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There are two canonical approaches to treating the Standard Model as an Effective Field Theory (EFT): Standard Model EFT (SMEFT), expressed in the electroweak symmetric phase utilizing the Higgs doublet, and Higgs EFT (HEFT), expressed in…

High Energy Physics - Phenomenology · Physics 2021-08-11 Timothy Cohen , Nathaniel Craig , Xiaochuan Lu , Dave Sutherland

This note gives an overview of the tools for the precision matching of ultraviolet theories to the Standard Model effective field theory (SMEFT) at the tree level and one loop. Several semi- and fully automated codes are presented, as well…

Truncations of effective field theory expansions are technically necessary but inherently intertwined with the redundancies of general field redefinitions. This can be viewed as a juxtaposition of power-counting and theoretical…

High Energy Physics - Phenomenology · Physics 2026-03-30 Rodrigo Alonso , Christoph Englert , Wrishik Naskar , Shakeel Ur Rahaman

Gravitational wave (GW) observations offer a promising probe of new physics associated with a first-order electroweak phase transition. Precision studies of the Higgs potential, including Fisher matrix analyses, have been extensively…

High Energy Physics - Phenomenology · Physics 2025-09-11 Katsuya Hashino , Daiki Ueda

We write down a geometric realization of the Standard Model Effective Field Theory (SMEFT) extended by $n_f$ flavours of light sterile neutrinos, a so-called geo$\nu$SMEFT. As with the geoSMEFT introduced by Helset, Martin and Trott, we…

High Energy Physics - Phenomenology · Physics 2023-08-22 Jim Talbert

New physics interactions beyond the Standard Model can make themselves known as small corrections to Standard Model reactions. There is a diverse array of proposals for new physics, and so any parametrization of those effects must be as…

High Energy Physics - Phenomenology · Physics 2020-03-12 Michael E. Peskin

We present the Standard Model Effective Field Theories (SMEFT) from purely on-shell arguments. Starting from a few basic assumptions such as Poincar\'e invariance and locality, we classify all the renormalisable and non-renormalisable…

High Energy Physics - Theory · Physics 2022-05-04 Manuel Accettulli Huber , Stefano De Angelis

One of the forthcoming major challenges in particle physics is the experimental determination of the Higgs trilinear self-coupling. While efforts have largely focused on on-shell double- and single-Higgs production in proton-proton…

High Energy Physics - Phenomenology · Physics 2026-05-18 Aishik Ghosh , Maximilian Griese , Ulrich Haisch , Tae Hyoun Park

The Standard Model Effective Field Theory (SMEFT) offers a systematic approach to study potential deviations from the Standard Model (SM) through higher-dimensional operators that encapsulate new physics effects. In this work, we analyze…

High Energy Physics - Phenomenology · Physics 2025-03-06 Luca Mantani , Veronica Sanz

Effective field theories are useful tools to search for physics beyond the Standard Model (SM). However, effective theories can lead to non-unitary behavior with fastly growing amplitudes. This unphysical behavior may lead to large…

High Energy Physics - Phenomenology · Physics 2022-01-19 Iñigo Asiáin , Domènec Espriu , Federico Mescia

We define a set of pseudo-observables characterizing the properties of Higgs decays in generic extensions of the Standard Model with no new particles below the Higgs mass. The pseudo-observables can be determined from experimental data,…

High Energy Physics - Phenomenology · Physics 2015-06-23 Martin Gonzalez-Alonso , Admir Greljo , Gino Isidori , David Marzocca

We analyze the scalar potential of the Simplest Little Higgs (SLH) model in an approach consistent with the spirit of continuum effective field theory (CEFT). By requiring correct electroweak symmetry breaking (EWSB) with the…

High Energy Physics - Phenomenology · Physics 2018-09-12 Kingman Cheung , Shi-Ping He , Ying-nan Mao , Chen Zhang , Yang Zhou

We classify effective field theory (EFT) deformations of the Standard Model (SM) according to the analyticity property of the Lagrangian as a function of the Higgs doublet H. Our distinction in analytic and non-analytic corresponds to the…

High Energy Physics - Phenomenology · Physics 2020-01-08 Adam Falkowski , Riccardo Rattazzi

We compute the two-loop contributions to Higgs production via gluon-gluon fusion ($gg \to h$) and Higgs decay into two photons ($h \to \gamma\gamma$), arising from third-generation four-quark operators in the Standard Model effective field…

High Energy Physics - Phenomenology · Physics 2025-07-29 Ulrich Haisch , Marco Niggetiedt

We treat the Standard Model as the low-energy limit of an effective field theory that incorporates higher-dimensional operators to capture the effects of decoupled new physics. We consider the constraints imposed on the coefficients of…

High Energy Physics - Phenomenology · Physics 2014-10-29 John Ellis , Veronica Sanz , Tevong You

The Standard Model Effective Field Theory (SMEFT) based on the unbroken gauge group $\text{SU(3)}_C\otimes\text{SU(2)}_L\otimes\text{U(1)}_Y$ and containing only particles of the Standard Model (SM) has developed in the last decade to a…

High Energy Physics - Phenomenology · Physics 2025-11-13 Jason Aebischer , Andrzej J. Buras , Jacky Kumar

This Report summarizes the results of the activities of the LHC Higgs Cross Section Working Group in the period 2014-2016. The main goal of the working group was to present the state-of-the-art of Higgs physics at the LHC, integrating all…

High Energy Physics - Phenomenology · Physics 2017-05-16 D. de Florian , C. Grojean , F. Maltoni , C. Mariotti , A. Nikitenko , M. Pieri , P. Savard , M. Schumacher , R. Tanaka , R. Aggleton , M. Ahmad , B. Allanach , C. Anastasiou , W. Astill , S. Badger , M. Badziak , J. Baglio , E. Bagnaschi , A. Ballestrero , A. Banfi , D. Barducci , M. Beckingham , C. Becot , G. Bélanger , J. Bellm , N. Belyaev , F. U. Bernlochner , C. Beskidt , A. Biekötter , F. Bishara , W. Bizon , N. E. Bomark , M. Bonvini , S. Borowka , V. Bortolotto , S. Boselli , F. J. Botella , R. Boughezal , G. C. Branco , J. Brehmer , L. Brenner , S. Bressler , I. Brivio , A. Broggio , H. Brun , G. Buchalla , C. D. Burgard , A. Calandri , L. Caminada , R. Caminal Armadans , F. Campanario , J. Campbell , F. Caola , C. M. Carloni Calame , S. Carrazza , A. Carvalho , M. Casolino , O. Cata , A. Celis , F. Cerutti , N. Chanon , M. Chen , X. Chen , B. Chokoufé Nejad , N. Christensen , M. Ciuchini , R. Contino , T. Corbett , R. Costa , D. Curtin , M. Dall'Osso , A. David , S. Dawson , J. de Blas , W. de Boer , P. de Castro Manzano , C. Degrande , R. L. Delgado , F. Demartin , A. Denner , B. Di Micco , R. Di Nardo , S. Dittmaier , A. Dobado , T. Dorigo , F. A. Dreyer , M. Dührssen , C. Duhr , F. Dulat , K. Ecker , K. Ellis , U. Ellwanger , C. Englert , D. Espriu , A. Falkowski , L. Fayard , R. Feger , G. Ferrera , A. Ferroglia , N. Fidanza , T. Figy , M. Flechl , D. Fontes , S. Forte , P. Francavilla , E. Franco , R. Frederix , A. Freitas , F. F. Freitas , F. Frensch , S. Frixione , B. Fuks , E. Furlan , S. Gadatsch , J. Gao , Y. Gao , M. V. Garzelli , T. Gehrmann , R. Gerosa , M. Ghezzi , D. Ghosh , S. Gieseke , D. Gillberg , G. F. Giudice , E. W. N. Glover , F. Goertz , D. Gonçalves , J. Gonzalez-Fraile , M. Gorbahn , S. Gori , C. A. Gottardo , M. Gouzevitch , P. Govoni , D. Gray , M. Grazzini , N. Greiner , A. Greljo , J. Grigo , A. V. Gritsan , R. Gröber , S. Guindon , H. E. Haber , C. Han , T. Han , R. Harlander , M. A. Harrendorf , H. B. Hartanto , C. Hays , S. Heinemeyer , G. Heinrich , M. Herrero , F. Herzog , B. Hespel , V. Hirschi , S. Hoeche , S. Honeywell , S. J. Huber , C. Hugonie , J. Huston , A. Ilnicka , G. Isidori , B. Jäger , M. Jaquier , S. P. Jones , A. Juste , S. Kallweit , A. Kaluza , A. Kardos , A. Karlberg , Z. Kassabov , N. Kauer , D. I. Kazakov , M. Kerner , W. Kilian , F. Kling , K. Köneke , R. Kogler , R. Konoplich , S. Kortner , S. Kraml , C. Krause , F. Krauss , M. Krawczyk , A. Kulesza , S. Kuttimalai , R. Lane , A. Lazopoulos , G. Lee , P. Lenzi , I. M. Lewis , Y. Li , S. Liebler , J. Lindert , X. Liu , Z. Liu , F. J. Llanes-Estrada , H. E. Logan , D. Lopez-Val , I. Low , G. Luisoni , P. Maierhöfer , E. Maina , B. Mansoulié , H. Mantler , M. Mantoani , A. C. Marini , V. I. Martinez Outschoorn , S. Marzani , D. Marzocca , A. Massironi , K. Mawatari , J. Mazzitelli , A. McCarn , B. Mellado , K. Melnikov , S. B. Menari , L. Merlo , C. Meyer , P. Milenovic , K. Mimasu , S. Mishima , B. Mistlberger , S. -O. Moch , A. Mohammadi , P. F. Monni , G. Montagna , M. Moreno Llácer , N. Moretti , S. Moretti , L. Motyka , A. Mück , M. Mühlleitner , S. Munir , P. Musella , P. Nadolsky , D. Napoletano , M. Nebot , C. Neu , M. Neubert , R. Nevzorov , O. Nicrosini , J. Nielsen , K. Nikolopoulos , J. M. No , C. O'Brien , T. Ohl , C. Oleari , T. Orimoto , D. Pagani , C. E. Pandini , A. Papaefstathiou , A. S. Papanastasiou , G. Passarino , B. D. Pecjak , M. Pelliccioni , G. Perez , L. Perrozzi , F. Petriello , G. Petrucciani , E. Pianori , F. Piccinini , M. Pierini , A. Pilkington , S. Plätzer , T. Plehn , R. Podskubka , C. T. Potter , S. Pozzorini , K. Prokofiev , A. Pukhov , I. Puljak , M. Queitsch-Maitland , J. Quevillon , D. Rathlev , M. Rauch , E. Re , M. N. Rebelo , D. Rebuzzi , L. Reina , C. Reuschle , J. Reuter , M. Riembau , F. Riva , A. Rizzi , T. Robens , R. Röntsch , J. Rojo , J. C. Romão , N. Rompotis , J. Roskes , R. Roth , G. P. Salam , R. Salerno , M. O. P. Sampaio , R. Santos , V. Sanz , J. J. Sanz-Cillero , H. Sargsyan , U. Sarica , P. Schichtel , J. Schlenk , T. Schmidt , C. Schmitt , M. Schönherr , U. Schubert , M. Schulze , S. Sekula , M. Sekulla , E. Shabalina , H. S. Shao , J. Shelton , C. H. Shepherd-Themistocleous , S. Y. Shim , F. Siegert , A. Signer , J. P. Silva , L. Silvestrini , M. Sjodahl , P. Slavich , M. Slawinska , L. Soffi , M. Spannowsky , C. Speckner , D. M. Sperka , M. Spira , O. Stål , F. Staub , T. Stebel , T. Stefaniak , M. Steinhauser , I. W. Stewart , M. J. Strassler , J. Streicher , D. M. Strom , S. Su , X. Sun , F. J. Tackmann , K. Tackmann , A. M. Teixeira , R. Teixeira de Lima , V. Theeuwes , R. Thorne , D. Tommasini , P. Torrielli , M. Tosi , F. Tramontano , Z. Trócsányi , M. Trott , I. Tsinikos , M. Ubiali , P. Vanlaer , W. Verkerke , A. Vicini , L. Viliani , E. Vryonidou , D. Wackeroth , C. E. M. Wagner , J. Wang , S. Wayand , G. Weiglein , C. Weiss , M. Wiesemann , C. Williams , J. Winter , D. Winterbottom , R. Wolf , M. Xiao , L. L. Yang , R. Yohay , S. P. Y. Yuen , G. Zanderighi , M. Zaro , D. Zeppenfeld , R. Ziegler , T. Zirke , J. Zupan

As there seems to be a large mass gap between the SM and new physics particles, the EFT framework emerges as the natural approach for the analysis and interpretation of collider data. However, this large gap and the fact that (so far) all…

High Energy Physics - Phenomenology · Physics 2017-10-23 J. J. Sanz-Cillero

Physics beyond the Standard Model (BSM) can be described in a consistent and general way through the Higgs Effective Field Theory (HEFT). Measurements of model-independent HEFT coefficients allow one to constrain the parameter space of BSM…

High Energy Physics - Phenomenology · Physics 2024-02-29 Sally Dawson , Duarte Fontes , Carlos Quezada-Calonge , Juan José Sanz-Cillero

Deviations from the Standard Model (SM) can be parameterized in terms of the SM effective field theory (SMEFT), which is typically truncated at dimension-6. Including higher dimension operators -- as well as considering simultaneous…

High Energy Physics - Phenomenology · Physics 2024-02-16 Konstantin Asteriadis , Sally Dawson , Duarte Fontes
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