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The measurements of the inclusive and differential fiducial cross sections of the Higgs boson decaying to a pair of photons are presented. The analysis is performed using proton-proton collisions data recorded with the CMS detector at the LHC at a centre-of-mass energy of 13TeV and corresponding to an integrated luminosity of 137 fb(-1). The inclusive fiducial cross section is measured to be sigma(fid) = 73.4(-5.3)(+5.4)(stat)(+2.4)(-2.2)(syst) fb, in agreement with the standard model expectation of 75.4 +/- 4.1 fb. The measurements are also performed in fiducial regions targeting different production modes and as function of several observables describing the diphoton system, the number of additional jets present in the event, and other kinematic observables. Two double differential measurements are performed. No significant deviations from the standard model expectations are observed.
A. Tumasyan, W. Adam, J. W. Andrejkovic, T. Bergauer, S. Chatterjee, K. Damanakis, et al. (2023). Measurement of the Higgs boson inclusive and differential fiducial production cross sections in the diphoton decay channel with pp collisions at $$ \sqrt{s} $$ = 13 TeV. JOURNAL OF HIGH ENERGY PHYSICS, 2023(7), 0-65 [10.1007/jhep07(2023)091].
Measurement of the Higgs boson inclusive and differential fiducial production cross sections in the diphoton decay channel with pp collisions at $$ \sqrt{s} $$ = 13 TeV
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Royon;R. Salvatico;S. Sanders;E. Schmitz;C. Smith;Q. Wang;J. Williams;G. Wilson;B. Allmond;S. Duric;R. Gujju Gurunadha;A. Ivanov;K. Kaadze;D. Kim;Y. Maravin;T. Mitchell;A. Modak;K. Nam;J. Natoli;D. Roy;F. Rebassoo;D. Wright;E. Adams;A. Baden;O. Baron;A. Belloni;A. Bethani;S. C. Eno;N. J. Hadley;S. Jabeen;R. G. Kellogg;T. Koeth;Y. Lai;S. Lascio;A. C. Mignerey;S. Nabili;C. Palmer;C. Papageorgakis;M. Seidel;L. Wang;K. Wong;D. Abercrombie;R. Bi;W. Busza;I. A. Cali;Y. Chen;M. D???Alfonso;J. Eysermans;C. Freer;G. Gomez-Ceballos;M. Goncharov;P. Harris;M. Hu;D. Kovalskyi;J. Krupa;Y. -J. Lee;K. Long;C. Mironov;C. Paus;D. Rankin;C. Roland;G. Roland;Z. Shi;G. S. F. Stephans;J. Wang;Z. Wang;B. Wyslouch;R. M. Chatterjee;B. Crossman;A. Evans;J. Hiltbrand;Sh. Jain;B. M. Joshi;C. Kapsiak;M. Krohn;Y. Kubota;J. Mans;M. Revering;R. Rusack;R. Saradhy;N. Schroeder;N. Strobbe;M. A. Wadud;L. M. Cremaldi;K. Bloom;M. Bryson;D. R. Claes;C. Fangmeier;L. Finco;F. Golf;C. Joo;I. Kravchenko;I. Reed;J. E. Siado;G. R. Snow;W. Tabb;A. Wightman;F. Yan;A. G. Zecchinelli;G. Agarwal;H. Bandyopadhyay;L. Hay;I. Iashvili;A. Kharchilava;C. McLean;M. Morris;D. Nguyen;J. Pekkanen;S. Rappoccio;A. Williams;G. Alverson;E. Barberis;Y. Haddad;Y. Han;A. Krishna;J. Li;J. Lidrych;G. Madigan;B. Marzocchi;D. M. Morse;V. Nguyen;T. Orimoto;A. Parker;L. Skinnari;A. Tishelman-Charny;T. Wamorkar;B. Wang;A. Wisecarver;D. Wood;S. Bhattacharya;J. Bueghly;Z. Chen;A. Gilbert;T. Gunter;K. A. Hahn;Y. Liu;N. Odell;M. H. Schmitt;M. Velasco;R. Band;R. Bucci;S. Castells;M. Cremonesi;A. Das;R. Goldouzian;M. Hildreth;K. Hurtado Anampa;C. Jessop;K. Lannon;J. Lawrence;N. Loukas;L. Lutton;J. Mariano;N. Marinelli;I. Mcalister;T. McCauley;C. Mcgrady;K. Mohrman;C. Moore;Y. Musienko;H. Nelson;R. Ruchti;A. Townsend;M. Wayne;H. Yockey;M. Zarucki;L. Zygala;B. Bylsma;M. Carrigan;L. S. Durkin;B. Francis;C. Hill;A. Lesauvage;M. Nunez Ornelas;K. Wei;B. L. Winer;B. R. Yates;F. M. Addesa;B. Bonham;P. Das;G. Dezoort;P. Elmer;A. Frankenthal;B. Greenberg;N. Haubrich;S. Higginbotham;A. Kalogeropoulos;G. Kopp;S. Kwan;D. Lange;D. Marlow;K. Mei;I. Ojalvo;J. Olsen;D. Stickland;C. Tully;S. Malik;S. Norberg;A. S. Bakshi;V. E. Barnes;R. Chawla;S. Das;L. Gutay;M. Jones;A. W. Jung;D. Kondratyev;A. M. Koshy;M. Liu;G. Negro;N. Neumeister;G. Paspalaki;S. Piperov;A. Purohit;J. F. Schulte;M. Stojanovic;J. Thieman;F. Wang;R. Xiao;W. Xie;J. Dolen;N. Parashar;D. Acosta;A. Baty;T. Carnahan;M. Decaro;S. Dildick;K. M. Ecklund;P. J. Fern??ndez Manteca;S. Freed;P. Gardner;F. J. M. Geurts;A. Kumar;W. Li;B. P. Padley;R. Redjimi;J. Rotter;W. Shi;S. Yang;E. Yigitbasi;L. Zhang;Y. Zhang;X. Zuo;A. Bodek;P. de Barbaro;R. Demina;J. L. Dulemba;C. Fallon;T. Ferbel;M. Galanti;A. Garcia-Bellido;O. Hindrichs;A. Khukhunaishvili;E. Ranken;R. Taus;G. P. Van Onsem;K. Goulianos;B. Chiarito;J. P. Chou;Y. Gershtein;E. Halkiadakis;A. Hart;M. Heindl;D. Jaroslawski;O. Karacheban;I. Laflotte;A. Lath;R. Montalvo;K. Nash;M. Osherson;S. Salur;S. Schnetzer;S. Somalwar;R. 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Belyaev;V. Blinov;E. Boos;V. Borshch;D. Budkouski;O. Bychkova;V. Chekhovsky;R. Chistov;M. Danilov;A. Dermenev;T. Dimova;I. Dremin;M. Dubinin;L. Dudko;V. Epshteyn;A. Ershov;G. Gavrilov;V. Gavrilov;S. Gninenko;V. Golovtcov;N. Golubev;I. Golutvin;I. Gorbunov;A. Gribushin;V. Ivanchenko;Y. Ivanov;V. Kachanov;L. Kardapoltsev;V. Karjavine;A. Karneyeu;V. Kim;M. Kirakosyan;D. Kirpichnikov;M. Kirsanov;V. Klyukhin;O. Kodolova;D. Konstantinov;V. Korenkov;A. Kozyrev;N. Krasnikov;E. Kuznetsova;A. Lanev;P. Levchenko;A. Litomin;N. Lychkovskaya;V. Makarenko;A. Malakhov;V. Matveev;V. Murzin;A. Nikitenko;S. Obraztsov;V. Okhotnikov;I. Ovtin;V. Palichik;P. Parygin;V. Perelygin;S. Petrushanko;G. Pivovarov;S. Polikarpov;V. Popov;O. Radchenko;M. Savina;V. Savrin;D. Selivanova;V. Shalaev;S. Shmatov;S. Shulha;Y. Skovpen;S. Slabospitskii;V. Smirnov;A. Snigirev;D. Sosnov;A. Stepennov;V. Sulimov;E. Tcherniaev;A. Terkulov;O. Teryaev;I. Tlisova;M. Toms;A. Toropin;L. Uvarov;A. Uzunian;E. Vlasov;A. Vorobyev;N. Voytishin;B. S. Yuldashev;A. Zarubin;I. Zhizhin;A. Zhokin
2023
Abstract
The measurements of the inclusive and differential fiducial cross sections of the Higgs boson decaying to a pair of photons are presented. The analysis is performed using proton-proton collisions data recorded with the CMS detector at the LHC at a centre-of-mass energy of 13TeV and corresponding to an integrated luminosity of 137 fb(-1). The inclusive fiducial cross section is measured to be sigma(fid) = 73.4(-5.3)(+5.4)(stat)(+2.4)(-2.2)(syst) fb, in agreement with the standard model expectation of 75.4 +/- 4.1 fb. The measurements are also performed in fiducial regions targeting different production modes and as function of several observables describing the diphoton system, the number of additional jets present in the event, and other kinematic observables. Two double differential measurements are performed. No significant deviations from the standard model expectations are observed.
A. Tumasyan, W. Adam, J. W. Andrejkovic, T. Bergauer, S. Chatterjee, K. Damanakis, et al. (2023). Measurement of the Higgs boson inclusive and differential fiducial production cross sections in the diphoton decay channel with pp collisions at $$ \sqrt{s} $$ = 13 TeV. JOURNAL OF HIGH ENERGY PHYSICS, 2023(7), 0-65 [10.1007/jhep07(2023)091].
A. Tumasyan; W. Adam; J. W. Andrejkovic; T. Bergauer; S. Chatterjee; K. Damanakis; M. Dragicevic; A. Escalante Del Valle; P. S. Hussain; M. Jeitler; N...espandi
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11585/953578
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simulazione ASN
Il report seguente simula gli indicatori relativi alla propria produzione scientifica in relazione alle soglie ASN 2023-2025 del proprio SC/SSD. Si ricorda che il superamento dei valori soglia (almeno 2 su 3) è requisito necessario ma non sufficiente al conseguimento dell'abilitazione. La simulazione si basa sui dati IRIS e sugli indicatori bibliometrici alla data indicata e non tiene conto di eventuali periodi di congedo obbligatorio, che in sede di domanda ASN danno diritto a incrementi percentuali dei valori. La simulazione può differire dall'esito di un’eventuale domanda ASN sia per errori di catalogazione e/o dati mancanti in IRIS, sia per la variabilità dei dati bibliometrici nel tempo. Si consideri che Anvur calcola i valori degli indicatori all'ultima data utile per la presentazione delle domande.
La presente simulazione è stata realizzata sulla base delle specifiche raccolte sul tavolo ER del Focus Group IRIS coordinato dall’Università di Modena e Reggio Emilia e delle regole riportate nel DM 589/2018 e allegata Tabella A. Cineca, l’Università di Modena e Reggio Emilia e il Focus Group IRIS non si assumono alcuna responsabilità in merito all’uso che il diretto interessato o terzi faranno della simulazione. Si specifica inoltre che la simulazione contiene calcoli effettuati con dati e algoritmi di pubblico dominio e deve quindi essere considerata come un mero ausilio al calcolo svolgibile manualmente o con strumenti equivalenti.