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Main Authors: Lin, Zi-Yang, Cheng, Jian-Bo, Zhu, Shi-Lin
Format: Preprint
Published: 2022
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Online Access:https://arxiv.org/abs/2205.14628
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author Lin, Zi-Yang
Cheng, Jian-Bo
Zhu, Shi-Lin
author_facet Lin, Zi-Yang
Cheng, Jian-Bo
Zhu, Shi-Lin
contents We use the leading order (LO) contact interactions and OPE potentials to investigate the newly observed double-charm state $T_{cc}^+$. The $DDπ$ three-body effect is important in this system since the intermediate states can go on shell. We keep the dependence of the pion propagators on the center-of-mass energy, which results in a unitary cut of the OPE potential at the $DDπ$ three-body threshold. By solving the complex scaled Schrödinger equation, we find a pole corresponding to the $T_{cc}^+$ on the physical Riemann sheet. Its width is around 80 keV and nearly independent of the choice of the cutoff. Assuming the $D\bar{D}π$ and $D\bar{D}^*$ channels as the main decay channels, we apply the similar calculations to the $X(3872)$, and find its width is even smaller. Besides, the isospin breaking effect is significant for the $X(3872)$ while its impact on the $T_{cc}^+$ is relatively small.
format Preprint
id arxiv_https___arxiv_org_abs_2205_14628
institution arXiv
publishDate 2022
record_format arxiv
spellingShingle $T_{cc}^+$ and $X(3872)$ with the complex scaling method and $DD(\bar{D})π$ three-body effect
Lin, Zi-Yang
Cheng, Jian-Bo
Zhu, Shi-Lin
High Energy Physics - Phenomenology
We use the leading order (LO) contact interactions and OPE potentials to investigate the newly observed double-charm state $T_{cc}^+$. The $DDπ$ three-body effect is important in this system since the intermediate states can go on shell. We keep the dependence of the pion propagators on the center-of-mass energy, which results in a unitary cut of the OPE potential at the $DDπ$ three-body threshold. By solving the complex scaled Schrödinger equation, we find a pole corresponding to the $T_{cc}^+$ on the physical Riemann sheet. Its width is around 80 keV and nearly independent of the choice of the cutoff. Assuming the $D\bar{D}π$ and $D\bar{D}^*$ channels as the main decay channels, we apply the similar calculations to the $X(3872)$, and find its width is even smaller. Besides, the isospin breaking effect is significant for the $X(3872)$ while its impact on the $T_{cc}^+$ is relatively small.
title $T_{cc}^+$ and $X(3872)$ with the complex scaling method and $DD(\bar{D})π$ three-body effect
topic High Energy Physics - Phenomenology
url https://arxiv.org/abs/2205.14628