Measurement of the e + e − → K S 0 K L 0 π 0 cross sections from s = 2. 000 to 3. 080 GeV
Based on e+e− collision data collected at center-of-mass energies from 2.000 to 3.080 GeV by the BESIII detector at the BEPCII collider, a partial wave analysis is performed for the process e+e− → KS0KL0π0. The results allow the Born cross sections of the process e+e− → KS0KL0π0, as well as its subp...
Main Authors: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
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Format: | Journal article |
Language: | English |
Published: |
Springer
2024
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Summary: | Based on e+e− collision data collected at center-of-mass energies from 2.000 to 3.080 GeV by the BESIII detector at the BEPCII collider, a partial wave analysis is performed for the process e+e− → KS0KL0π0. The results allow the Born cross sections of the process e+e− → KS0KL0π0, as well as its subprocesses e+e− → K∗(892)0K¯0 and K2∗(1430)0K¯0 to be measured. The Born cross sections for e+e− → KS0KL0π0 are consistent with previous measurements by BaBar, but with substantially improved precision. The Born cross section lineshape of the process e+e−K∗(892)0K¯0 is consistent with a vector meson state around 2.2 GeV with a significance of 3.2σ. A Breit-Wigner fit determines its mass as MY = (2164.7 ± 9.1 ± 3.1) MeV/c2 and its width as ΓY = (32.4 ± 21.0 ± 1.8) MeV. |
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