Measurement of the running of the electromagnetic coupling at large momentum-transfer at LEP
- Autores
- Dova, María Teresa; L3 Collaboration
- Año de publicación
- 2005
- Idioma
- inglés
- Tipo de recurso
- artículo
- Estado
- versión publicada
- Descripción
- The evolution of the electromagnetic coupling, α, in the momentum-transfer range 1800 GeV2 < −Q2 < 21600 GeV2 is studied with about 40 000 Bhabha-scattering events collected with the L3 detector at LEP at centre-of-mass energies √s = 189–209 GeV. The running of α is parametrised as: where α0 ≡ α(Q2 = 0) is the fine-structure constant and C = 1 corresponds to the evolution expected in QED. A fit to the differential cross section of the e+e− → e+e− process for scattering angles in the range |cos θ| < 0.9 excludes the hypothesis of a constant value of α, C = 0, and validates the QED prediction with the result: C = 1.05 ± 0.07 ± 0.14, where the first uncertainty is statistical and the second systematic.
Facultad de Ciencias Exactas - Materia
-
Ciencias Exactas
Física
Electromagnetismo
L3 detector - Nivel de accesibilidad
- acceso abierto
- Condiciones de uso
- http://creativecommons.org/licenses/by/3.0/
- Repositorio
.jpg)
- Institución
- Universidad Nacional de La Plata
- OAI Identificador
- oai:sedici.unlp.edu.ar:10915/79504
Ver los metadatos del registro completo
| id |
SEDICI_e963a35b8c5c3e1696167919d13e87ce |
|---|---|
| oai_identifier_str |
oai:sedici.unlp.edu.ar:10915/79504 |
| network_acronym_str |
SEDICI |
| repository_id_str |
1329 |
| network_name_str |
SEDICI (UNLP) |
| spelling |
Measurement of the running of the electromagnetic coupling at large momentum-transfer at LEPDova, María TeresaL3 CollaborationCiencias ExactasFísicaElectromagnetismoL3 detectorThe evolution of the electromagnetic coupling, α, in the momentum-transfer range 1800 GeV<sup>2</sup> < −Q<sup>2</sup> < 21600 GeV<sup>2</sup> is studied with about 40 000 Bhabha-scattering events collected with the L3 detector at LEP at centre-of-mass energies √s = 189–209 GeV. The running of α is parametrised as: <math><mi is="true">α</mi><mrow is="true"><mo is="true">(</mo><msup is="true"><mi is="true">Q</mi><mn is="true">2</mn></msup><mo is="true">)</mo></mrow><mo is="true">=</mo><mfrac is="true"><msub is="true"><mi is="true">α</mi><mn is="true">0</mn></msub><mrow is="true"><mn is="true">1</mn><mo is="true">−</mo><mi is="true">C</mi><mi mathvariant="normal" is="true">Δ</mi><mi is="true">α</mi><mo stretchy="false" is="true">(</mo><msup is="true"><mi is="true">Q</mi><mn is="true">2</mn></msup><mo stretchy="false" is="true">)</mo></mrow></mfrac><mo is="true">,</mo></math> where α<sub>0</sub> ≡ α(Q<sup>2</sup> = 0) is the fine-structure constant and C = 1 corresponds to the evolution expected in QED. A fit to the differential cross section of the e<sup>+</sup>e<sup>−</sup> → e<sup>+</sup>e<sup>−</sup> process for scattering angles in the range |cos θ| < 0.9 excludes the hypothesis of a constant value of α, C = 0, and validates the QED prediction with the result: C = 1.05 ± 0.07 ± 0.14, where the first uncertainty is statistical and the second systematic.Facultad de Ciencias Exactas2005-08-02info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionArticulohttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdf26-36http://sedici.unlp.edu.ar/handle/10915/79504enginfo:eu-repo/semantics/altIdentifier/issn/0370-2693info:eu-repo/semantics/altIdentifier/doi/10.1016/j.physletb.2005.07.052info:eu-repo/semantics/openAccesshttp://creativecommons.org/licenses/by/3.0/Creative Commons Attribution 3.0 Unported (CC BY 3.0)reponame:SEDICI (UNLP)instname:Universidad Nacional de La Platainstacron:UNLP2025-11-12T10:36:39Zoai:sedici.unlp.edu.ar:10915/79504Institucionalhttp://sedici.unlp.edu.ar/Universidad públicaNo correspondehttp://sedici.unlp.edu.ar/oai/snrdalira@sedici.unlp.edu.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:13292025-11-12 10:36:39.452SEDICI (UNLP) - Universidad Nacional de La Platafalse |
| dc.title.none.fl_str_mv |
Measurement of the running of the electromagnetic coupling at large momentum-transfer at LEP |
| title |
Measurement of the running of the electromagnetic coupling at large momentum-transfer at LEP |
| spellingShingle |
Measurement of the running of the electromagnetic coupling at large momentum-transfer at LEP Dova, María Teresa Ciencias Exactas Física Electromagnetismo L3 detector |
| title_short |
Measurement of the running of the electromagnetic coupling at large momentum-transfer at LEP |
| title_full |
Measurement of the running of the electromagnetic coupling at large momentum-transfer at LEP |
| title_fullStr |
Measurement of the running of the electromagnetic coupling at large momentum-transfer at LEP |
| title_full_unstemmed |
Measurement of the running of the electromagnetic coupling at large momentum-transfer at LEP |
| title_sort |
Measurement of the running of the electromagnetic coupling at large momentum-transfer at LEP |
| dc.creator.none.fl_str_mv |
Dova, María Teresa L3 Collaboration |
| author |
Dova, María Teresa |
| author_facet |
Dova, María Teresa L3 Collaboration |
| author_role |
author |
| author2 |
L3 Collaboration |
| author2_role |
author |
| dc.subject.none.fl_str_mv |
Ciencias Exactas Física Electromagnetismo L3 detector |
| topic |
Ciencias Exactas Física Electromagnetismo L3 detector |
| dc.description.none.fl_txt_mv |
The evolution of the electromagnetic coupling, α, in the momentum-transfer range 1800 GeV<sup>2</sup> < −Q<sup>2</sup> < 21600 GeV<sup>2</sup> is studied with about 40 000 Bhabha-scattering events collected with the L3 detector at LEP at centre-of-mass energies √s = 189–209 GeV. The running of α is parametrised as: <math><mi is="true">α</mi><mrow is="true"><mo is="true">(</mo><msup is="true"><mi is="true">Q</mi><mn is="true">2</mn></msup><mo is="true">)</mo></mrow><mo is="true">=</mo><mfrac is="true"><msub is="true"><mi is="true">α</mi><mn is="true">0</mn></msub><mrow is="true"><mn is="true">1</mn><mo is="true">−</mo><mi is="true">C</mi><mi mathvariant="normal" is="true">Δ</mi><mi is="true">α</mi><mo stretchy="false" is="true">(</mo><msup is="true"><mi is="true">Q</mi><mn is="true">2</mn></msup><mo stretchy="false" is="true">)</mo></mrow></mfrac><mo is="true">,</mo></math> where α<sub>0</sub> ≡ α(Q<sup>2</sup> = 0) is the fine-structure constant and C = 1 corresponds to the evolution expected in QED. A fit to the differential cross section of the e<sup>+</sup>e<sup>−</sup> → e<sup>+</sup>e<sup>−</sup> process for scattering angles in the range |cos θ| < 0.9 excludes the hypothesis of a constant value of α, C = 0, and validates the QED prediction with the result: C = 1.05 ± 0.07 ± 0.14, where the first uncertainty is statistical and the second systematic. Facultad de Ciencias Exactas |
| description |
The evolution of the electromagnetic coupling, α, in the momentum-transfer range 1800 GeV<sup>2</sup> < −Q<sup>2</sup> < 21600 GeV<sup>2</sup> is studied with about 40 000 Bhabha-scattering events collected with the L3 detector at LEP at centre-of-mass energies √s = 189–209 GeV. The running of α is parametrised as: <math><mi is="true">α</mi><mrow is="true"><mo is="true">(</mo><msup is="true"><mi is="true">Q</mi><mn is="true">2</mn></msup><mo is="true">)</mo></mrow><mo is="true">=</mo><mfrac is="true"><msub is="true"><mi is="true">α</mi><mn is="true">0</mn></msub><mrow is="true"><mn is="true">1</mn><mo is="true">−</mo><mi is="true">C</mi><mi mathvariant="normal" is="true">Δ</mi><mi is="true">α</mi><mo stretchy="false" is="true">(</mo><msup is="true"><mi is="true">Q</mi><mn is="true">2</mn></msup><mo stretchy="false" is="true">)</mo></mrow></mfrac><mo is="true">,</mo></math> where α<sub>0</sub> ≡ α(Q<sup>2</sup> = 0) is the fine-structure constant and C = 1 corresponds to the evolution expected in QED. A fit to the differential cross section of the e<sup>+</sup>e<sup>−</sup> → e<sup>+</sup>e<sup>−</sup> process for scattering angles in the range |cos θ| < 0.9 excludes the hypothesis of a constant value of α, C = 0, and validates the QED prediction with the result: C = 1.05 ± 0.07 ± 0.14, where the first uncertainty is statistical and the second systematic. |
| publishDate |
2005 |
| dc.date.none.fl_str_mv |
2005-08-02 |
| 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/10915/79504 |
| url |
http://sedici.unlp.edu.ar/handle/10915/79504 |
| dc.language.none.fl_str_mv |
eng |
| language |
eng |
| dc.relation.none.fl_str_mv |
info:eu-repo/semantics/altIdentifier/issn/0370-2693 info:eu-repo/semantics/altIdentifier/doi/10.1016/j.physletb.2005.07.052 |
| dc.rights.none.fl_str_mv |
info:eu-repo/semantics/openAccess http://creativecommons.org/licenses/by/3.0/ Creative Commons Attribution 3.0 Unported (CC BY 3.0) |
| eu_rights_str_mv |
openAccess |
| rights_invalid_str_mv |
http://creativecommons.org/licenses/by/3.0/ Creative Commons Attribution 3.0 Unported (CC BY 3.0) |
| dc.format.none.fl_str_mv |
application/pdf 26-36 |
| 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 |
| _version_ |
1848605441773273088 |
| score |
12.976206 |