Novel Method for Precisely Measuring the X(3872) Mass
The X(3872) is the first and the most interesting one amongst the abundant XYZ states. Its mass coincides exactly with the D^{0}D[over ¯]^{*0} threshold with an uncertainty of 180 keV. Precise knowledge of its mass is crucial to understand the X(3872). However, whether it is above or below the D^{0}...
Gespeichert in:
Veröffentlicht in: | Physical review letters 2019-05, Vol.122 (20), p.202002-202002, Article 202002 |
---|---|
1. Verfasser: | |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
Zusammenfassung: | The X(3872) is the first and the most interesting one amongst the abundant XYZ states. Its mass coincides exactly with the D^{0}D[over ¯]^{*0} threshold with an uncertainty of 180 keV. Precise knowledge of its mass is crucial to understand the X(3872). However, whether it is above or below the D^{0}D[over ¯]^{*0} threshold is still unknown. We propose a completely new method to measure the X(3872) mass precisely by measuring the X(3872)γ line shape between 4010 and 4020 MeV, which is strongly sensitive to the X(3872) mass relative to the D^{0}D[over ¯]^{*0} threshold due to a triangle singularity. This method can be applied to experiments which produce copious D^{*0}D[over ¯]^{*0} pairs, such as electron-positron, proton-antiproton, and other experiments, and may lead to much more precise knowledge of the X(3872) mass. |
---|---|
ISSN: | 0031-9007 1079-7114 |
DOI: | 10.1103/PhysRevLett.122.202002 |