications

(1 citation statement)

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“…The literature contains few studies investigating the electromagnetic form factors of pentaquark states with hidden-charm, despite the valuable information they provide. The electromagnetic features of the pentaquark state with hidden-charm were theoretically investigated in various configurations and models [22][23][24][25][26][27][28][29][30][31][32][33][34][35][36][37][38]. In the future, the discovery of many new pentaquarks is not far off with the continuous advancement of experimental techniques.…”

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confidence: 99%

Magnetic dipole moments of the hidden-charm pentaquark states: $$P_c(4440)$$, $$P_c(4457)$$ and $$P_{cs}(4459)$$

Özdem

2021

Eur. Phys. J. C

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In this work, we employ the light-cone QCD sum rule to calculate the magnetic dipole moments of the $$P_c(4440)$$ P c ( 4440 ) , $$P_c(4457)$$ P c ( 4457 ) and $$P_{cs}(4459)$$ P cs ( 4459 ) pentaquark states by considering them as the diquark–diquark–antiquark and molecular pictures with quantum numbers $$J^P = \frac{3}{2}^-$$ J P = 3 2 - , $$J^P = \frac{1}{2}^-$$ J P = 1 2 - and $$J^P = \frac{1}{2}^-$$ J P = 1 2 - , respectively. In the analyses, we use the diquark–diquark–antiquark and molecular form of interpolating currents, and photon distribution amplitudes to obtain the magnetic dipole moment of pentaquark states. Theoretical examinations on magnetic dipole moments of the hidden-charm pentaquark states, are essential as their results can help us better figure out their substructure and the dynamics of the QCD as the theory of the strong interaction. As a by product, we extract the electric quadrupole and magnetic octupole moments of the $$P_c(4440)$$ P c ( 4440 ) pentaquark. These values show a non-spherical charge distribution.

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Magnetic dipole moments of the hidden-charm pentaquark states: $$P_c(4440)$$, $$P_c(4457)$$ and $$P_{cs}(4459)$$

Özdem

2021

Eur. Phys. J. C

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Magnetic dipole moments of the Ω (3185)0 and Ω (3327)0 states from molecular perspective

Özdem

2024

Physics Letters B

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Elucidating the nature of hidden-charm pentaquark states with spin-32 through their electromagnetic form factors

Özdem

2024

Physics Letters B

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Electromagnetic properties of D¯(⁎)Ξc

Cited by 10 publications

References 96 publications

Magnetic dipole moments of the hidden-charm pentaquark states: $$P_c(4440)$$, $$P_c(4457)$$ and $$P_{cs}(4459)$$

Magnetic dipole moments of the hidden-charm pentaquark states: $$P_c(4440)$$, $$P_c(4457)$$ and $$P_{cs}(4459)$$

Magnetic dipole moments of the Ω (3185)0 and Ω (3327)0 states from molecular perspective

Elucidating the nature of hidden-charm pentaquark states with spin-32 through their electromagnetic form factors

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