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Study of $e^+e^-\to \Upsilon(\rm1S,2S)\eta$ and $e^+e^-\to \Upsilon(\rm 1S)\eta^{\prime}$ at $\sqrt{s}=10.866$ GeV with the Belle detector
- Source :
- Physical review / D 104(11), 112006 (2021). doi:10.1103/PhysRevD.104.112006
- Publication Year :
- 2021
-
Abstract
- Physical review / D 104(11), 112006 (2021). doi:10.1103/PhysRevD.104.112006<br />We report the first observation of the processes $e^+e^-\to\Upsilon(\rm 1S,2S)\eta$ at $\sqrt{s}=10.866$~GeV with a $10.2\sigma$ and $16.5\sigma$ significance respectively. The measured Born cross sections are $\sigma(e^+e^- \to \Upsilon(2S)\eta)=2.07 \pm 0.21 \pm 0.19$~pb, and $\sigma(e^+e^- \to \Upsilon(\rm 1S)\eta)=0.42 \pm 0.08 \pm 0.04$~pb. We also set the upper limit on the cross section of the process $e^+e^- \to \Upsilon(\rm 1S)\eta^{\prime}$ to be $\sigma(e^+e^- \to \Upsilon(\rm 1S)\eta^{\prime})<br />Published by Inst., Melville, NY
- Subjects :
- Born approximation
eta(958)
Upsilon(9460): electroproduction
measured [channel cross section]
BELLE
annihilation [electron positron]
electron positron: annihilation
eta
channel cross section: upper limit
High Energy Physics - Experiment
14.40.Pq
KEK-B
Upsilon(10020): electroproduction
13.25.Gv
tree approximation
ddc:530
electron positron --> Upsilon(9460) eta(958)
Nuclear Experiment
electron positron --> Upsilon(9460) eta
electroproduction [Upsilon(10020)]
upper limit [channel cross section]
electron positron: colliding beams
electron positron --> Upsilon(10020) eta
10.63-11.02 GeV-cms
13.66.Bc
colliding beams [electron positron]
electroproduction [Upsilon(9460)]
High Energy Physics::Experiment
channel cross section: measured
experimental results
Subjects
Details
- Language :
- English
- Database :
- OpenAIRE
- Journal :
- Physical review / D 104(11), 112006 (2021). doi:10.1103/PhysRevD.104.112006
- Accession number :
- edsair.doi.dedup.....11476b85315b866276683a7ea8ff69cd
- Full Text :
- https://doi.org/10.3204/PUBDB-2021-04684