Abstract
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 crucial as their results can help us better understand their internal structure and the dynamics of the QCD as the theory of the strong interaction. We compare the results extracted for the magnetic moment with the existing theoretical predictions. It is seen that the obtained magnetic moment values are quite compatible with the results in the literature.
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Appendix: The explicit expressions of \(\Delta ^{QCD}\) function
Appendix: The explicit expressions of \(\Delta ^{QCD}\) function
In this appendix, we present the explicit expression for the function \(\Delta ^{QCD} \) obtained from the LCSR in subsection 2.1. It is acquired by selecting the \(\varepsilon \!\!\!/q\!\!\!/\) structure as follows
The functions I[n, m, l] is defined as:
where \(\alpha = (2m_Q+m_{Q^\prime })^2 \).
It should be noted that in the expressions given in Eq. (27), we have given only the terms that make significant contributions to the numerical values of the magnetic moments. Contributions not given here are taken into account in numerical calculations, but for simplicity they are not shown in the text.
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Mutuk, H., Özdem, U. Magnetic moments of spin–1/2 triply heavy baryons: a study of light-cone QCD and quark–diquark model. Eur. Phys. J. Plus 137, 508 (2022). https://doi.org/10.1140/epjp/s13360-022-02724-5
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DOI: https://doi.org/10.1140/epjp/s13360-022-02724-5