Measurement of exclusive<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>γ</mml:mi><mml:mi>γ</mml:mi><mml:mo stretchy="false">→</mml:mo><mml:msup><mml:mi>W</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mi>W</mml:mi><mml:mo>−</mml:mo></mml:msup></mml:math>production and search for exclusive Higgs boson production in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>p</mml:mi><mml:mi>p</mml:mi></mml:math>collisions at<mml:math …
Creators
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H. Zhu1
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Georges Aad2, 3, 4
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B. Abbott5
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J. Weingarten6
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O. Abdinov7
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Baptiste Abeloos8, 3, 9, 4
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Goetz Gaycken10, 11
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O. S. AbouZeid12
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N. Luke Abraham13
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Halina Abramowicz14
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Henso Abreu15
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S. L. Wu16
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Yiming Abulaiti17
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B. S. Acharya18, 19
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L. Adamczyk20
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David Barney21
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J. Adelman22
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S. Guindon23
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T. Adye24
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Agni Bethani25
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T. Agatonović-Jovin26
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R. M. Bianchi27
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Agni Bethani28, 29
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S. P. Ahlen30
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Faig Ahmadov31
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G. Aielli32, 33
- H. Åkerstedt17
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T. P. A. Åkesson34
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Andrei Akimov35
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Gian Luigi Alberghi36, 37, 38
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J. Albert39
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K. Jon-And40, 41, 3, 4
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María Josefina Alconada Verzini42, 43, 44
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F. Malek45
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S. Palestini31
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C. Alexa
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G. Alexander14
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Tal Roelof van Daalen46
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M. Alhroob5
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Babar Ali47
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S. Ali48, 49
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G. Alimonti50
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A. Lister51, 52
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H. Zhu53
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Cristinel Diaconu13
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A. I. Mincer16
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P. P. Allport54
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Francisco Alonso55
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A. Alonso56
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Francisco Alonso42, 43, 44
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Cristiano Alpigiani57
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Mahmoud Alstaty2, 3, 4
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Bárbara Álvarez González45
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S. Henrot-Versillé58, 59, 60
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N. Hod55
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A. Ventura61, 62
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B. R. Ko63
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David Barney64
- Christoph Amelung65
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D. Amidei66
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Susana Patricia Amor dos Santos28, 67
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A. Amorim28, 68
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Simone Amoroso45
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A. Ventura65
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Ana Rosario Cueto Gomez69
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N. Hod70
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A. Ventura54
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Kun Liu71
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C. F. Anders72
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G. Anders45
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John Kenneth Anders25
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J. Kretzschmar51, 52
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A. Andreazza73, 50
- V. Andrei72
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Stamatios Gkaitatzis74
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P. Pralavorio10, 11
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T. Carli75
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A. Angerami53
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S. Tisserant45
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Alexey Anisenkov76, 77
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Jos Vermeulen78
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Alexey Anisenkov79, 80
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A. Annovi72
- M. Antonelli81
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Romain Madar82
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F. Anulli83
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F. Hubaut63
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G. Bella54
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Jian Liu84
- Y. Arai63
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Jian Liu28
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Kun Liu85
- F. A. Arduh42, 43, 44
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Jean-François Arguin86, 87
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S. Argyropoulos6
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M. Arık88
- A. J. Armbruster89
- Lewis James Armitage90
- O. Arnaez45
- H. Arnold91
- 1. Mohamed I University
- 2. Aix-Marseille Université
- 3. Institut National de Physique Nucléaire et de Physique des Particules
- 4. Centre National de la Recherche Scientifique
- 5. University of Oklahoma
- 6. University of Iowa
- 7. Azerbaijan National Academy of Sciences
- 8. Université Paris-Saclay
- 9. Université Paris-Sud
- 10. National Institute for Subatomic Physics
- 11. University of Amsterdam
- 12. University of California, Santa Cruz
- 13. University of Sussex
- 14. Tel Aviv University
- 15. Technion – Israel Institute of Technology
- 16. University of Oregon
- 17. Stockholm University
- 18. The Abdus Salam International Centre for Theoretical Physics (ICTP)
- 19. INFN Sezione di Trieste
- 20. AGH University of Krakow
- 21. Brookhaven National Laboratory
- 22. Northern Illinois University
- 23. Ludwig-Maximilians-Universität München
- 24. Rutherford Appleton Laboratory
- 25. University of Liverpool
- 26. University of Belgrade
- 27. University of Göttingen
- 28. LIP - Laboratory of Instrumentation and Experimental Particle Physics
- 29. Universidad de Granada
- 30. Boston University
- 31. Joint Institute for Nuclear Research
- 32. University of Rome Tor Vergata
- 33. INFN Sezione di Roma II
- 34. Lund University
- 35. P.N. Lebedev Physical Institute of the Russian Academy of Sciences
- 36. Osservatorio astronomico di Bologna
- 37. University of Bologna
- 38. INFN Sezione di Bologna
- 39. University of Victoria
- 40. Laboratoire de Physique Subatomique et de Cosmologie
- 41. Université Grenoble Alpes
- 42. Instituto de Física La Plata
- 43. Consejo Nacional de Investigaciones Científicas y Técnicas
- 44. Universidad Nacional de La Plata
- 45. European Organization for Nuclear Research
- 46. National Technical University of Athens
- 47. Czech Technical University in Prague
- 48. INFN Sezione di Lecce
- 49. University of Salento
- 50. INFN Sezione di Milano
- 51. Fermi National Accelerator Laboratory
- 52. University of Chicago
- 53. Columbia University
- 54. University of Birmingham
- 55. INFN Sezione di Napoli
- 56. University of Copenhagen
- 57. University of Washington
- 58. Instituto de Física Corpuscular
- 59. Institut de Microelectrònica de Barcelona
- 60. Universitat de València
- 61. Lawrence Berkeley National Laboratory
- 62. University of California, Berkeley
- 63. High Energy Accelerator Research Organization
- 64. Universidade Federal do Rio de Janeiro
- 65. Brandeis University
- 66. University of Michigan–Ann Arbor
- 67. University of Coimbra
- 68. University of Lisbon
- 69. University of Sheffield
- 70. University of Geneva
- 71. The University of Texas at Austin
- 72. Heidelberg University
- 73. University of Milan
- 74. National and Kapodistrian University of Athens
- 75. TU Dresden
- 76. Budker Institute of Nuclear Physics
- 77. Siberian Branch of the Russian Academy of Sciences
- 78. Institute for High Energy Physics
- 79. INFN Sezione di Pisa
- 80. University of Pisa
- 81. National Laboratory of Frascati
- 82. Moscow Engineering Physics Institute
- 83. INFN Sezione di Roma I
- 84. Michigan State University
- 85. Duke University
- 86. Institute of Particle Physics
- 87. Université de Montréal
- 88. Boğaziçi University
- 89. SLAC National Accelerator Laboratory
- 90. Queen Mary University of London
- 91. University of Freiburg
Description
Searches for exclusively produced $W$ boson pairs in the process $pp(\ensuremath{\gamma}\ensuremath{\gamma})\ensuremath{\rightarrow}p{W}^{+}{W}^{\ensuremath{-}}p$ and an exclusively produced Higgs boson in the process $pp(gg)\ensuremath{\rightarrow}pHp$ have been performed using ${e}^{\ifmmode\pm\else\textpm\fi{}}{\ensuremath{\mu}}^{\ensuremath{\mp}}$ final states. These measurements use $20.2\text{ }\text{ }{\mathrm{fb}}^{\ensuremath{-}1}$ of $pp$ collisions collected by the ATLAS experiment at a center-of-mass energy $\sqrt{s}=8\text{ }\text{ }\mathrm{TeV}$ at the LHC. Exclusive production of ${W}^{+}{W}^{\ensuremath{-}}$ consistent with the Standard Model prediction is found with $3.0\ensuremath{\sigma}$ significance. The exclusive ${W}^{+}{W}^{\ensuremath{-}}$ production cross section is determined to be $\ensuremath{\sigma}(\ensuremath{\gamma}\ensuremath{\gamma}\ensuremath{\rightarrow}{W}^{+}{W}^{\ensuremath{-}}\ensuremath{\rightarrow}{e}^{\ifmmode\pm\else\textpm\fi{}}{\ensuremath{\mu}}^{\ensuremath{\mp}}X)=6.9\ifmmode\pm\else\textpm\fi{}2.2(\mathrm{stat})\ifmmode\pm\else\textpm\fi{}1.4(\mathrm{sys})\text{ }\text{ }\mathrm{fb}$, in agreement with the Standard Model prediction. Limits on anomalous quartic gauge couplings are set at 95% confidence level as $\ensuremath{-}1.7\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}6}<{a}_{0}^{W}/{\mathrm{\ensuremath{\Lambda}}}^{2}<1.7\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}6}\text{ }\text{ }{\mathrm{GeV}}^{\ensuremath{-}2}$ and $\ensuremath{-}6.4\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}6}<{a}_{C}^{W}/{\mathrm{\ensuremath{\Lambda}}}^{2}<6.3\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}6}\text{ }\text{ }{\mathrm{GeV}}^{\ensuremath{-}2}$. A 95% confidence-level upper limit on the total production cross section for an exclusive Higgs boson is set to 1.2 pb.
Translated Descriptions
Translated Description (Arabic)
البحث عن أزواج بوزون W$ المنتجة حصريًا في العملية $pp(\ ensuremath {\ gamma}\ ensuremath {\ gamma})\ ensuremath {\ rightarrow}p{W }^{+}{ W }^{\ ensuremath {-}} p$ و بوزون هيجز المنتج حصريًا في العملية $pp(gg)\ ensuremath {\ rightarrow} pHp $ تم إجراؤها باستخدام الحالات النهائية ${e}^{\ ifmmode\pm\ else\ textpm\ fi {}}{\ ensuremath {\ mu }}^{\ ensuremath {\mp }}$. تستخدم هذه القياسات $ 20.2\text{}\text {} {\ mathrm{fb }}^{\ ensuremath {-} 1 }$ من $ pp$ التصادمات التي جمعتها تجربة أطلس في طاقة مركز الكتلة $\sqrt{s }=8\text {}\text {}\mathrm{TeV }$ في مصادم الهادرونات الكبير. تم العثور على إنتاج حصري بقيمة ${W}^{+}{W}^{\ensuremath{-}}$ بما يتفق مع تنبؤات النموذج القياسي بقيمة $ 3.0\ensuremath{\ sigma }$. تم تحديد المقطع العرضي الحصري للإنتاج ${W}^{+}{W}^{\ ensuremath {-}}$ ليكون $\ ensuremath {\ sigma }(\ ensuremath {\ gamma}\ ensuremath {\ rightarrow }{ W }^{+}{ W }^{\ ensuremath {-}}\ ensuremath {\ rightarrow }{ e }^{\ ifmmode\ pm\ else\ textpm\ fi {}}{\ ensuremath {\ mp}} X )=6.9\ ifmmode\ pm\ else\ textpm\ fi {}2.2(\ mathrm{stat})\ ifmmode\ pm\ else\ textpm\fi {}1.4(\mathrm{sys})\text {}\ mathrm{fb }$، بما يتفق مع التنبؤ النموذجي. يتم تعيين الحدود على وصلات المقياس الرباعي الشاذة عند مستوى ثقة 95 ٪ مثل $\ ensuremath {-} 1.7\ ifmmode\ times\ else\ texttimes\ fi {} {10 }^{\ ensuremath {-} 6}<{ a }_{ 0 }^{ W }/{\ mathrm {\ ensuremath {\ lambda }}}}^{ 2 }<1.7\ ifmmode\ times\ else\ texttimes\fi{}^{ 10 }^{\ ensuremath {-} 6}\ text {}\text {} {} {\ mathrm{GeV }}^{\ ensuremath {-} 2 }$ و $\ ensuremath {-} 6.4\ ifmmode\ times\ else\ texttimes\fi {}{ 10 }^{\ ensuremath {-} 6 }<{ a }_{ C }^{ W }/{\ mathrm {\ ensuremathrm {\ Lambda }}}^{ 2 <\ ensuremode {-}\ times\ else\ texttimes\\ ftimes ^{ 10 }^{\ ensuremath {-}-}-}-{\ ensuremath {-}{ 6 }{ a }^{ C }^{ C }^{ W }/{ W }/ mathrm {\ ensuremath {\ lambda }}}}^{{{{\ endmath {-}}}}}{{\ endmath {\ endmath {-}}{-}{{{\ endmath {-}}{{{{{{\ endmath }}}}}}{{{\ endmath {-}}{{{{{{{\ endmath }}}}{{{{{\ endmath {-}}}{{{{{{{{\ endmath }}}}}}}{{{{{\ endmath }}{{{{{{{{{\ endmath }}}}}{{\ endmath }}{{\ endmath {{{{{{{\ endmath }}}}{{{{{{{{\ endmath }}}}}}}}{{{{{{{{{{\{{\{\ تم تعيين الحد الأعلى لمستوى الثقة بنسبة 95 ٪ على إجمالي المقطع العرضي للإنتاج لبوزون هيغز الحصري على 1.2 رطل.Translated Description (French)
Les recherches de paires de bosons $W$ produites exclusivement dans le processus $pp(\ ensuremath {\gamma}\ ensuremath {\gamma})\ ensuremath {\rightarrow}p{W}^{+}{W}^{\ ensuremath {-}}p$ et d'un boson de Higgs produit exclusivement dans le processus $pp(gg)\ ensuremath {\rightarrow} pHp $ ont été effectuées en utilisant ${e} ^{\ ifmmode\ pm\ else\ textpm\fi{}}{\ ensuremath {\mu}}^{\ ensuremath {\mp}}$ états finaux. Ces mesures utilisent $ 20.2\text{ }\text{ }{\mathrm{fb}}^{\ ensuremath {-}1}$ de $pp$ collisions collectées par l'expérience ATLAS à une énergie de centre de masse $ \sqrt{s}=8\text{ }\text{ }\mathrm{TeV}$ au LHC. Une production exclusive de ${W}^{+}{W}^{\ensuremath{-}}$ conforme à la prédiction du modèle standard est trouvée avec une signification de $ 3.0\ ensuremath {\sigma}$ . La section efficace de production exclusive ${W}^{+} {W} ^ {\ ensuremath {-}}$ est déterminée comme étant $ \ ensuremath {\sigma}(\ ensuremath {\gamma}\ ensuremath {\gamma}\ ensuremath {\rightarrow}{W}^{+}{W}^{\ ensuremath {-}}\ ensuremath {\rightarrow}{e}^{\ ifmmode\pm\else\ textpm\fi{}}{\ ensuremath {\mu}}^{\ ensuremath {\mp}}X)=6,9\ ifmmode\pm\else\ textpm\fi{}2,2(\mathrm{stat})\ ifmmode\pm\else\ textpm\fi{}1,4(\mathrm{sys})\text{ }\text{ }\mathrm{fb}$ , en accord avec la prévision du modèle standard. Les limites sur les couplages de jauges quartiques anormaux sont fixées à un niveau de confiance de 95 % comme suit : $ \ ensuremath {-}1,7\ ifmmode\ times\ else\ texttimes\ fi {} {10} ^ {\ ensuremath {-} 6} < {a}_{0} ^ {W}/{\mathrm {\ ensuremath {\ Lambda}}} ^ {2} <1,7\ ifmmode\ times\ else\ texttimes\ fi {} {10} ^ {\ ensuremath {-} 6}\ text {}\ text {} {\ mathrm {GeV}} ^ {\ ensuremath {-} 2} $ et $ \ ensuremath {-} 6,4\ ifmmode\ times\ else\ texttimes\ fi {} {10} ^ {\ ensuremath {-} 6} < {a}_{C} ^ {W}/{\mathrm {\ ensuremath {\ Lambda}}} ^ {2} <6,3\ ifmmode\ times\ else\ texttimes\ fi {} {10} ^ {\ ensuremath {-} 6}\ text {\mathrm {GeV}^ {-}2}$ . Une limite supérieure de niveau de confiance à 95 % sur la section efficace de production totale pour un boson de Higgs exclusif est fixée à 1,2 pb.Translated Description (Spanish)
Las búsquedas de pares de bosones $W$ producidos exclusivamente en el proceso $pp(\ ensuremath {\gamma}\ ensuremath {\gamma})\ ensuremath {\rightarrow}p{W}^{+}{W}^{\ ensuremath {-}}p$ y un bosón de Higgs producido exclusivamente en el proceso $pp(gg)\ ensuremath {\rightarrow} pHp $ se han realizado utilizando ${e} ^{\ ifmmode\pm\else\ textpm\fi{}}{\ ensuremath {\mu}}^{\ ensuremath {\mp}}$ estados finales. Estas mediciones utilizan $ 20.2\text{ }\text{ }{\mathrm{fb}}^{\ ensuremath {-}1}$ de $ pp$ colisiones recogidas por el experimento ATLAS en un centro de energía de masa $\sqrt{s}=8\text{ }\text{ }\mathrm{TeV}$ en el LHC. La producción exclusiva de${W} ^{+}{W}^{\ensuremath{-}}$ consistente con la predicción del Modelo Estándar se encuentra con $ 3.0\ensuremath{\sigma}$ de importancia. La sección transversal de producción exclusiva de ${W} ^{+} {W} ^ {\ ensuremath {-}} $ se determina como $\ ensuremath {\sigma}(\ ensuremath {\gamma}\ ensuremath {\gamma}\ ensuremath {\rightarrow}{W}^{+}{W}^{\ ensuremath {-}}\ ensuremath {\rightarrow}{e}^{\ ifmmode\pm\else\ textpm\fi{}}{\ ensuremath {\mu}}^{\ ensuremath {\mp}}X)=6.9\ ifmmode\pm\else\ textpm\fi{}2.2(\mathrm{stat})\ ifmmode\pm\else\ textpm\fi{}1.4(\mathrm{sys})\text{ }\text{ }\mathrm{fb}$, de acuerdo con la predicción del modelo estándar. Los límites de los acoplamientos de calibre cuártico anómalos se establecen en un nivel de confianza del 95% como $\ ensuremath {-}1.7\ ifmmode\ times\ else\ texttimes\ fi{} {10} ^ {\ ensuremath {-} 6} < {a}_{0} ^ {W}/{\mathrm {\ ensuremath {\ Lambda}}} ^{2}<1.7\ ifmmode\ times\ else\ texttimes\ fi{} {10} ^ {\ ensuremath {-} 6}\text{ }\ text {} {\ mathrm {GeV}} ^ {\ ensuremath {-} 2} $ y $\ ensuremath {-}6.4\ ifmmode\ times\ else\ texttimes\ fi{} {10} ^ {\ ensuremath {-} 6} < {a}_{C} ^ {W}/{\mathrm {\ ensuremath {\ Lambda}} ^{2}<6.3\ ifmmode\ times\ else\ texttimes\ fi{} {10} ^ {\ ensuremath {- 6}\text{ }{\ mathmath {\ geV}}^{\ ensuremath {- 2}$. Un límite superior de nivel de confianza del 95% en la sección transversal de producción total para un bosón de Higgs exclusivo se establece en 1,2 pb.Files
PhysRevD.94.032011.pdf
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Additional details
Additional titles
- Translated title (Arabic)
- قياس الإنتاج الحصري لـ<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>γ</mml:mi><mml:mi>γ</mml:mi><mml:mo stretchy="false">→</mml:mo><mml:msup><mml:mi>W</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mi>W</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:math> والبحث عن إنتاج بوزون هيغز الحصري في تصادمات<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi> p</mml:mi><mml:mi>p</mml:mi></mml:math> عند<mml:math ...
- Translated title (French)
- Mesure de la production exclusive de<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi> γ</mml:mi><mml:mi>γ</mml:mi><mml:mo stretchy="false">→</mml:mo><mml:msup><mml:mi>W</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mi>W</mml:mi><mml:mo>−</mml:mo></mml:msup></mml:math> et recherche de la production exclusive du boson de Higgs dans les collisions<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi> p</mml:mi><mml:mi>p</mml:mi></mml:math> à<mml :math …
- Translated title (Spanish)
- Medición de la producción exclusiva<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>γ</mml:mi><mml:mi>γ</mml:mi><mml:mo stretchy="false">→</mml:mo><mml:msup><mml:mi>W</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mi>W</mml:mi><mml:mo>−</mml:mo></mml:msup></mml:math> y búsqueda de la producción exclusiva del bosón de Higgs en<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>p</mml:mi><mml:mi>p</mml:mi></mml:math>colisiones a<mml:matemáticas ...
Identifiers
- Other
- https://openalex.org/W2508726494
- DOI
- 10.1103/physrevd.94.032011
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