M. Zaro

M. Zaro
Are you M. Zaro?

Claim your profile, edit publications, add additional information:

Contact Details

Name
M. Zaro
Affiliation
Location

Pubs By Year

Pub Categories

 
High Energy Physics - Phenomenology (31)
 
High Energy Physics - Experiment (10)

Publications Authored By M. Zaro

We study the production of jets in hadronic collisions, by computing all contributions proportional to $\alpha_S^n\alpha^m$, with $n+m=2$ and $n+m=3$. These correspond to leading and next-to-leading order results, respectively, for single-inclusive and dijet observables in a perturbative expansion that includes both QCD and electroweak effects. We discuss issues relevant to the definition of hadronic jets in the context of electroweak corrections, and present sample phenomenological predictions for the 13-TeV LHC. Read More

2016Oct
Authors: D. de Florian1, C. Grojean2, F. Maltoni3, C. Mariotti4, A. Nikitenko5, M. Pieri6, P. Savard7, M. Schumacher8, R. Tanaka9, R. Aggleton10, M. Ahmad11, B. Allanach12, C. Anastasiou13, W. Astill14, S. Badger15, M. Badziak16, J. Baglio17, E. Bagnaschi18, A. Ballestrero19, A. Banfi20, D. Barducci21, M. Beckingham22, C. Becot23, G. Bélanger24, J. Bellm25, N. Belyaev26, F. U. Bernlochner27, C. Beskidt28, A. Biekötter29, F. Bishara30, W. Bizon31, N. E. Bomark32, M. Bonvini33, S. Borowka34, V. Bortolotto35, S. Boselli36, F. J. Botella37, R. Boughezal38, G. C. Branco39, J. Brehmer40, L. Brenner41, S. Bressler42, I. Brivio43, A. Broggio44, H. Brun45, G. Buchalla46, C. D. Burgard47, A. Calandri48, L. Caminada49, R. Caminal Armadans50, F. Campanario51, J. Campbell52, F. Caola53, C. M. Carloni Calame54, S. Carrazza55, A. Carvalho56, M. Casolino57, O. Cata58, A. Celis59, F. Cerutti60, N. Chanon61, M. Chen62, X. Chen63, B. Chokoufé Nejad64, N. Christensen65, M. Ciuchini66, R. Contino67, T. Corbett68, D. Curtin69, M. Dall'Osso70, A. David71, S. Dawson72, J. de Blas73, W. de Boer74, P. de Castro Manzano75, C. Degrande76, R. L. Delgado77, F. Demartin78, A. Denner79, B. Di Micco80, R. Di Nardo81, S. Dittmaier82, A. Dobado83, T. Dorigo84, F. A. Dreyer85, M. Dührssen86, C. Duhr87, F. Dulat88, K. Ecker89, K. Ellis90, U. Ellwanger91, C. Englert92, D. Espriu93, A. Falkowski94, L. Fayard95, R. Feger96, G. Ferrera97, A. Ferroglia98, N. Fidanza99, T. Figy100, M. Flechl101, D. Fontes102, S. Forte103, P. Francavilla104, E. Franco105, R. Frederix106, A. Freitas107, F. F. Freitas108, F. Frensch109, S. Frixione110, B. Fuks111, E. Furlan112, S. Gadatsch113, J. Gao114, Y. Gao115, M. V. Garzelli116, T. Gehrmann117, R. Gerosa118, M. Ghezzi119, D. Ghosh120, S. Gieseke121, D. Gillberg122, G. F. Giudice123, E. W. N. Glover124, F. Goertz125, D. Gonçalves126, J. Gonzalez-Fraile127, M. Gorbahn128, S. Gori129, C. A. Gottardo130, M. Gouzevitch131, P. Govoni132, D. Gray133, M. Grazzini134, N. Greiner135, A. Greljo136, J. Grigo137, A. V. Gritsan138, R. Gröber139, S. Guindon140, H. E. Haber141, C. Han142, T. Han143, R. Harlander144, M. A. Harrendorf145, H. B. Hartanto146, C. Hays147, S. Heinemeyer148, G. Heinrich149, M. Herrero150, F. Herzog151, B. Hespel152, V. Hirschi153, S. Hoeche154, S. Honeywell155, S. J. Huber156, C. Hugonie157, J. Huston158, A. Ilnicka159, G. Isidori160, B. Jäger161, M. Jaquier162, S. P. Jones163, A. Juste164, S. Kallweit165, A. Kaluza166, A. Kardos167, A. Karlberg168, Z. Kassabov169, N. Kauer170, D. I. Kazakov171, M. Kerner172, W. Kilian173, F. Kling174, K. Köneke175, R. Kogler176, R. Konoplich177, S. Kortner178, S. Kraml179, C. Krause180, F. Krauss181, M. Krawczyk182, A. Kulesza183, S. Kuttimalai184, R. Lane185, A. Lazopoulos186, G. Lee187, P. Lenzi188, I. M. Lewis189, Y. Li190, S. Liebler191, J. Lindert192, X. Liu193, Z. Liu194, F. J. Llanes-Estrada195, H. E. Logan196, D. Lopez-Val197, I. Low198, G. Luisoni199, P. Maierhöfer200, E. Maina201, B. Mansoulié202, H. Mantler203, M. Mantoani204, A. C. Marini205, V. I. Martinez Outschoorn206, S. Marzani207, D. Marzocca208, A. Massironi209, K. Mawatari210, J. Mazzitelli211, A. McCarn212, B. Mellado213, K. Melnikov214, S. B. Menari215, L. Merlo216, C. Meyer217, P. Milenovic218, K. Mimasu219, S. Mishima220, B. Mistlberger221, S. -O. Moch222, A. Mohammadi223, P. F. Monni224, G. Montagna225, M. Moreno Llácer226, N. Moretti227, S. Moretti228, L. Motyka229, A. Mück230, M. Mühlleitner231, S. Munir232, P. Musella233, P. Nadolsky234, D. Napoletano235, M. Nebot236, C. Neu237, M. Neubert238, R. Nevzorov239, O. Nicrosini240, J. Nielsen241, K. Nikolopoulos242, J. M. No243, C. O'Brien244, T. Ohl245, C. Oleari246, T. Orimoto247, D. Pagani248, C. E. Pandini249, A. Papaefstathiou250, A. S. Papanastasiou251, G. Passarino252, B. D. Pecjak253, M. Pelliccioni254, G. Perez255, L. Perrozzi256, F. Petriello257, G. Petrucciani258, E. Pianori259, F. Piccinini260, M. Pierini261, A. Pilkington262, S. Plätzer263, T. Plehn264, R. Podskubka265, C. T. Potter266, S. Pozzorini267, K. Prokofiev268, A. Pukhov269, I. Puljak270, M. Queitsch-Maitland271, J. Quevillon272, D. Rathlev273, M. Rauch274, E. Re275, M. N. Rebelo276, D. Rebuzzi277, L. Reina278, C. Reuschle279, J. Reuter280, M. Riembau281, F. Riva282, A. Rizzi283, T. Robens284, R. Röntsch285, J. Rojo286, J. C. Romão287, N. Rompotis288, J. Roskes289, R. Roth290, G. P. Salam291, R. Salerno292, R. Santos293, V. Sanz294, J. J. Sanz-Cillero295, H. Sargsyan296, U. Sarica297, P. Schichtel298, J. Schlenk299, T. Schmidt300, C. Schmitt301, M. Schönherr302, U. Schubert303, M. Schulze304, S. Sekula305, M. Sekulla306, E. Shabalina307, H. S. Shao308, J. Shelton309, C. H. Shepherd-Themistocleous310, S. Y. Shim311, F. Siegert312, A. Signer313, J. P. Silva314, L. Silvestrini315, M. Sjodahl316, P. Slavich317, M. Slawinska318, L. Soffi319, M. Spannowsky320, C. Speckner321, D. M. Sperka322, M. Spira323, O. Stål324, F. Staub325, T. Stebel326, T. Stefaniak327, M. Steinhauser328, I. W. Stewart329, M. J. Strassler330, J. Streicher331, D. M. Strom332, S. Su333, X. Sun334, F. J. Tackmann335, K. Tackmann336, A. M. Teixeira337, R. Teixeira de Lima338, V. Theeuwes339, R. Thorne340, D. Tommasini341, P. Torrielli342, M. Tosi343, F. Tramontano344, Z. Trócsányi345, M. Trott346, I. Tsinikos347, M. Ubiali348, P. Vanlaer349, W. Verkerke350, A. Vicini351, L. Viliani352, E. Vryonidou353, D. Wackeroth354, C. E. M. Wagner355, J. Wang356, S. Wayand357, G. Weiglein358, C. Weiss359, M. Wiesemann360, C. Williams361, J. Winter362, D. Winterbottom363, R. Wolf364, M. Xiao365, L. L. Yang366, R. Yohay367, S. P. Y. Yuen368, G. Zanderighi369, M. Zaro370, D. Zeppenfeld371, R. Ziegler372, T. Zirke373, J. Zupan374
Affiliations: 1eds., 2eds., 3eds., 4eds., 5eds., 6eds., 7eds., 8eds., 9eds., 10The LHC Higgs Cross Section Working Group, 11The LHC Higgs Cross Section Working Group, 12The LHC Higgs Cross Section Working Group, 13The LHC Higgs Cross Section Working Group, 14The LHC Higgs Cross Section Working Group, 15The LHC Higgs Cross Section Working Group, 16The LHC Higgs Cross Section Working Group, 17The LHC Higgs Cross Section Working Group, 18The LHC Higgs Cross Section Working Group, 19The LHC Higgs Cross Section Working Group, 20The LHC Higgs Cross Section Working Group, 21The LHC Higgs Cross Section Working Group, 22The LHC Higgs Cross Section Working Group, 23The LHC Higgs Cross Section Working Group, 24The LHC Higgs Cross Section Working Group, 25The LHC Higgs Cross Section Working Group, 26The LHC Higgs Cross Section Working Group, 27The LHC Higgs Cross Section Working Group, 28The LHC Higgs Cross Section Working Group, 29The LHC Higgs Cross Section Working Group, 30The LHC Higgs Cross Section Working Group, 31The LHC Higgs Cross Section Working Group, 32The LHC Higgs Cross Section Working Group, 33The LHC Higgs Cross Section Working Group, 34The LHC Higgs Cross Section Working Group, 35The LHC Higgs Cross Section Working Group, 36The LHC Higgs Cross Section Working Group, 37The LHC Higgs Cross Section Working Group, 38The LHC Higgs Cross Section Working Group, 39The LHC Higgs Cross Section Working Group, 40The LHC Higgs Cross Section Working Group, 41The LHC Higgs Cross Section Working Group, 42The LHC Higgs Cross Section Working Group, 43The LHC Higgs Cross Section Working Group, 44The LHC Higgs Cross Section Working Group, 45The LHC Higgs Cross Section Working Group, 46The LHC Higgs Cross Section Working Group, 47The LHC Higgs Cross Section Working Group, 48The LHC Higgs Cross Section Working Group, 49The LHC Higgs Cross Section Working Group, 50The LHC Higgs Cross Section Working Group, 51The LHC Higgs Cross Section Working Group, 52The LHC Higgs Cross Section Working Group, 53The LHC Higgs Cross Section Working Group, 54The LHC Higgs Cross Section Working Group, 55The LHC Higgs Cross Section Working Group, 56The LHC Higgs Cross Section Working Group, 57The LHC Higgs Cross Section Working Group, 58The LHC Higgs Cross Section Working Group, 59The LHC Higgs Cross Section Working Group, 60The LHC Higgs Cross Section Working Group, 61The LHC Higgs Cross Section Working Group, 62The LHC Higgs Cross Section Working Group, 63The LHC Higgs Cross Section Working Group, 64The LHC Higgs Cross Section Working Group, 65The LHC Higgs Cross Section Working Group, 66The LHC Higgs Cross Section Working Group, 67The LHC Higgs Cross Section Working Group, 68The LHC Higgs Cross Section Working Group, 69The LHC Higgs Cross Section Working Group, 70The LHC Higgs Cross Section Working Group, 71The LHC Higgs Cross Section Working Group, 72The LHC Higgs Cross Section Working Group, 73The LHC Higgs Cross Section Working Group, 74The LHC Higgs Cross Section Working Group, 75The LHC Higgs Cross Section Working Group, 76The LHC Higgs Cross Section Working Group, 77The LHC Higgs Cross Section Working Group, 78The LHC Higgs Cross Section Working Group, 79The LHC Higgs Cross Section Working Group, 80The LHC Higgs Cross Section Working Group, 81The LHC Higgs Cross Section Working Group, 82The LHC Higgs Cross Section Working Group, 83The LHC Higgs Cross Section Working Group, 84The LHC Higgs Cross Section Working Group, 85The LHC Higgs Cross Section Working Group, 86The LHC Higgs Cross Section Working Group, 87The LHC Higgs Cross Section Working Group, 88The LHC Higgs Cross Section Working Group, 89The LHC Higgs Cross Section Working Group, 90The LHC Higgs Cross Section Working Group, 91The LHC Higgs Cross Section Working Group, 92The LHC Higgs Cross Section Working Group, 93The LHC Higgs Cross Section Working Group, 94The LHC Higgs Cross Section Working Group, 95The LHC Higgs Cross Section Working Group, 96The LHC Higgs Cross Section Working Group, 97The LHC Higgs Cross Section Working Group, 98The LHC Higgs Cross Section Working Group, 99The LHC Higgs Cross Section Working Group, 100The LHC Higgs Cross Section Working Group, 101The LHC Higgs Cross Section Working Group, 102The LHC Higgs Cross Section Working Group, 103The LHC Higgs Cross Section Working Group, 104The LHC Higgs Cross Section Working Group, 105The LHC Higgs Cross Section Working Group, 106The LHC Higgs Cross Section Working Group, 107The LHC Higgs Cross Section Working Group, 108The LHC Higgs Cross Section Working Group, 109The LHC Higgs Cross Section Working Group, 110The LHC Higgs Cross Section Working Group, 111The LHC Higgs Cross Section Working Group, 112The LHC Higgs Cross Section Working Group, 113The LHC Higgs Cross Section Working Group, 114The LHC Higgs Cross Section Working Group, 115The LHC Higgs Cross Section Working Group, 116The LHC Higgs Cross Section Working Group, 117The LHC Higgs Cross Section Working Group, 118The LHC Higgs Cross Section Working Group, 119The LHC Higgs Cross Section Working Group, 120The LHC Higgs Cross Section Working Group, 121The LHC Higgs Cross Section Working Group, 122The LHC Higgs Cross Section Working Group, 123The LHC Higgs Cross Section Working Group, 124The LHC Higgs Cross Section Working Group, 125The LHC Higgs Cross Section Working Group, 126The LHC Higgs Cross Section Working Group, 127The LHC Higgs Cross Section Working Group, 128The LHC Higgs Cross Section Working Group, 129The LHC Higgs Cross Section Working Group, 130The LHC Higgs Cross Section Working Group, 131The LHC Higgs Cross Section Working Group, 132The LHC Higgs Cross Section Working Group, 133The LHC Higgs Cross Section Working Group, 134The LHC Higgs Cross Section Working Group, 135The LHC Higgs Cross Section Working Group, 136The LHC Higgs Cross Section Working Group, 137The LHC Higgs Cross Section Working Group, 138The LHC Higgs Cross Section Working Group, 139The LHC Higgs Cross Section Working Group, 140The LHC Higgs Cross Section Working Group, 141The LHC Higgs Cross Section Working Group, 142The LHC Higgs Cross Section Working Group, 143The LHC Higgs Cross Section Working Group, 144The LHC Higgs Cross Section Working Group, 145The LHC Higgs Cross Section Working Group, 146The LHC Higgs Cross Section Working Group, 147The LHC Higgs Cross Section Working Group, 148The LHC Higgs Cross Section Working Group, 149The LHC Higgs Cross Section Working Group, 150The LHC Higgs Cross Section Working Group, 151The LHC Higgs Cross Section Working Group, 152The LHC Higgs Cross Section Working Group, 153The LHC Higgs Cross Section Working Group, 154The LHC Higgs Cross Section Working Group, 155The LHC Higgs Cross Section Working Group, 156The LHC Higgs Cross Section Working Group, 157The LHC Higgs Cross Section Working Group, 158The LHC Higgs Cross Section Working Group, 159The LHC Higgs Cross Section Working Group, 160The LHC Higgs Cross Section Working Group, 161The LHC Higgs Cross Section Working Group, 162The LHC Higgs Cross Section Working Group, 163The LHC Higgs Cross Section Working Group, 164The LHC Higgs Cross Section Working Group, 165The LHC Higgs Cross Section Working Group, 166The LHC Higgs Cross Section Working Group, 167The LHC Higgs Cross Section Working Group, 168The LHC Higgs Cross Section Working Group, 169The LHC Higgs Cross Section Working Group, 170The LHC Higgs Cross Section Working Group, 171The LHC Higgs Cross Section Working Group, 172The LHC Higgs Cross Section Working Group, 173The LHC Higgs Cross Section Working Group, 174The LHC Higgs Cross Section Working Group, 175The LHC Higgs Cross Section Working Group, 176The LHC Higgs Cross Section Working Group, 177The LHC Higgs Cross Section Working Group, 178The LHC Higgs Cross Section Working Group, 179The LHC Higgs Cross Section Working Group, 180The LHC Higgs Cross Section Working Group, 181The LHC Higgs Cross Section Working Group, 182The LHC Higgs Cross Section Working Group, 183The LHC Higgs Cross Section Working Group, 184The LHC Higgs Cross Section Working Group, 185The LHC Higgs Cross Section Working Group, 186The LHC Higgs Cross Section Working Group, 187The LHC Higgs Cross Section Working Group, 188The LHC Higgs Cross Section Working Group, 189The LHC Higgs Cross Section Working Group, 190The LHC Higgs Cross Section Working Group, 191The LHC Higgs Cross Section Working Group, 192The LHC Higgs Cross Section Working Group, 193The LHC Higgs Cross Section Working Group, 194The LHC Higgs Cross Section Working Group, 195The LHC Higgs Cross Section Working Group, 196The LHC Higgs Cross Section Working Group, 197The LHC Higgs Cross Section Working Group, 198The LHC Higgs Cross Section Working Group, 199The LHC Higgs Cross Section Working Group, 200The LHC Higgs Cross Section Working Group, 201The LHC Higgs Cross Section Working Group, 202The LHC Higgs Cross Section Working Group, 203The LHC Higgs Cross Section Working Group, 204The LHC Higgs Cross Section Working Group, 205The LHC Higgs Cross Section Working Group, 206The LHC Higgs Cross Section Working Group, 207The LHC Higgs Cross Section Working Group, 208The LHC Higgs Cross Section Working Group, 209The LHC Higgs Cross Section Working Group, 210The LHC Higgs Cross Section Working Group, 211The LHC Higgs Cross Section Working Group, 212The LHC Higgs Cross Section Working Group, 213The LHC Higgs Cross Section Working Group, 214The LHC Higgs Cross Section Working Group, 215The LHC Higgs Cross Section Working Group, 216The LHC Higgs Cross Section Working Group, 217The LHC Higgs Cross Section Working Group, 218The LHC Higgs Cross Section Working Group, 219The LHC Higgs Cross Section Working Group, 220The LHC Higgs Cross Section Working Group, 221The LHC Higgs Cross Section Working Group, 222The LHC Higgs Cross Section Working Group, 223The LHC Higgs Cross Section Working Group, 224The LHC Higgs Cross Section Working Group, 225The LHC Higgs Cross Section Working Group, 226The LHC Higgs Cross Section Working Group, 227The LHC Higgs Cross Section Working Group, 228The LHC Higgs Cross Section Working Group, 229The LHC Higgs Cross Section Working Group, 230The LHC Higgs Cross Section Working Group, 231The LHC Higgs Cross Section Working Group, 232The LHC Higgs Cross Section Working Group, 233The LHC Higgs Cross Section Working Group, 234The LHC Higgs Cross Section Working Group, 235The LHC Higgs Cross Section Working Group, 236The LHC Higgs Cross Section Working Group, 237The LHC Higgs Cross Section Working Group, 238The LHC Higgs Cross Section Working Group, 239The LHC Higgs Cross Section Working Group, 240The LHC Higgs Cross Section Working Group, 241The LHC Higgs Cross Section Working Group, 242The LHC Higgs Cross Section Working Group, 243The LHC Higgs Cross Section Working Group, 244The LHC Higgs Cross Section Working Group, 245The LHC Higgs Cross Section Working Group, 246The LHC Higgs Cross Section Working Group, 247The LHC Higgs Cross Section Working Group, 248The LHC Higgs Cross Section Working Group, 249The LHC Higgs Cross Section Working Group, 250The LHC Higgs Cross Section Working Group, 251The LHC Higgs Cross Section Working Group, 252The LHC Higgs Cross Section Working Group, 253The LHC Higgs Cross Section Working Group, 254The LHC Higgs Cross Section Working Group, 255The LHC Higgs Cross Section Working Group, 256The LHC Higgs Cross Section Working Group, 257The LHC Higgs Cross Section Working Group, 258The LHC Higgs Cross Section Working Group, 259The LHC Higgs Cross Section Working Group, 260The LHC Higgs Cross Section Working Group, 261The LHC Higgs Cross Section Working Group, 262The LHC Higgs Cross Section Working Group, 263The LHC Higgs Cross Section Working Group, 264The LHC Higgs Cross Section Working Group, 265The LHC Higgs Cross Section Working Group, 266The LHC Higgs Cross Section Working Group, 267The LHC Higgs Cross Section Working Group, 268The LHC Higgs Cross Section Working Group, 269The LHC Higgs Cross Section Working Group, 270The LHC Higgs Cross Section Working Group, 271The LHC Higgs Cross Section Working Group, 272The LHC Higgs Cross Section Working Group, 273The LHC Higgs Cross Section Working Group, 274The LHC Higgs Cross Section Working Group, 275The LHC Higgs Cross Section Working Group, 276The LHC Higgs Cross Section Working Group, 277The LHC Higgs Cross Section Working Group, 278The LHC Higgs Cross Section Working Group, 279The LHC Higgs Cross Section Working Group, 280The LHC Higgs Cross Section Working Group, 281The LHC Higgs Cross Section Working Group, 282The LHC Higgs Cross Section Working Group, 283The LHC Higgs Cross Section Working Group, 284The LHC Higgs Cross Section Working Group, 285The LHC Higgs Cross Section Working Group, 286The LHC Higgs Cross Section Working Group, 287The LHC Higgs Cross Section Working Group, 288The LHC Higgs Cross Section Working Group, 289The LHC Higgs Cross Section Working Group, 290The LHC Higgs Cross Section Working Group, 291The LHC Higgs Cross Section Working Group, 292The LHC Higgs Cross Section Working Group, 293The LHC Higgs Cross Section Working Group, 294The LHC Higgs Cross Section Working Group, 295The LHC Higgs Cross Section Working Group, 296The LHC Higgs Cross Section Working Group, 297The LHC Higgs Cross Section Working Group, 298The LHC Higgs Cross Section Working Group, 299The LHC Higgs Cross Section Working Group, 300The LHC Higgs Cross Section Working Group, 301The LHC Higgs Cross Section Working Group, 302The LHC Higgs Cross Section Working Group, 303The LHC Higgs Cross Section Working Group, 304The LHC Higgs Cross Section Working Group, 305The LHC Higgs Cross Section Working Group, 306The LHC Higgs Cross Section Working Group, 307The LHC Higgs Cross Section Working Group, 308The LHC Higgs Cross Section Working Group, 309The LHC Higgs Cross Section Working Group, 310The LHC Higgs Cross Section Working Group, 311The LHC Higgs Cross Section Working Group, 312The LHC Higgs Cross Section Working Group, 313The LHC Higgs Cross Section Working Group, 314The LHC Higgs Cross Section Working Group, 315The LHC Higgs Cross Section Working Group, 316The LHC Higgs Cross Section Working Group, 317The LHC Higgs Cross Section Working Group, 318The LHC Higgs Cross Section Working Group, 319The LHC Higgs Cross Section Working Group, 320The LHC Higgs Cross Section Working Group, 321The LHC Higgs Cross Section Working Group, 322The LHC Higgs Cross Section Working Group, 323The LHC Higgs Cross Section Working Group, 324The LHC Higgs Cross Section Working Group, 325The LHC Higgs Cross Section Working Group, 326The LHC Higgs Cross Section Working Group, 327The LHC Higgs Cross Section Working Group, 328The LHC Higgs Cross Section Working Group, 329The LHC Higgs Cross Section Working Group, 330The LHC Higgs Cross Section Working Group, 331The LHC Higgs Cross Section Working Group, 332The LHC Higgs Cross Section Working Group, 333The LHC Higgs Cross Section Working Group, 334The LHC Higgs Cross Section Working Group, 335The LHC Higgs Cross Section Working Group, 336The LHC Higgs Cross Section Working Group, 337The LHC Higgs Cross Section Working Group, 338The LHC Higgs Cross Section Working Group, 339The LHC Higgs Cross Section Working Group, 340The LHC Higgs Cross Section Working Group, 341The LHC Higgs Cross Section Working Group, 342The LHC Higgs Cross Section Working Group, 343The LHC Higgs Cross Section Working Group, 344The LHC Higgs Cross Section Working Group, 345The LHC Higgs Cross Section Working Group, 346The LHC Higgs Cross Section Working Group, 347The LHC Higgs Cross Section Working Group, 348The LHC Higgs Cross Section Working Group, 349The LHC Higgs Cross Section Working Group, 350The LHC Higgs Cross Section Working Group, 351The LHC Higgs Cross Section Working Group, 352The LHC Higgs Cross Section Working Group, 353The LHC Higgs Cross Section Working Group, 354The LHC Higgs Cross Section Working Group, 355The LHC Higgs Cross Section Working Group, 356The LHC Higgs Cross Section Working Group, 357The LHC Higgs Cross Section Working Group, 358The LHC Higgs Cross Section Working Group, 359The LHC Higgs Cross Section Working Group, 360The LHC Higgs Cross Section Working Group, 361The LHC Higgs Cross Section Working Group, 362The LHC Higgs Cross Section Working Group, 363The LHC Higgs Cross Section Working Group, 364The LHC Higgs Cross Section Working Group, 365The LHC Higgs Cross Section Working Group, 366The LHC Higgs Cross Section Working Group, 367The LHC Higgs Cross Section Working Group, 368The LHC Higgs Cross Section Working Group, 369The LHC Higgs Cross Section Working Group, 370The LHC Higgs Cross Section Working Group, 371The LHC Higgs Cross Section Working Group, 372The LHC Higgs Cross Section Working Group, 373The LHC Higgs Cross Section Working Group, 374The LHC Higgs Cross Section Working Group

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 new results that have appeared in the last few years. The first part compiles the most up-to-date predictions of Higgs boson production cross sections and decay branching ratios, parton distribution functions, and off-shell Higgs boson production and interference effects. Read More

We study Higgs boson production in association with a top quark and a $W$ boson at the LHC. At NLO in QCD, $tWH$ interferes with $t\bar t H$ and a procedure to meaningfully separate the two processes needs to be employed. In order to define $tWH$ production for both total rates and differential distributions, we consider the diagram removal and diagram subtraction techniques that have been previously proposed for treating intermediate resonances at NLO, in particular in the context of $tW$ production. Read More

We present predictions for the total cross section for the production of a charged Higgs boson in a generic type-II two-Higgs-doublet model in the intermediate-mass range ($m_{H^{\pm}}\sim m_t$) at the LHC. Results are obtained at next-to-leading order (NLO) accuracy in QCD perturbation theory, by studying the full process $pp\to H^\pm W^\mp b \bar b$ in the complex-(top)-mass scheme with massive bottom quarks. Compared to lowest-order predictions, NLO corrections have a sizable impact: they increase the cross section by roughly 50% and reduce uncertainties due to scale variations by more than a factor of two. Read More

This report summarises the properties of Standard Model processes at the 100 TeV pp collider. We document the production rates and typical distributions for a number of benchmark Standard Model processes, and discuss new dynamical phenomena arising at the highest energies available at this collider. We discuss the intrinsic physics interest in the measurement of these Standard Model processes, as well as their role as backgrounds for New Physics searches. Read More

We discuss the impact of EW corrections on differential distributions in top-quark pair production at the LHC and future hadron colliders, focusing on the effects of initial-state photons. Performing a calculation at Next-to-Leading Order QCD+EW accuracy, we investigate in detail the impact of photon-initiated channels on central values as well as PDF and scale uncertainties, both at order $\alpha_s\alpha$ and $\alpha_s^2\alpha$. We present predictions at 13 and 100 TeV, and provide results for the 8 TeV differential measurements performed by ATLAS and CMS. Read More

This Report summarizes the proceedings of the 2015 Les Houches workshop on Physics at TeV Colliders. Session 1 dealt with (I) new developments relevant for high precision Standard Model calculations, (II) the new PDF4LHC parton distributions, (III) issues in the theoretical description of the production of Standard Model Higgs bosons and how to relate experimental measurements, (IV) a host of phenomenological studies essential for comparing LHC data from Run I with theoretical predictions and projections for future measurements in Run II, and (V) new developments in Monte Carlo event generators. Read More

We study the phenomenology of the Georgi-Machacek model at next-to-leading order (NLO) in QCD matched to parton shower, using a fully-automated tool chain based on MadGraph5_aMC@NLO and FeynRules. We focus on the production of the fermiophobic custodial fiveplet scalars H_5^0, H_5^+/-, and H_5^++/-- through vector boson fusion (VBF), associated production with a vector boson (V H_5), and scalar pair production (H_5 H_5). For these production mechanisms we compute NLO corrections to production rates as well as to differential distributions. Read More

In this paper we discuss the effect of the complete leading-order QED corrections to the DGLAP equations in the perturbative evolution of parton distribution functions (PDFs). This requires the extension of the purely QCD DGLAP evolution, including a PDF for the photons and, consistently, also for the charged leptons $e^{\pm}$, $\mu^\pm$ and $\tau^\pm$. We present the implementation of the QED-corrected DGLAP evolution in the presence of photon and lepton PDFs in the APFEL program and, by means of different assumptions for the initial scale PDFs, we produce for the first time PDF sets containing charged lepton distributions. Read More

In this paper we study the production of a heavy charged Higgs boson in association with heavy quarks at the LHC, in a type-II two-Higgs-doublet model. We present for the first time fully-differential results obtained in the four-flavour scheme at NLO accuracy, both at fixed order and including the matching with parton showers. Relevant differential distributions are studied for two values of the charged boson mass and a thorough comparison is performed between predictions obtained in the four- and five-flavour schemes. Read More

We present the Higgs Characterisation (HC) framework to study the properties of the Higgs boson observed at 125 GeV. In this report, we focus on CP properties of the top-quark Yukawa interaction, and show predictions at next-to-leading order accuracy in QCD, including parton-shower effects, for Higgs production in association with a single top quark at the LHC. Read More

We compute the contribution of order $\alpha_S^2\alpha^2$ to the cross section of a top-antitop pair in association with at least one heavy Standard Model boson -- $Z$, $W^\pm$, and Higgs -- by including all effects of QCD, QED, and weak origin and by working in the automated MadGraph5_aMC@NLO framework. This next-to-leading order contribution is then combined with that of order $\alpha_S^3\alpha$, and with the two dominant lowest-order ones, $\alpha_S^2\alpha$ and $\alpha_S\alpha^2$, to obtain phenomenological results relevant to a 8, 13, and 100~TeV $pp$ collider. Read More

We present a detailed study of Higgs boson production in association with a single top quark at the LHC, at next-to-leading order accuracy in QCD. We consider total and differential cross sections, at the parton level as well as by matching short distance events to parton showers, for both t-channel and s-channel production. We provide predictions relevant for the LHC at 13 TeV together with a thorough evaluation of the residual uncertainties coming from scale variation, parton distributions, strong coupling constant and heavy quark masses. Read More

The observation of double and triple scalar boson production at hadron colliders could provide key information on the Higgs self couplings and the potential. As for single Higgs production the largest rates for multiple Higgs production come from gluon-gluon fusion processes mediated by a top-quark loop. However, at variance with single Higgs production, top-quark mass and width effects from the loops cannot be neglected. Read More

At the LHC the CP properties of the top-quark Yukawa interaction can be probed through Higgs production in gluon fusion or in association with top quarks. We consider the possibility for both CP-even and CP-odd couplings to the top quark to be present, and study CP-sensitive observables at next-to-leading order (NLO) in QCD, including parton-shower effects. We show that the inclusion of NLO corrections sizeably reduces the theoretical uncertainties, and confirm that di-jet correlations in $H+2$ jet production through gluon fusion and correlations of the top-quark decay products in $t\bar tH$ production can provide sensitive probes of the CP nature of the Higgs interactions. Read More

We present the calculation of the next-to-leading contribution of order $\alpha_S^2\alpha^2$ to the production of a Standard Model Higgs boson in association with a top-quark pair at hadron colliders. All effects of weak and QCD origin are included, whereas those of QED origin are ignored. We work in the MadGraph5_aMC@NLO framework, and discuss sample phenomenological applications at a 8, 13, and 100 TeV $pp$ collider, including the effects of the dominant next-to-leading QCD corrections of order $\alpha_S^3\alpha$. Read More

We study the charge asymmetry between the $t$ and $\bar t$ quark at the LHC, when they are produced in association with a $W$ boson. Though sizably reducing the cross section with respect to the inclusive production, requiring a $W$ boson in the final state has two important implications. First, at leading order in QCD, $t \bar t W^{\pm}$ production can only occur via $q \bar q$ annihilation. Read More

We discuss the theoretical bases that underpin the automation of the computations of tree-level and next-to-leading order cross sections, of their matching to parton shower simulations, and of the merging of matched samples that differ by light-parton multiplicities. We present a computer program, MadGraph5_aMC@NLO, capable of handling all these computations -- parton-level fixed order, shower-matched, merged -- in a unified framework whose defining features are flexibility, high level of parallelisation, and human intervention limited to input physics quantities. We demonstrate the potential of the program by presenting selected phenomenological applications relevant to the LHC and to a 1-TeV $e^+e^-$ collider. Read More

We present predictions for the SM-Higgs-pair production channels of relevance at the LHC: gluon-gluon fusion, VBF, and top-pair, W, Z and single-top associated production. All these results are at the NLO accuracy in QCD, and matched to parton showers by means of the MC@NLO method; hence, they are fully differential. With the exception of the gluon-gluon fusion process, for which a special treatment is needed in order to improve upon the infinite-top-mass limit, our predictions are obtained in a fully automatic way within the publicly available MadGraph5_aMC@NLO framework. Read More

Vector-boson fusion and associated production at the LHC can provide key information on the strength and structure of the Higgs couplings to the Standard Model particles. Using an effective field theory approach, we study the effects of next-to-leading order (NLO) QCD corrections matched to parton shower on selected observables for various spin-0 hypotheses. We find that inclusion of NLO corrections is needed to reduce the theoretical uncertainties on total rates as well as to reliably predict the shapes of the distributions. Read More

2013Jul
Authors: The LHC Higgs Cross Section Working Group, S. Heinemeyer1, C. Mariotti2, G. Passarino3, R. Tanaka4, J. R. Andersen, P. Artoisenet, E. A. Bagnaschi, A. Banfi, T. Becher, F. U. Bernlochner, S. Bolognesi, P. Bolzoni, R. Boughezal, D. Buarque, J. Campbell, F. Caola, M. Carena, F. Cascioli, N. Chanon, T. Cheng, S. Y. Choi, A. David, P. de Aquino, G. Degrassi, D. Del Re, A. Denner, H. van Deurzen, S. Diglio, B. Di Micco, R. Di Nardo, S. Dittmaier, M. Duhrssen, R. K. Ellis, G. Ferrera, N. Fidanza, M. Flechl, D. de Florian, S. Forte, R. Frederix, S. Frixione, S. Gangal, Y. Gao, M. V. Garzelli, D. Gillberg, P. Govoni, M. Grazzini, N. Greiner, J. Griffiths, A . V. Gritsan, C. Grojean, D. C. Hall, C. Hays, R. Harlander, R. Hernandez-Pinto, S. Hoche, J. Huston, T. Jubb, M. Kadastik, S. Kallweit, A. Kardos, L. Kashif, N. Kauer, H. Kim, R. Klees, M. Kramer, F. Krauss, A. Laureys, S. Laurila, S. Lehti, Q. Li, S. Liebler, X. Liu, H. E. Logan, G. Luisoni, M. Malberti, F. Maltoni, K. Mawatari, F. Maierhofer, H. Mantler, S. Martin, P. Mastrolia, O. Mattelaer, J. Mazzitelli, B. Mellado, K. Melnikov, P. Meridiani, D. J. Miller, E. Mirabella, S. O. Moch, P. Monni, N. Moretti, A. Muck, M. Muhlleitner, P. Musella, P. Nason, C. Neu, M. Neubert, C. Oleari, J. Olsen, G. Ossola, T. Peraro, K. Peters, F. Petriello, G. Piacquadio, C. T. Potter, S. Pozzorini, K. Prokofiev, I. Puljak, M. Rauch, D. Rebuzzi, L. Reina, R. Rietkerk, A. Rizzi, Y. Rotstein-Habarnau, G. P. Salam, G. Sborlini, F. Schissler, M. Schonherr, M. Schulze, M. Schumacher, F. Siegert, P. Slavich, J. M. Smillie, O. Stal, J. F. von Soden-Fraunhofen, M. Spira, I. W. Stewart, F. J. Tackmann, P. T. E. Taylor, D. Tommasini, J. Thompson, R. S. Thorne, P. Torrielli, F. Tramontano, N. V. Tran, Z. Trocsanyi, M. Ubiali, P. Vanlaer, M. Vazquez Acosta, T. Vickey, A. Vicini, W. J. Waalewijn, D. Wackeroth, C. Wagner, J. R. Walsh, J. Wang, G. Weiglein, A. Whitbeck, C. Williams, J. Yu, G. Zanderighi, M. Zanetti, M. Zaro, P. M. Zerwas, C. Zhang, T. J . E. Zirke, S. Zuberi
Affiliations: 1eds., 2eds., 3eds., 4eds.

This Report summarizes the results of the activities in 2012 and the first half of 2013 of the LHC Higgs Cross Section Working Group. The main goal of the working group was to present the state of the art of Higgs Physics at the LHC, integrating all new results that have appeared in the last few years. This report follows the first working group report Handbook of LHC Higgs Cross Sections: 1. Read More

We introduce a framework, based on an effective field theory approach, that allows one to perform characterisation studies of the boson recently discovered at the LHC, for all the relevant channels and in a consistent, systematic and accurate way. The production and decay of such a boson with various spin and parity assignments can be simulated by means of multi-parton, tree-level matrix elements and of next-to-leading order QCD calculations, both matched with parton showers. Several sample applications are presented which show, in particular, that beyond-leading-order effects in QCD have non-trivial phenomenological implications. Read More

We present a study of Higgs hadroproduction through vector-boson fusion at the NLO in QCD matched with parton showers. We discuss the matching systematics affecting this process through a comparison of the aMC@NLO predictions with the POWHEG and the pure-NLO ones. Read More

In this paper, we present the next-to-leading order predictions for diphoton production in the ADD model, matched to the HERWIG parton shower using the MC@NLO formalism. A selection of the results is presented for d=2-6 extra dimensions, using generic cuts as well as analysis cuts mimicking the search strategies as pursued by the ATLAS and CMS experiments. Read More

Current methods to extract the quark-mixing matrix element $|V_{tb}|$ from single-top production measurements assume that $|V_{tb}|\gg |V_{td}|, |V_{ts}|$: top quarks decay into $b$ quarks with 100% branching fraction, s-channel single-top production is always accompanied by a $b$ quark and initial-state contributions from $d$ and $s$ quarks in the $t$-channel production of single top quarks are neglected. Triggered by a recent measurement of the ratio $R=\frac{|V_{tb}|^{2}}{|V_{td}|^{2}+|V_{ts}|^{2}+|V_{tb}|^{2}}=0.90 \pm 0. Read More

Weak vector boson fusion provides a unique channel to directly probe the mechanism of electroweak symmetry breaking at hadron colliders. We present a method that allows to calculate total cross sections to next-to-next-to-leading order (NNLO) in QCD for an arbitrary V* V* -> X process, the so-called structure function approach. By discussing the case of Higgs production in detail, we estimate several classes of previously neglected contributions and we argue that such method is accurate at a precision level well above the typical residual scale and PDF uncertainties at NNLO. Read More

We present the total cross sections at next-to-next-to-leading order (NNLO) in the strong coupling for single and double charged Higgs production via weak boson fusion. Results are obtained via the structure function approach, which builds upon the approximate, though very accurate, factorization of the QCD corrections between the two quark lines. The theoretical uncertainty on the total cross sections at the LHC from higher order corrections and the parton distribution uncertainties are estimated at the 2% level each for a wide range of Higgs boson masses. Read More

We present a phenomenological study for the production of the Higgs boson at next-to-next-to-leading order (NNLO) in QCD via the vector boson fusion (VBF) process. After a general discussion about the different production channels of the Higgs, we show results for hadron colliders like LHC and Tevatron in VBF. The theoretical predictions are obtained using the structure function approach. Read More

We present the total cross sections at next-to-next-to-leading order (NNLO) in the strong coupling for Higgs production via weak boson fusion. Our results are obtained via the structure function approach, which builds upon the approximate, though very accurate, factorization of the QCD corrections between the two quark lines. The theoretical uncertainty on the total cross sections at the LHC from higher order corrections and the parton distribution uncertainties are estimated at the 2% level each for a wide range of Higgs boson masses. Read More