Study of the B<sup>+</sup><sub>c</sub> → J/ψ D<sup>+</sup><sub>s</sub> and B<sup>+</sup><sub>c</sub>→ J/ψ D<sup>*+</sup><sub>s</sub> decays with the ATLAS detector
- Autores
- Alconada Verzini, María Josefina; Alonso, Francisco; Arduh, Francisco Anuar; Dova, María Teresa; Monticelli, Fernando Gabriel; Wahlberg, Hernán Pablo; The ATLAS Collaboration
- Año de publicación
- 2016
- Idioma
- inglés
- Tipo de recurso
- artículo
- Estado
- versión publicada
- Descripción
- The decays B+c→J/ψD+s and B+c→J/ψD*+s are studied with the ATLAS detector at the LHC using a dataset corresponding to integrated luminosities of 4.9 and 20.6 fb−1 of pp collisions collected at centre-of-mass energies √s=7 TeV and 8 TeV, respectively. Signal candidates are identified through J/ψ→μ+μ− and D(*)+s→ϕπ+(γ/π0) decays. With a two-dimensional likelihood fit involving the B+c reconstructed invariant mass and an angle between the μ+ and D+s candidate momenta in the muon pair rest frame, the yields of B+c→J/ψD+s and B+c→J/ψD*+s, and the transverse polarisation fraction in B+c→J/ψD*+s decay are measured. The transverse polarisation fraction is determined to be Γ±±(B+c→J/ψD*+s)/Γ(B+c→J/ψD*+s)=0.38±0.23±0.07, and the derived ratio of the branching fractions of the two modes is BB+c→J/ψD*+s/BB+c→J/ψD+s=2.8+1.2−0.8±0.3 , where the first error is statistical and the second is systematic. Finally, a sample of B+c→J/ψπ+ decays is used to derive the ratios of branching fractions BBB+c→J/ψD*+s/BB+c→J/ψπ+=3.8±1.1±0.4±0.2 and BB+c→J/ψD*+s/BB+c→J/ψπ+=10.4±3.1±1.5±0.6, where the third error corresponds to the uncertainty of the branching fraction of D+s→ϕ(K+K−)π+ decay. The available theoretical predictions are generally consistent with the measurement.
Facultad de Ciencias Exactas - Materia
-
Ciencias Exactas
Física
Partículas Elementales
ATLAS detector
la̵rge hadron collider - Nivel de accesibilidad
- acceso abierto
- Condiciones de uso
- http://creativecommons.org/licenses/by/4.0/
- Repositorio
- Institución
- Universidad Nacional de La Plata
- OAI Identificador
- oai:sedici.unlp.edu.ar:10915/80966
Ver los metadatos del registro completo
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SEDICI (UNLP) |
spelling |
Study of the B<sup>+</sup><sub>c</sub> → J/ψ D<sup>+</sup><sub>s</sub> and B<sup>+</sup><sub>c</sub>→ J/ψ D<sup>*+</sup><sub>s</sub> decays with the ATLAS detectorAlconada Verzini, María JosefinaAlonso, FranciscoArduh, Francisco AnuarDova, María TeresaMonticelli, Fernando GabrielWahlberg, Hernán PabloThe ATLAS CollaborationCiencias ExactasFísicaPartículas ElementalesATLAS detectorla̵rge hadron colliderThe decays B<sup>+</sup><sub>c</sub>→J/ψD<sup>+</sup><sub>s</sub> and B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub> are studied with the ATLAS detector at the LHC using a dataset corresponding to integrated luminosities of 4.9 and 20.6 fb<sup>−1</sup> of pp collisions collected at centre-of-mass energies √s=7 TeV and 8 TeV, respectively. Signal candidates are identified through J/ψ→μ+μ− and D<sup>(*)+</sup><sub>s</sub>→ϕπ+(γ/π<sup>0</sup>) decays. With a two-dimensional likelihood fit involving the B<sup>+</sup><sub>c</sub> reconstructed invariant mass and an angle between the μ+ and D<sup>+</sup><sub>s</sub> candidate momenta in the muon pair rest frame, the yields of B<sup>+</sup><sub>c</sub>→J/ψD<sup>+</sup><sub>s</sub> and B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub>, and the transverse polarisation fraction in B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub> decay are measured. The transverse polarisation fraction is determined to be Γ±±(B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub>)/Γ(B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub>)=0.38±0.23±0.07, and the derived ratio of the branching fractions of the two modes is B<sub>B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub></sub>/B<sub>B<sup>+</sup><sub>c</sub>→J/ψD<sup>+</sup><sub>s</sub></sub>=2.8+1.2−0.8±0.3 , where the first error is statistical and the second is systematic. Finally, a sample of B<sup>+</sup><sub>c</sub>→J/ψπ+ decays is used to derive the ratios of branching fractions BB<sub>B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub></sub>/B<sub>B<sup>+</sup><sub>c</sub>→J/ψπ+</sub>=3.8±1.1±0.4±0.2 and B<sub>B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub></sub>/B<sub>B<sup>+</sup><sub>c</sub>→J/ψπ+</sub>=10.4±3.1±1.5±0.6, where the third error corresponds to the uncertainty of the branching fraction of D<sup>+</sup><sub>s</sub>→ϕ(K+K−)π+ decay. The available theoretical predictions are generally consistent with the measurement.Facultad de Ciencias Exactas2016-01-05info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionArticulohttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfhttp://sedici.unlp.edu.ar/handle/10915/80966enginfo:eu-repo/semantics/altIdentifier/issn/1434-6052info:eu-repo/semantics/altIdentifier/doi/10.1140/epjc/s10052-015-3743-8info:eu-repo/semantics/openAccesshttp://creativecommons.org/licenses/by/4.0/Creative Commons Attribution 4.0 International (CC BY 4.0)reponame:SEDICI (UNLP)instname:Universidad Nacional de La Platainstacron:UNLP2025-09-29T11:14:57Zoai:sedici.unlp.edu.ar:10915/80966Institucionalhttp://sedici.unlp.edu.ar/Universidad públicaNo correspondehttp://sedici.unlp.edu.ar/oai/snrdalira@sedici.unlp.edu.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:13292025-09-29 11:14:57.957SEDICI (UNLP) - Universidad Nacional de La Platafalse |
dc.title.none.fl_str_mv |
Study of the B<sup>+</sup><sub>c</sub> → J/ψ D<sup>+</sup><sub>s</sub> and B<sup>+</sup><sub>c</sub>→ J/ψ D<sup>*+</sup><sub>s</sub> decays with the ATLAS detector |
title |
Study of the B<sup>+</sup><sub>c</sub> → J/ψ D<sup>+</sup><sub>s</sub> and B<sup>+</sup><sub>c</sub>→ J/ψ D<sup>*+</sup><sub>s</sub> decays with the ATLAS detector |
spellingShingle |
Study of the B<sup>+</sup><sub>c</sub> → J/ψ D<sup>+</sup><sub>s</sub> and B<sup>+</sup><sub>c</sub>→ J/ψ D<sup>*+</sup><sub>s</sub> decays with the ATLAS detector Alconada Verzini, María Josefina Ciencias Exactas Física Partículas Elementales ATLAS detector la̵rge hadron collider |
title_short |
Study of the B<sup>+</sup><sub>c</sub> → J/ψ D<sup>+</sup><sub>s</sub> and B<sup>+</sup><sub>c</sub>→ J/ψ D<sup>*+</sup><sub>s</sub> decays with the ATLAS detector |
title_full |
Study of the B<sup>+</sup><sub>c</sub> → J/ψ D<sup>+</sup><sub>s</sub> and B<sup>+</sup><sub>c</sub>→ J/ψ D<sup>*+</sup><sub>s</sub> decays with the ATLAS detector |
title_fullStr |
Study of the B<sup>+</sup><sub>c</sub> → J/ψ D<sup>+</sup><sub>s</sub> and B<sup>+</sup><sub>c</sub>→ J/ψ D<sup>*+</sup><sub>s</sub> decays with the ATLAS detector |
title_full_unstemmed |
Study of the B<sup>+</sup><sub>c</sub> → J/ψ D<sup>+</sup><sub>s</sub> and B<sup>+</sup><sub>c</sub>→ J/ψ D<sup>*+</sup><sub>s</sub> decays with the ATLAS detector |
title_sort |
Study of the B<sup>+</sup><sub>c</sub> → J/ψ D<sup>+</sup><sub>s</sub> and B<sup>+</sup><sub>c</sub>→ J/ψ D<sup>*+</sup><sub>s</sub> decays with the ATLAS detector |
dc.creator.none.fl_str_mv |
Alconada Verzini, María Josefina Alonso, Francisco Arduh, Francisco Anuar Dova, María Teresa Monticelli, Fernando Gabriel Wahlberg, Hernán Pablo The ATLAS Collaboration |
author |
Alconada Verzini, María Josefina |
author_facet |
Alconada Verzini, María Josefina Alonso, Francisco Arduh, Francisco Anuar Dova, María Teresa Monticelli, Fernando Gabriel Wahlberg, Hernán Pablo The ATLAS Collaboration |
author_role |
author |
author2 |
Alonso, Francisco Arduh, Francisco Anuar Dova, María Teresa Monticelli, Fernando Gabriel Wahlberg, Hernán Pablo The ATLAS Collaboration |
author2_role |
author author author author author author |
dc.subject.none.fl_str_mv |
Ciencias Exactas Física Partículas Elementales ATLAS detector la̵rge hadron collider |
topic |
Ciencias Exactas Física Partículas Elementales ATLAS detector la̵rge hadron collider |
dc.description.none.fl_txt_mv |
The decays B<sup>+</sup><sub>c</sub>→J/ψD<sup>+</sup><sub>s</sub> and B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub> are studied with the ATLAS detector at the LHC using a dataset corresponding to integrated luminosities of 4.9 and 20.6 fb<sup>−1</sup> of pp collisions collected at centre-of-mass energies √s=7 TeV and 8 TeV, respectively. Signal candidates are identified through J/ψ→μ+μ− and D<sup>(*)+</sup><sub>s</sub>→ϕπ+(γ/π<sup>0</sup>) decays. With a two-dimensional likelihood fit involving the B<sup>+</sup><sub>c</sub> reconstructed invariant mass and an angle between the μ+ and D<sup>+</sup><sub>s</sub> candidate momenta in the muon pair rest frame, the yields of B<sup>+</sup><sub>c</sub>→J/ψD<sup>+</sup><sub>s</sub> and B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub>, and the transverse polarisation fraction in B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub> decay are measured. The transverse polarisation fraction is determined to be Γ±±(B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub>)/Γ(B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub>)=0.38±0.23±0.07, and the derived ratio of the branching fractions of the two modes is B<sub>B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub></sub>/B<sub>B<sup>+</sup><sub>c</sub>→J/ψD<sup>+</sup><sub>s</sub></sub>=2.8+1.2−0.8±0.3 , where the first error is statistical and the second is systematic. Finally, a sample of B<sup>+</sup><sub>c</sub>→J/ψπ+ decays is used to derive the ratios of branching fractions BB<sub>B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub></sub>/B<sub>B<sup>+</sup><sub>c</sub>→J/ψπ+</sub>=3.8±1.1±0.4±0.2 and B<sub>B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub></sub>/B<sub>B<sup>+</sup><sub>c</sub>→J/ψπ+</sub>=10.4±3.1±1.5±0.6, where the third error corresponds to the uncertainty of the branching fraction of D<sup>+</sup><sub>s</sub>→ϕ(K+K−)π+ decay. The available theoretical predictions are generally consistent with the measurement. Facultad de Ciencias Exactas |
description |
The decays B<sup>+</sup><sub>c</sub>→J/ψD<sup>+</sup><sub>s</sub> and B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub> are studied with the ATLAS detector at the LHC using a dataset corresponding to integrated luminosities of 4.9 and 20.6 fb<sup>−1</sup> of pp collisions collected at centre-of-mass energies √s=7 TeV and 8 TeV, respectively. Signal candidates are identified through J/ψ→μ+μ− and D<sup>(*)+</sup><sub>s</sub>→ϕπ+(γ/π<sup>0</sup>) decays. With a two-dimensional likelihood fit involving the B<sup>+</sup><sub>c</sub> reconstructed invariant mass and an angle between the μ+ and D<sup>+</sup><sub>s</sub> candidate momenta in the muon pair rest frame, the yields of B<sup>+</sup><sub>c</sub>→J/ψD<sup>+</sup><sub>s</sub> and B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub>, and the transverse polarisation fraction in B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub> decay are measured. The transverse polarisation fraction is determined to be Γ±±(B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub>)/Γ(B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub>)=0.38±0.23±0.07, and the derived ratio of the branching fractions of the two modes is B<sub>B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub></sub>/B<sub>B<sup>+</sup><sub>c</sub>→J/ψD<sup>+</sup><sub>s</sub></sub>=2.8+1.2−0.8±0.3 , where the first error is statistical and the second is systematic. Finally, a sample of B<sup>+</sup><sub>c</sub>→J/ψπ+ decays is used to derive the ratios of branching fractions BB<sub>B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub></sub>/B<sub>B<sup>+</sup><sub>c</sub>→J/ψπ+</sub>=3.8±1.1±0.4±0.2 and B<sub>B<sup>+</sup><sub>c</sub>→J/ψD<sup>*+</sup><sub>s</sub></sub>/B<sub>B<sup>+</sup><sub>c</sub>→J/ψπ+</sub>=10.4±3.1±1.5±0.6, where the third error corresponds to the uncertainty of the branching fraction of D<sup>+</sup><sub>s</sub>→ϕ(K+K−)π+ decay. The available theoretical predictions are generally consistent with the measurement. |
publishDate |
2016 |
dc.date.none.fl_str_mv |
2016-01-05 |
dc.type.none.fl_str_mv |
info:eu-repo/semantics/article info:eu-repo/semantics/publishedVersion Articulo http://purl.org/coar/resource_type/c_6501 info:ar-repo/semantics/articulo |
format |
article |
status_str |
publishedVersion |
dc.identifier.none.fl_str_mv |
http://sedici.unlp.edu.ar/handle/10915/80966 |
url |
http://sedici.unlp.edu.ar/handle/10915/80966 |
dc.language.none.fl_str_mv |
eng |
language |
eng |
dc.relation.none.fl_str_mv |
info:eu-repo/semantics/altIdentifier/issn/1434-6052 info:eu-repo/semantics/altIdentifier/doi/10.1140/epjc/s10052-015-3743-8 |
dc.rights.none.fl_str_mv |
info:eu-repo/semantics/openAccess http://creativecommons.org/licenses/by/4.0/ Creative Commons Attribution 4.0 International (CC BY 4.0) |
eu_rights_str_mv |
openAccess |
rights_invalid_str_mv |
http://creativecommons.org/licenses/by/4.0/ Creative Commons Attribution 4.0 International (CC BY 4.0) |
dc.format.none.fl_str_mv |
application/pdf |
dc.source.none.fl_str_mv |
reponame:SEDICI (UNLP) instname:Universidad Nacional de La Plata instacron:UNLP |
reponame_str |
SEDICI (UNLP) |
collection |
SEDICI (UNLP) |
instname_str |
Universidad Nacional de La Plata |
instacron_str |
UNLP |
institution |
UNLP |
repository.name.fl_str_mv |
SEDICI (UNLP) - Universidad Nacional de La Plata |
repository.mail.fl_str_mv |
alira@sedici.unlp.edu.ar |
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score |
13.070432 |