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DC Field | Value | Language |
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dc.contributor.author | Bhardwaj, V. | - |
dc.date.accessioned | 2020-12-03T06:39:02Z | - |
dc.date.available | 2020-12-03T06:39:02Z | - |
dc.date.issued | 2016 | - |
dc.identifier.citation | Physical Review D, 93(11). | en_US |
dc.identifier.other | https://doi.org/10.1103/PhysRevD.93.112017 | - |
dc.identifier.uri | https://journals.aps.org/prd/abstract/10.1103/PhysRevD.93.112017 | - |
dc.identifier.uri | http://hdl.handle.net/123456789/2557 | - |
dc.description | Only IISERM authors are available in the record. | - |
dc.description.abstract | The process γ γ → p ¯ p K + K − and its intermediate processes are measured for the first time using a 980 fb − 1 data sample collected with the Belle detector at the KEKB asymmetric-energy e + e − collider. The production of p ¯ p K + K − and a Λ ( 1520 ) 0 ( ¯¯¯ Λ ( 1520 ) 0 ) signal in the p K − ( ¯ p K + ) invariant mass spectrum are clearly observed. However, no evidence for an exotic baryon near 1540 MeV / c 2 , denoted as Θ ( 1540 ) 0 ( ¯¯¯ Θ ( 1540 ) 0 ) or Θ ( 1540 ) + + ( Θ ( 1540 ) − − ), is seen in the p K − ( ¯ p K + ) or p K + ( ¯ p K − ) invariant mass spectra. Cross sections for γ γ → p ¯ p K + K − , Λ ( 1520 ) 0 ¯ p K + + c . c . and the products σ ( γ γ → Θ ( 1540 ) 0 ¯ p K + + c . c . ) B ( Θ ( 1540 ) 0 → p K − ) and σ ( γ γ → Θ ( 1540 ) + + ¯ p K − + c . c . ) B ( Θ ( 1540 ) + + → p K + ) are measured. We also determine upper limits on the products of the χ c 0 and χ c 2 two-photon decay widths and their branching fractions to p ¯ p K + K − at the 90% credibility level. | en_US |
dc.language.iso | en | en_US |
dc.publisher | American Physical Society | en_US |
dc.subject | Asymmetric-energy | en_US |
dc.subject | KEKB | en_US |
dc.subject | Intermediate processes | en_US |
dc.subject | Belle detector | en_US |
dc.title | First observation of γ γ → p ¯ p K + K − and search for exotic baryons in p K systems | en_US |
dc.type | Article | en_US |
Appears in Collections: | Research Articles |
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