Measurement of B(Λc+→pK-π+)
The Λc+→pK-π+ yield has been measured in a sample of two-jet continuum events containing both a charm tag ("D̄") as well as an antiproton (e+e-→D̄p̄X), with the antiproton in the hemisphere opposite the D̄ (measurement of charge conjugate modes is implicit throughout). Under the hypothesis...
| Asıl Yazarlar: | , , , , , , , , , , , , , , , , , , , , , , , , |
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| Materyal Türü: | Journal article |
| Dil: | English |
| Baskı/Yayın Bilgisi: |
2000
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| _version_ | 1826303129587548160 |
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| author | Jaffe, D Masek, G Paar, H Potter, E Prell, S Sharma, V Asner, D Eppich, A Gronberg, J Hill, T Lange, D Morrison, R Briere, R Behrens, B Ford, W Gritsan, A Roy, J Smith, J Alexander, J Baker, R Bebek, C Berger, B Berkelman, K Blanc, F Boisvert, V |
| author_facet | Jaffe, D Masek, G Paar, H Potter, E Prell, S Sharma, V Asner, D Eppich, A Gronberg, J Hill, T Lange, D Morrison, R Briere, R Behrens, B Ford, W Gritsan, A Roy, J Smith, J Alexander, J Baker, R Bebek, C Berger, B Berkelman, K Blanc, F Boisvert, V |
| author_sort | Jaffe, D |
| collection | OXFORD |
| description | The Λc+→pK-π+ yield has been measured in a sample of two-jet continuum events containing both a charm tag ("D̄") as well as an antiproton (e+e-→D̄p̄X), with the antiproton in the hemisphere opposite the D̄ (measurement of charge conjugate modes is implicit throughout). Under the hypothesis that such selection criteria tag e+e-→D̄p̄Λc+X events, the Λc+→pK-π+ branching fraction can be determined by measuring the pK-π+ yield in the same hemisphere as the antiprotons in our D̄p̄X sample. Three types of D charm tags are used, πsoft- (from D*-→D̄0πsoft-), electrons (from D̄→Xe-v), and fully reconstructed D̄0→K+π- or D- →K+π-π- or Ds-→φπ-. Combining our results obtained from the three independent charm tags, we obtain B(Λc+→pK-π +)=(5.0±0.5±1.2)%. ©2000 The American Physical Society. |
| first_indexed | 2024-03-07T05:57:57Z |
| format | Journal article |
| id | oxford-uuid:eb2c4a53-e235-4a19-bc6e-34c4bfb51b4e |
| institution | University of Oxford |
| language | English |
| last_indexed | 2024-03-07T05:57:57Z |
| publishDate | 2000 |
| record_format | dspace |
| spelling | oxford-uuid:eb2c4a53-e235-4a19-bc6e-34c4bfb51b4e2022-03-27T11:07:48ZMeasurement of B(Λc+→pK-π+)Journal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:eb2c4a53-e235-4a19-bc6e-34c4bfb51b4eEnglishSymplectic Elements at Oxford2000Jaffe, DMasek, GPaar, HPotter, EPrell, SSharma, VAsner, DEppich, AGronberg, JHill, TLange, DMorrison, RBriere, RBehrens, BFord, WGritsan, ARoy, JSmith, JAlexander, JBaker, RBebek, CBerger, BBerkelman, KBlanc, FBoisvert, VThe Λc+→pK-π+ yield has been measured in a sample of two-jet continuum events containing both a charm tag ("D̄") as well as an antiproton (e+e-→D̄p̄X), with the antiproton in the hemisphere opposite the D̄ (measurement of charge conjugate modes is implicit throughout). Under the hypothesis that such selection criteria tag e+e-→D̄p̄Λc+X events, the Λc+→pK-π+ branching fraction can be determined by measuring the pK-π+ yield in the same hemisphere as the antiprotons in our D̄p̄X sample. Three types of D charm tags are used, πsoft- (from D*-→D̄0πsoft-), electrons (from D̄→Xe-v), and fully reconstructed D̄0→K+π- or D- →K+π-π- or Ds-→φπ-. Combining our results obtained from the three independent charm tags, we obtain B(Λc+→pK-π +)=(5.0±0.5±1.2)%. ©2000 The American Physical Society. |
| spellingShingle | Jaffe, D Masek, G Paar, H Potter, E Prell, S Sharma, V Asner, D Eppich, A Gronberg, J Hill, T Lange, D Morrison, R Briere, R Behrens, B Ford, W Gritsan, A Roy, J Smith, J Alexander, J Baker, R Bebek, C Berger, B Berkelman, K Blanc, F Boisvert, V Measurement of B(Λc+→pK-π+) |
| title | Measurement of B(Λc+→pK-π+) |
| title_full | Measurement of B(Λc+→pK-π+) |
| title_fullStr | Measurement of B(Λc+→pK-π+) |
| title_full_unstemmed | Measurement of B(Λc+→pK-π+) |
| title_short | Measurement of B(Λc+→pK-π+) |
| title_sort | measurement of b λc pk π |
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