How does the $X(3872)$ show up in $e^+e^-$ collisions: dip versus peak

Fuente: arXiv
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Autori principali: Baru, Vadim, Guo, Feng-Kun, Hanhart, Christoph, Nefediev, Alexey
Natura: Preprint
Pubblicazione: 2024
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author Baru, Vadim
Guo, Feng-Kun
Hanhart, Christoph
Nefediev, Alexey
author_facet Baru, Vadim
Guo, Feng-Kun
Hanhart, Christoph
Nefediev, Alexey
contents We demonstrate that the dip observed near the total energy of 3872 MeV in the recent cross section data from the BESIII Collaboration for $e^+e^-\to J/ψπ^+π^- $ admits a natural explanation as a coupled-channel effect: it is a consequence of unitarity and a strong $S$-wave $D\bar D^*$ attraction that generates the state $X(3872)$. We anticipate the appearance of a similar dip in the $e^+e^-\to J/ψπ^+π^-π^0$ final state near the $D^*\bar{D}^*$ threshold driven by the same general mechanism, then to be interpreted as a signature of the predicted spin-two partner of the $X(3872)$.
format Preprint
id arxiv_https___arxiv_org_abs_2404_12003
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle How does the $X(3872)$ show up in $e^+e^-$ collisions: dip versus peak
Baru, Vadim
Guo, Feng-Kun
Hanhart, Christoph
Nefediev, Alexey
High Energy Physics - Phenomenology
We demonstrate that the dip observed near the total energy of 3872 MeV in the recent cross section data from the BESIII Collaboration for $e^+e^-\to J/ψπ^+π^- $ admits a natural explanation as a coupled-channel effect: it is a consequence of unitarity and a strong $S$-wave $D\bar D^*$ attraction that generates the state $X(3872)$. We anticipate the appearance of a similar dip in the $e^+e^-\to J/ψπ^+π^-π^0$ final state near the $D^*\bar{D}^*$ threshold driven by the same general mechanism, then to be interpreted as a signature of the predicted spin-two partner of the $X(3872)$.
title How does the $X(3872)$ show up in $e^+e^-$ collisions: dip versus peak
topic High Energy Physics - Phenomenology
url https://arxiv.org/abs/2404.12003