Combined effective field theory interpretation of Higgs boson, electroweak vector boson, top quark, and multijet measurements

CMS Collaboration

doi:10.1140/epjc/s10052-025-14997-y

Combined effective field theory interpretation of Higgs boson, electroweak vector boson, top quark, and multijet measurements

CMS Collaboration

European Organization for Nuclear Research
California Institute of Technology
Institute of Nuclear Physics of the Uzbekistan Academy of Sciences
University of Louvain
Yerevan Physics Institute
Imperial College London
University of Wisconsin-Madison
Wayne State University
University of Virginia
Vanderbilt University
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Horia Hulubei National Institute of Physics and Nuclear Engineering
Johns Hopkins University
University of Iowa
Erciyes University
Sinop University
Georgian Technical University
Bingol University
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Florida Institute of Technology
Ain Shams University
Florida State University
University of Florida
Fermi National Accelerator Laboratory
The United States Naval Academy
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Carnegie Mellon University
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University of California, Riverside
University of California, Los Angeles
University of California, Davis
Women and Infants Hospital of Rhode Island-Warren Alpert Medical School of Brown University
Karamanoğlu Mehmetbey University
Bethel University
Boston University
University of Alabama
University of Turin
Catholic University of America
Baylor University
Brunel University London
Monash University
CCLRC Rutherford Appleton Laboratory
University of Southampton
University of Bristol
Kharkov Institute of Physics and Technology
Academy of Science of Ukraine
Yildiz Technical University
Istinye University
Istanbul University
Istanbul University — Cerrahpasa
Erzincan University
Istanbul Technical University
Hacettepe University
Near East University
stanbul Okan University
Bogazici University
Kafkas University
Milli Savunma University
Marmara University
Middle East Technical University (METU)
Bozok Universitesi Rektörlügü
Cukurova University
Adiyaman University
Izmir Bakircay University
Konya Technical University
University of Tunis El Manar
Chulalongkorn University
National Taiwan University
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Indian Institute of Science
Université Paris-Sud
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ETH Zurich
ENAC-IIC-GEL
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Eastern University, Sri Lanka
CSIC-Univ. Cantabria
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Universidad Autónoma de Madrid
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University of Belgrade
University of Belgrade
Lisboa
Warsaw University of Technology
University of Warsaw
National Centre for Nuclear Research
Agh University of Science and Technology Faculty of Computer Science
Quaid-i-Azam University
University of Canterbury
University of Montenegro
Benemerita Universidad Autonoma de Puebla
Universidad Iberoamericana
CINVESTAV-IPN
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Universidad de Sonora
University Malaya
Universiti Kebangsaan Malaysia
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Riga Technical University
Kuwait University
American University of the Middle East
Sungkyunkwan University
Yonsei University
University of Seoul
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Sejong University
Kyung Hee University
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Institut de Physique des 2 Infinis de Lyon
Chonnam National University
Kangwon National University
Kyungpook National University
University of Trieste
University of Rome
University of Pisa
University of Perugia
Ev-K2-CNR Committee
University of Pavia
University of Padova
Luleå University of Technology
University of Naples Federico II
University of Milano-Bicocca
University of Genoa
LNF-INFN
Università degli Studi Guglielmo Marconi
University of Florence
Università degli Studi di Catania
CSFNSM
University of Bologna
ENEA Climate Modeling and Impacts
Università degli studi di Bari Aldo Moro
Helwan University
University College Dublin
Institute for Research in Fundamental Sciences (IPM)
Arak University
University of Science and Technology of Mazandaran, Behshahr
Isfahan University of Technology
Sharif University of Technology
c/o DESY
Indian Institute of Science Education and Research (IISER)
University of Hyderabad
An OCC of Homi Bhabha National Institute
Institute of Physics Bhubaneswar
IIT Bhubaneswar
Tata Institute of Fundamental Research, Mumbai
UPES — University of Petroleum and Energy Studies
Indian Institute of Technology Madras
Amity University
Saha Institute of Nuclear Physics
University of Visva-Bharati
Indian Institute of Technology Kanpur
University of Delhi
Panjab University
Punjab Agricultural University
Eszterhazy Karoly University
Wigner Research Centre for Physics
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Eötvös Loránd University
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National Technical University of Athens
NCSR Demokritos
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Universität Hamburg
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Bergische Universität Gesamthochschule Wuppertal
Research Centre Julich
The University of the State of Amazonas
Université de Strasbourg
Université de Haute Alsace
Ip Paris
Université Paris-Saclay
LUT University
Helsinki Institute of Physics
University of Helsinki
National Institute of Chemical Physics and Biophysics, Tallinn
Fayoum University
Egyptian Network of High Energy Physics
Cairo University
British University in Egypt
Zewail City of Science and Technology
Universidad San Francisco de Quito
Escuela Politecnica Nacional
Charles University
University of Cyprus
Ruđer Bošković Institute
Faculty of Science, University of Split
Faculty of Electrical Engineering, Mechanical Engineering and Naval Architecture, University of Split
Universidad de Antioquia
Universidad de Los Andes, Colombia
Zhejiang University
Institute of Modern Physics Chinese Academy of Sciences
Nanjing Normal University
University of Shanghai for Science and Technology
Henan Normal University
University of Science and Technology of China
Sun Yat-Sen University
South China Normal University
State Key Laboratory of Nuclear Physics and Technology
Institute of High Energy Physics, Chinese Academy of Sciences
University of Chinese Academy of Sciences
China Spallation Neutron Source
China Center of Advanced Science and Technology World Laboratory
Tsinghua University
Beihang University
Universidad de Tarapacá
University of Sofia
Institute for Nuclear Research and Nuclear Energy Bulgarian Academy of Sciences
São Paulo State University
Universidade Federal do Rio Grande do Sul
Rua São Francisco de Xavier
University of Campinas (UNICAMP)
Centro Brasileiro de Pesquisas Fisicas
FACAMP—Faculdades de Campinas
Ghent University
Université Libre de Bruxelles
Vrjie Universiteit Brussel
University of Antwerp
Institut für Hochenergiephysik
Vienna University of Technology
Yerevan State University

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1 Citation (Scopus)

Résumé

Constraints on Wilson coefficients (WCs) corresponding to dimension-6 operators of the standard model effective field theory (SMEFT) are determined from a simultaneous fit to seven sets of CMS measurements probing Higgs boson, electroweak vector boson, top quark, and multijet production. Measurements of electroweak precision observables are also included and provide complementary constraints to those from the CMS experiment. The CMS measurements, using LHC proton-proton collision data at s=13Te, corresponding to integrated luminosities of 36.3 or 138fb-1, are chosen to provide sensitivity to a broad set of operators, for which consistent SMEFT predictions can be derived. These are primarily measurements of differential cross sections which are parameterized as functions of the WCs. In measurements targeting t(t¯)X production, SMEFT effects are modelled at the detector level. Individual constraints on 64 WCs, and constraints on 43 linear combinations of WCs, are obtained.

langue originale	Anglais
Numéro d'article	331
journal	European Physical Journal C
Volume	86
Numéro de publication	4
Les DOIs	https://doi.org/10.1140/epjc/s10052-025-14997-y
état	Publié - 1 avr. 2026

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10.1140/epjc/s10052-025-14997-y

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@article{e6ec5c7318504f89aa55f940651d408c,

title = "Combined effective field theory interpretation of Higgs boson, electroweak vector boson, top quark, and multijet measurements",

abstract = "Constraints on Wilson coefficients (WCs) corresponding to dimension-6 operators of the standard model effective field theory (SMEFT) are determined from a simultaneous fit to seven sets of CMS measurements probing Higgs boson, electroweak vector boson, top quark, and multijet production. Measurements of electroweak precision observables are also included and provide complementary constraints to those from the CMS experiment. The CMS measurements, using LHC proton-proton collision data at s=13Te, corresponding to integrated luminosities of 36.3 or 138fb-1, are chosen to provide sensitivity to a broad set of operators, for which consistent SMEFT predictions can be derived. These are primarily measurements of differential cross sections which are parameterized as functions of the WCs. In measurements targeting t(t¯)X production, SMEFT effects are modelled at the detector level. Individual constraints on 64 WCs, and constraints on 43 linear combinations of WCs, are obtained.",

author = "CMS Collaboration and V. Borshch and A. Babaev and A. Uzunian and S. Slabospitskii and V. Kachanov and V. Blinov and A. Snigirev and V. Savrin and M. Dubinin and V. Bunichev and E. Boos and A. Terkulov and M. Kirakosyan and M. Azarkin and V. Andreev and A. Zhokin and V. Popov and N. Lychkovskaya and V. Gavrilov and D. Kirpichnikov and N. Golubev and A. Dermenev and A. Vorobyev and L. Uvarov and Y. Ivanov and V. Golovtcov and G. Gavrilov and I. Zhizhin and A. Zarubin and Yuldashev, \{B. S.\} and N. Voytishin and A. Toropin and I. Tlisova and O. Teryaev and V. Smirnov and Y. Skovpen and S. Shulha and S. Shmatov and V. Shalaev and A. Zghiche and A. Zabi and Y. Sirois and C. Ochando and M. Nguyen and \{Granier de Cassagnac\}, R. and \{De Wit\}, A. and O. Davignon and G. Boldrini and F. Beaudette and A. Cappati",

note = "Publisher Copyright: {\textcopyright} CERN for the benefit of the CMS Collaboration 2026.",

year = "2026",

month = apr,

day = "1",

doi = "10.1140/epjc/s10052-025-14997-y",

language = "English",

volume = "86",

journal = "European Physical Journal C",

issn = "1434-6044",

publisher = "Springer Nature",

number = "4",

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TY - JOUR

T1 - Combined effective field theory interpretation of Higgs boson, electroweak vector boson, top quark, and multijet measurements

AU - CMS Collaboration

AU - Borshch, V.

AU - Babaev, A.

AU - Uzunian, A.

AU - Slabospitskii, S.

AU - Kachanov, V.

AU - Blinov, V.

AU - Snigirev, A.

AU - Savrin, V.

AU - Dubinin, M.

AU - Bunichev, V.

AU - Boos, E.

AU - Terkulov, A.

AU - Kirakosyan, M.

AU - Azarkin, M.

AU - Andreev, V.

AU - Zhokin, A.

AU - Popov, V.

AU - Lychkovskaya, N.

AU - Gavrilov, V.

AU - Kirpichnikov, D.

AU - Golubev, N.

AU - Dermenev, A.

AU - Vorobyev, A.

AU - Uvarov, L.

AU - Ivanov, Y.

AU - Golovtcov, V.

AU - Gavrilov, G.

AU - Zhizhin, I.

AU - Zarubin, A.

AU - Yuldashev, B. S.

AU - Voytishin, N.

AU - Toropin, A.

AU - Tlisova, I.

AU - Teryaev, O.

AU - Smirnov, V.

AU - Skovpen, Y.

AU - Shulha, S.

AU - Shmatov, S.

AU - Shalaev, V.

AU - Zghiche, A.

AU - Zabi, A.

AU - Sirois, Y.

AU - Ochando, C.

AU - Nguyen, M.

AU - Granier de Cassagnac, R.

AU - De Wit, A.

AU - Davignon, O.

AU - Boldrini, G.

AU - Beaudette, F.

AU - Cappati, A.

PY - 2026/4/1

Y1 - 2026/4/1

N2 - Constraints on Wilson coefficients (WCs) corresponding to dimension-6 operators of the standard model effective field theory (SMEFT) are determined from a simultaneous fit to seven sets of CMS measurements probing Higgs boson, electroweak vector boson, top quark, and multijet production. Measurements of electroweak precision observables are also included and provide complementary constraints to those from the CMS experiment. The CMS measurements, using LHC proton-proton collision data at s=13Te, corresponding to integrated luminosities of 36.3 or 138fb-1, are chosen to provide sensitivity to a broad set of operators, for which consistent SMEFT predictions can be derived. These are primarily measurements of differential cross sections which are parameterized as functions of the WCs. In measurements targeting t(t¯)X production, SMEFT effects are modelled at the detector level. Individual constraints on 64 WCs, and constraints on 43 linear combinations of WCs, are obtained.

AB - Constraints on Wilson coefficients (WCs) corresponding to dimension-6 operators of the standard model effective field theory (SMEFT) are determined from a simultaneous fit to seven sets of CMS measurements probing Higgs boson, electroweak vector boson, top quark, and multijet production. Measurements of electroweak precision observables are also included and provide complementary constraints to those from the CMS experiment. The CMS measurements, using LHC proton-proton collision data at s=13Te, corresponding to integrated luminosities of 36.3 or 138fb-1, are chosen to provide sensitivity to a broad set of operators, for which consistent SMEFT predictions can be derived. These are primarily measurements of differential cross sections which are parameterized as functions of the WCs. In measurements targeting t(t¯)X production, SMEFT effects are modelled at the detector level. Individual constraints on 64 WCs, and constraints on 43 linear combinations of WCs, are obtained.

UR - https://www.scopus.com/pages/publications/105040702882

U2 - 10.1140/epjc/s10052-025-14997-y

DO - 10.1140/epjc/s10052-025-14997-y

M3 - Article

AN - SCOPUS:105040702882

SN - 1434-6044

VL - 86

JO - European Physical Journal C

JF - European Physical Journal C

IS - 4

M1 - 331

ER -

Combined effective field theory interpretation of Higgs boson, electroweak vector boson, top quark, and multijet measurements

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