Handbook of LHC Higgs Cross Sections: 2. Differential Distributions

Dittmaier, S.; Lehti, S.; Mück, A.; Stirling, W.J.; Piacquadio, G.; Salam, G.P.; Cooper-Sarkar, A.M.; Warsinsky, M.; Puljak, I.; Schumacher, M.; Di Micco, B.; Goria, S.; Mellado, B.; Kauer, N.; Stewart, I.W.; Banfi, A.; D'Enterria, D.; Hamilton, K.; Siegert, F.; Ferrera, G.; Guillet, J.-Ph.; Maltoni, F.; Ellis, R.K.; Rosco, D.; Krauss, F.; Glazov, S.; Neu, C.; Vickey, T.; Tackmann, F.J.; Rebuzzi, D.; Jackson, C.; Palmer, S.; Tanaka, R.; Nikitenko, A.; Pilon, E.; Kuo, C.-M.; Kim, H.; Bagnaschi, E.A.; Hauru, M.; Felcini, M.; Slavich, P.; Garzelli, M.V.; Huston, J.; Potter, C.T.; Li, Q.; Reina, L.; Petriello, F.; Price, J.; Harlander, R.; Thorne, R.S.; Di Nardo, R.; Vazquez Acosta, M.; Gascon-Shotkin, S.; Sturm, C.; Paganis, S.; Alekhin, S.; Quayle, W.; Weiglein, G.; Grazzini, M.; Dawson, S.; Olsen, J.; Stöckli, F.; Flechl, M.; Mühlleitner, M.; Rojo, J.; Vicini, A.; Petersen, T..C.; Radescu, V.; Zanderighi, G.; Jorgensen, M.D.; Ganjour, S.; Lorenzo, N.; Mariotti, C.; Hackstein, C.; Nadolsky, P.; Höche, S.; Schaarschmidt, J.; Schönherr, M.; Krämer, M.; de Florian, D.; Cheng, T.; Uccirati, S.; Weber, M.; Oleari, C.; Ubiali, M.; Farilla, A.; Trócsányi, Z.; Forte, S.; Jimenez-Delgado, P.; Waalewijn, W.J.; Petrucci, F.; Nason, P.; Diglio, S.; Moch, S.O.; Heinemeyer, S.; Davies, G.; Kado, M.; Spira, M.; De Filippis, N.; Wackeroth, D.; Kallweit, S.; Chanon, N.; Cutajar, M.; Sapronov, A.; Alwall, J.; Wiesemann, M.; Kovac, M.; Passarino, G.; Kardos, A.; Bolognesi, S.; Denner, A.; Cieri, L.; Farrington, S.; Papadopoulos, C.G.; Tommasini, D.; Yu, J.; Blümlein, J.; Degrassi, G.; Torrielli, P.; Tramontano, F.
doi:10.5170/CERN-2012-002
001416519 001__ 1416519
001416519 003__ SzGeCERN
001416519 005__ 20230919073312.0
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001416519 020__ $$a9789290833710
001416519 035__ $$9arXiv$$aoai:arXiv.org:1201.3084
001416519 035__ $$9Inspire$$a1084695
001416519 037__ $$9arXiv$$aarXiv:1201.3084$$chep-ph
001416519 037__ $$aCERN-2012-002
001416519 041__ $$aeng
001416519 088__ $$aCERN-2012-002
001416519 084__ $$2CERN Yellow Report$$aCERN-2012-002
001416519 100__ $$aDittmaier, S.$$uFreiburg U.$$vPhysikalisches Institut,Albert-Ludwigs-Universität Freiburg,D-79104 Freiburg,Germany
001416519 245__ $$aHandbook of LHC Higgs Cross Sections: 2. Differential Distributions
001416519 269__ $$c2012-01
001416519 260__ $$aGeneva$$bCERN$$c2012
001416519 300__ $$a275 p
001416519 340__ $$apaper
001416519 490__ $$aCERN Yellow Reports: Monographs
001416519 500__ $$aThe authors dedicate this Report to the memory of Robert Brout and Simon van der Meer.
001416519 500__ $$9Inspire$$aLong author list - awaiting processing
001416519 500__ $$9arXiv$$a275 pages, 136 figures, to be submitted to CERN Report. Working Group web page: https://twiki.cern.ch/twiki/bin/view/LHCPhysics/CrossSections
001416519 520__ $$aThis Report summarises the results of the second year's activities 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. The first working group report Handbook of LHC Higgs Cross Sections: 1. Inclusive Observables (CERN-2011-002) focuses on predictions (central values and errors) for total Higgs production cross sections and Higgs branching ratios in the Standard Model and its minimal supersymmetric extension, covering also related issues such as Monte Carlo generators, parton distribution functions, and pseudo-observables. This second Report represents the next natural step towards realistic predictions upon providing results on cross sections with benchmark cuts, differential distributions, details of specific decay channels, and further recent developments.
001416519 520__ $$9arXiv$$aThis Report summarises the results of the second year's activities 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. The first working group report Handbook of LHC Higgs Cross Sections: 1. Inclusive Observables (CERN-2011-002) focuses on predictions (central values and errors) for total Higgs production cross sections and Higgs branching ratios in the Standard Model and its minimal supersymmetric extension, covering also related issues such as Monte Carlo generators, parton distribution functions, and pseudo-observables. This second Report represents the next natural step towards realistic predictions upon providing results on cross sections with benchmark cuts, differential distributions, details of specific decay channels, and further recent developments.
001416519 536__ $$rOpen Access
001416519 540__ $$3publication$$aCC-BY-3.0
001416519 542__ $$3publication$$dCERN$$g2012
001416519 595__ $$aLANL EDS
001416519 599__ $$aILSSYNC
001416519 599__ $$aILSLINK
001416519 65017 $$2arXiv$$aParticle Physics - Phenomenology
001416519 65027 $$2arXiv$$aParticle Physics - Experiment
001416519 690C_ $$aREPORT
001416519 690C_ $$aYELLOW REPORT
001416519 690C_ $$aCERN
001416519 695__ $$9LANL EDS$$ahep-ph
001416519 695__ $$9LANL EDS$$ahep-ex
001416519 700__ $$aMariotti, C.$$uINFN, Turin$$uCERN$$vINFN,Sezione di Torino,Via P. Giuria 1,10125 Torino,Italy$$vCERN,CH-1211 Geneva 23,Switzerland
001416519 700__ $$aPassarino, G.$$uINFN, Turin$$uTurin U.$$vINFN,Sezione di Torino,Via P. Giuria 1,10125 Torino,Italy$$vDipartimento di Fisica Teorica,Università di Torino,Via P. Giuria 1,10125 Torino,Italy
001416519 700__ $$aTanaka, R.$$uOrsay, LAL$$vLaboratoire de l'Accélérateur Linéaire,CNRS/IN2P3,F-91898 Orsay CEDEX,France
001416519 700__ $$aAlekhin, S.$$uDESY, Zeuthen$$uDubna U., Protvino Branch$$vDESY,Zeuthen,Platanenallee 6,D-15738 Zeuthen,Germany$$vInstitute for High Energy Physics,142281 Protvino,Moscow region,Russia
001416519 700__ $$aAlwall, J.$$uFermilab$$vTheoretical Physics Department,Fermi National Accelerator Laboratory MS 106,Batavia,IL 60510-0500,USA
001416519 700__ $$aBagnaschi, E.A.$$uMilan U.$$uParis U., VI-VII$$vDipartimento di Fisica,Università degli Studi di Milano and INFN,Sezione di Milano,Via Celoria 16,I-20133 Milan,Italy$$vLaboratoire de Physique Théorique et des Hautes Energies,4 Place Jussieu,F-75252 Paris CEDEX 05,France
001416519 700__ $$aBanfi, A.$$uZurich, ETH$$vZurich,ETH CH-8093 Zurich,Schafmattstrasse 16,8093,Zurich,Switzerland
001416519 700__ $$aBlümlein, J.$$uDESY, Zeuthen$$vDESY,Zeuthen,Platanenallee 6,D-15738 Zeuthen,Germany
001416519 700__ $$aBolognesi, S.$$uJohns Hopkins U.$$vJohns Hopkins University,Baltimore,Maryland. 410-516-8000,USA
001416519 700__ $$aChanon, N.$$uZurich, ETH$$vZurich,ETH CH-8093 Zurich,Schafmattstrasse 16,8093,Zurich,Switzerland
001416519 700__ $$aCheng, T.$$uFlorida U.$$vUniversity of Florida,215 Williamson Hall,P.O. Box 118440 Gainesville,FL 32611
001416519 700__ $$aCieri, L.$$uBuenos Aires U.$$vDepartamento de Física,Facultad de Ciencias Exactas y Naturales Universidad de Buenos Aires,Pabellon I,Ciudad Universitaria (1428) Capital Federal,Argentina
001416519 700__ $$aCooper-Sarkar, A.M.$$uJAI, UK$$vDepartment of Physics,University of Oxford,Denys Wilkinson Building,Keble Road,Oxford OX1 3RH,UK
001416519 700__ $$aCutajar, M.$$uImperial Coll., London$$vPhysics Dept.,Blackett Laboratory,Imperial College London,Prince Consort Rd,London SW7 2BW,UK
001416519 700__ $$aDawson, S.$$uBrookhaven$$vDepartment of Physics,Brookhaven National Laboratory,Upton,NY 11973,USA
001416519 700__ $$aDavies, G.$$uImperial Coll., London$$vPhysics Dept.,Blackett Laboratory,Imperial College London,Prince Consort Rd,London SW7 2BW,UK
001416519 700__ $$aDe Filippis, N.$$uBari Polytechnic$$vDipartimento Interateneo di Fisica dell'Università e del Politecnico di Bari,INFN Sezione di Bari,Via Orabona 4,70125 Bari,Italy
001416519 700__ $$aDegrassi, G.$$uRome III U.$$vUniversità degli Studi di "Roma Tre" Dipartimento di Fisica Via Vasca Navale 84,00146 Rome,Italy
001416519 700__ $$aDenner, A.$$uWurzburg U.$$vInstitut für Theoretische Physik und Astrophysik,Universität Würzburg,Emil-Hilb-Weg 22,D-97074 Würzburg,Germany
001416519 700__ $$aD'Enterria, D.$$uCERN$$vCERN,CH-1211 Geneva 23,Switzerland
001416519 700__ $$aDiglio, S.$$uMelbourne U.$$vSchool of Physics,University of Melbourne,Victoria,Australia
001416519 700__ $$aDi Micco, B.$$uCERN$$vCERN,CH-1211 Geneva 23,Switzerland
001416519 700__ $$aDi Nardo, R.$$uRome U., Tor Vergata$$vUnivversità di Roma 'Tor Vergata' Dipartimento di Fisica Via della Ricerca Scientifica,1 I-00133 Rome,Italy
001416519 700__ $$aEllis, R.K.$$uFermilab$$vTheoretical Physics Department,Fermi National Accelerator Laboratory MS 106,Batavia,IL 60510-0500,USA
001416519 700__ $$aFarilla, A.$$uRome III U.$$vUniversità degli Studi di "Roma Tre" Dipartimento di Fisica Via Vasca Navale 84,00146 Rome,Italy
001416519 700__ $$aFarrington, S.$$uJAI, UK$$vDepartment of Physics,University of Oxford,Denys Wilkinson Building,Keble Road,Oxford OX1 3RH,UK
001416519 700__ $$aFelcini, M.$$uCantabria Inst. of Phys.$$vInstituto de Física de Cantabria (IFCA),CSIC-Universidad de Cantabria,Santander,Spain
001416519 700__ $$aFerrera, G.$$uMilan U.$$vDipartimento di Fisica,Università degli Studi di Milano and INFN,Sezione di Milano,Via Celoria 16,I-20133 Milan,Italy
001416519 700__ $$aFlechl, M.$$uFreiburg U.$$vPhysikalisches Institut,Albert-Ludwigs-Universität Freiburg,D-79104 Freiburg,Germany
001416519 700__ $$ade Florian, D.$$uBuenos Aires U.$$vDepartamento de Física,Facultad de Ciencias Exactas y Naturales Universidad de Buenos Aires,Pabellon I,Ciudad Universitaria (1428) Capital Federal,Argentina
001416519 700__ $$aForte, S.$$uMilan U.$$vDipartimento di Fisica,Università degli Studi di Milano and INFN,Sezione di Milano,Via Celoria 16,I-20133 Milan,Italy
001416519 700__ $$aGanjour, S.$$uIRFU, Saclay$$vCEA - Centre d'Etudes de Saclay,France
001416519 700__ $$aGarzelli, M.V.$$uDebrecen U.$$uNova Gorica U.$$vInstitute of Physics,University of Debrecen H-4010 Debrecen P.O.Box 105,Hungary$$vUniversity of Nova Gorica,Laboratory for Astroparticle Physics SI-5000 Nova Gorica,Slovenia
001416519 700__ $$aGascon-Shotkin, S.$$uLyon, IPN$$vUniversité Claude Bernard Lyon 1,CNRS-IN2P3,Institut de Physique Nucleaire de Lyon (IPNL) 4,rue Enrico Fermi F-69622 Villeurbanne,CEDEX,France
001416519 700__ $$aGlazov, S.$$uDESY$$vDESY,Notkestrasse 85,D-22607 Hamburg,Germany
001416519 700__ $$aGoria, S.$$uINFN, Turin$$uTurin U.$$vINFN,Sezione di Torino,Via P. Giuria 1,10125 Torino,Italy$$vDipartimento di Fisica Teorica,Università di Torino,Via P. Giuria 1,10125 Torino,Italy
001416519 700__ $$aGrazzini, M.$$uZurich U.$$uINFN, Florence$$vInstitute for Theoretical Physics University of Zurich Winterthurerstrasse 190,CH-8057 Zurich,Switzerland$$vINFN,Sezione di Firenze,Italy
001416519 700__ $$aGuillet, J.-Ph.$$uAnnecy, LAPTH$$vLAPTH,Université de Savoie and CNRS,Annecy-le-Vieux,France
001416519 700__ $$aHackstein, C.$$uKarlsruhe U., TTP$$vInstitut für Theoretische Physik und Institut für Experimentelle Teilchenphysik,Karlsruhe Institut of Technology,D-76131 Karlsruhe,Germany
001416519 700__ $$aHamilton, K.$$uCERN$$vCERN,CH-1211 Geneva 23,Switzerland
001416519 700__ $$aHarlander, R.$$uWuppertal U.$$vBergische Universität Wuppertal,D-42097 Wuppertal,Germany
001416519 700__ $$aHauru, M.$$uHelsinki U.$$vHelsinki Institute of Physics,P.O. Box 64,FIN-00014 University of Helsinki,Finland
001416519 700__ $$aHeinemeyer, S.$$uCantabria Inst. of Phys.$$vInstituto de Física de Cantabria (IFCA),CSIC-Universidad de Cantabria,Santander,Spain
001416519 700__ $$aHöche, S.$$uSLAC$$vSLAC National Accelerator Laboratory,Menlo Park,CA 94025 USA
001416519 700__ $$aHuston, J.$$uMichigan State U.$$vDepartment of Physics and Astronomy,Michigan State University,East Lansing,MI 48824,USA
001416519 700__ $$aJackson, C.$$uTexas U., Arlington$$vDepartment of Physics,Univ. of Texas at Arlington,SH108,University of Texas,Arlington,TX 76019,USA
001416519 700__ $$aJimenez-Delgado, P.$$uZurich U.$$vInstitute for Theoretical Physics University of Zurich Winterthurerstrasse 190,CH-8057 Zurich,Switzerland
001416519 700__ $$aJorgensen, M.D.$$uBohr Inst.$$vNiels Bohr Institute (NBI) University of Copenhagen Blegdamsvej 17 DK-2100 Copenhagen DENMARK
001416519 700__ $$aKado, M.$$uOrsay, LAL$$vLaboratoire de l'Accélérateur Linéaire,CNRS/IN2P3,F-91898 Orsay CEDEX,France
001416519 700__ $$aKallweit, S.$$uZurich U.$$vInstitute for Theoretical Physics University of Zurich Winterthurerstrasse 190,CH-8057 Zurich,Switzerland
001416519 700__ $$aKardos, A.$$uDebrecen U.$$uTexas U., Arlington$$vInstitute of Physics,University of Debrecen H-4010 Debrecen P.O.Box 105,Hungary$$vDepartment of Physics,Univ. of Texas at Arlington,SH108,University of Texas,Arlington,TX 76019,USA
001416519 700__ $$aKauer, N.$$uRoyal Holloway, U. of London$$vDepartment of Physics,Royal Holloway,University of London Egham TW20 0EX,UK
001416519 700__ $$aKim, H.$$uTexas U., Arlington$$vDepartment of Physics,Univ. of Texas at Arlington,SH108,University of Texas,Arlington,TX 76019,USA
001416519 700__ $$aKovac, M.$$uSplit Tech. U.$$vUniversity of Split,FESB,R. Boskovica bb,21 000 Split,Croatia
001416519 700__ $$aKrämer, M.$$uRWTH Aachen U.$$vInstitut für Theoretische Teilchenphysik und Kosmologie,RWTH Aachen University,D-52056 Aachen,Germany
001416519 700__ $$aKrauss, F.$$uDurham U., IPPP$$vInstitute for Particle Physics Phenomenology,Department of Physics,University of Durham,Durham DH1 3LE,UK
001416519 700__ $$aKuo, C.-M.$$uTaiwan, Natl. Central U.$$vNational Central University,Chung-Li,Taiwan
001416519 700__ $$aLehti, S.$$uHelsinki U.$$vHelsinki Institute of Physics,P.O. Box 64,FIN-00014 University of Helsinki,Finland
001416519 700__ $$aLi, Q.$$uPeking U.$$uPeking U., SKLNPT$$vSchool of Physics,and State Key Laboratory of Nuclear Physics and Technology,Peking University,China
001416519 700__ $$aLorenzo, N.$$uOrsay, LAL$$vLaboratoire de l'Accélérateur Linéaire,CNRS/IN2P3,F-91898 Orsay CEDEX,France
001416519 700__ $$aMaltoni, F.$$uLouvain U., CP3$$vCentre for Cosmology,Particle Physics and Phenomenology (CP3),Université Catholique de Louvain,B-1348 Louvain-la-Neuve,Belgium
001416519 700__ $$aMellado, B.$$uWisconsin U., Madison$$vUniv. of Wisconsin Dept. of Physics,High Energy Physics 2506 Sterling Hall 1150 University Ave,Madison,WI 53706
001416519 700__ $$aMoch, S.O.$$uDESY, Zeuthen$$vDESY,Zeuthen,Platanenallee 6,D-15738 Zeuthen,Germany
001416519 700__ $$aMück, A.$$uRWTH Aachen U.$$vInstitut für Theoretische Teilchenphysik und Kosmologie,RWTH Aachen University,D-52056 Aachen,Germany
001416519 700__ $$aMühlleitner, M.$$uKarlsruhe U., TTP$$vInstitut für Theoretische Physik und Institut für Experimentelle Teilchenphysik,Karlsruhe Institut of Technology,D-76131 Karlsruhe,Germany
001416519 700__ $$aNadolsky, P.$$uSouthern Methodist U. (main)$$vSouthern Methodist University Dept. of Physics,Dallas,TX 75275,USA
001416519 700__ $$aNason, P.$$uINFN, Milan Bicocca$$vUniversità di Milano-Bicocca and INFN,Sezione di Milano-Bicocca,Piazza della Scienza 3,20126 Milan,Italy
001416519 700__ $$aNeu, C.$$uVirginia U.$$vUniversity of Virginia,Charlottesville,VA 22906,USA
001416519 700__ $$aNikitenko, A.$$uImperial Coll., London$$vPhysics Dept.,Blackett Laboratory,Imperial College London,Prince Consort Rd,London SW7 2BW,UK
001416519 700__ $$aOleari, C.$$uINFN, Milan Bicocca$$vUniversità di Milano-Bicocca and INFN,Sezione di Milano-Bicocca,Piazza della Scienza 3,20126 Milan,Italy
001416519 700__ $$aOlsen, J.$$uPrinceton U.$$vDepartment of Physics,Princeton University,Princeton,NJ 08542,USA
001416519 700__ $$aPalmer, S.$$uKarlsruhe U., TTP$$vInstitut für Theoretische Physik und Institut für Experimentelle Teilchenphysik,Karlsruhe Institut of Technology,D-76131 Karlsruhe,Germany
001416519 700__ $$aPaganis, S.$$uSheffield U.$$vDept. of Physics and Astronomy University of Sheffield,Sheffield S3 7RH,UK
001416519 700__ $$aPapadopoulos, C.G.$$uDemocritos Nucl. Res. Ctr.$$vNCSR Demokritos,Institute of Nuclear Physics,Athens,Greece
001416519 700__ $$aPetersen, T..C.$$uBohr Inst.$$vNiels Bohr Institute (NBI) University of Copenhagen Blegdamsvej 17 DK-2100 Copenhagen DENMARK
001416519 700__ $$aPetriello, F.$$uArgonne$$uNorthwestern U.$$vHigh Energy Physics Division,Argonne National Laboratory,Argonne,IL 60439,USA$$vDepartment of Physics & Astronomy,Northwestern University,Evanston,IL 60208,USA
001416519 700__ $$aPetrucci, F.$$uRome III U.$$vUniversità degli Studi di "Roma Tre" Dipartimento di Fisica Via Vasca Navale 84,00146 Rome,Italy
001416519 700__ $$aPiacquadio, G.$$uCERN$$vCERN,CH-1211 Geneva 23,Switzerland
001416519 700__ $$aPilon, E.$$uAnnecy, LAPTH$$vLAPTH,Université de Savoie and CNRS,Annecy-le-Vieux,France
001416519 700__ $$aPotter, C.T.$$uOregon U.$$vDepartment of Physics,University of Oregon,Eugene,OR 97403-1274,USA
001416519 700__ $$aPrice, J.$$uLiverpool U.$$vUniversity of Liverpool Dept. of Physics Oliver Lodge Lab,Oxford St. Liverpool L69 3BX UK
001416519 700__ $$aPuljak, I.$$uSplit Tech. U.$$vUniversity of Split,FESB,R. Boskovica bb,21 000 Split,Croatia
001416519 700__ $$aQuayle, W.$$uWisconsin U., Madison$$vUniv. of Wisconsin Dept. of Physics,High Energy Physics 2506 Sterling Hall 1150 University Ave,Madison,WI 53706
001416519 700__ $$aRadescu, V.$$uHeidelberg U.$$vPhysikalisches Institut,Universität Heidelberg,Heidelberg,Germany
001416519 700__ $$aRebuzzi, D.$$uINFN, Pavia$$vUniversità di Pavia and INFN,Sezione di Pavia Via A. Bassi,6,27100 Pavia,Italy
001416519 700__ $$aReina, L.$$uFlorida State U.$$vPhysics Department,Florida State University Tallahassee,FL 32306-4350,USA
001416519 700__ $$aRojo, J.$$uCERN$$vCERN,CH-1211 Geneva 23,Switzerland
001416519 700__ $$aRosco, D.$$uINFN, Turin$$uTurin U.$$vINFN,Sezione di Torino,Via P. Giuria 1,10125 Torino,Italy$$vDipartimento di Fisica Teorica,Università di Torino,Via P. Giuria 1,10125 Torino,Italy
001416519 700__ $$aSalam, G.P.$$uPrinceton U.$$uCERN$$uParis U., VI-VII$$vDepartment of Physics,Princeton University,Princeton,NJ 08542,USA$$vCERN,CH-1211 Geneva 23,Switzerland$$vLaboratoire de Physique Théorique et des Hautes Energies,4 Place Jussieu,F-75252 Paris CEDEX 05,France
001416519 700__ $$aSapronov, A.$$uDubna, JINR$$vJoint Institute for Nuclear Research (JINR),Joliot-Curie st.,6,Dubna,141980 Moscow region,Russia
001416519 700__ $$aSchaarschmidt, J.$$uOrsay, LAL$$vLaboratoire de l'Accélérateur Linéaire,CNRS/IN2P3,F-91898 Orsay CEDEX,France
001416519 700__ $$aSchönherr, M.$$uDurham U., IPPP$$vInstitute for Particle Physics Phenomenology,Department of Physics,University of Durham,Durham DH1 3LE,UK
001416519 700__ $$aSchumacher, M.$$uFreiburg U.$$vPhysikalisches Institut,Albert-Ludwigs-Universität Freiburg,D-79104 Freiburg,Germany
001416519 700__ $$aSiegert, F.$$uFreiburg U.$$vPhysikalisches Institut,Albert-Ludwigs-Universität Freiburg,D-79104 Freiburg,Germany
001416519 700__ $$aSlavich, P.$$uParis U., VI-VII$$vLaboratoire de Physique Théorique et des Hautes Energies,4 Place Jussieu,F-75252 Paris CEDEX 05,France
001416519 700__ $$aSpira, M.$$uPSI, Villigen$$vPaul Scherrer Institut,CH-5232 Villigen PSI,Switzerland
001416519 700__ $$aStewart, I.W.$$uMIT$$vMassachusetts Institute of Technology 77 Massachusetts Avenue Cambridge,MA 02139-4307 USA
001416519 700__ $$aStirling, W.J.$$uCambridge U.$$vCambridge University Dept. of Physics Cavendish Laboratory Cambridge CB3 0HE,UK
001416519 700__ $$aStöckli, F.$$uMIT$$vMassachusetts Institute of Technology 77 Massachusetts Avenue Cambridge,MA 02139-4307 USA
001416519 700__ $$aSturm, C.$$uMunich, Max Planck Inst.$$vMax-Planck-Institut für Physik,Werner-Heisenberg-Institut,Föhringer Ring 6,D-80805 München,Germany
001416519 700__ $$aTackmann, F.J.$$uDESY$$uMIT$$vDESY,Notkestrasse 85,D-22607 Hamburg,Germany$$vMassachusetts Institute of Technology 77 Massachusetts Avenue Cambridge,MA 02139-4307 USA
001416519 700__ $$aThorne, R.S.$$uUniversity Coll. London$$vDepartment of Physics and Astronomy,University College London,Gower Street,London WC1E 6BT,UK
001416519 700__ $$aTommasini, D.$$uZurich U.$$uFlorence U.$$vInstitute for Theoretical Physics University of Zurich Winterthurerstrasse 190,CH-8057 Zurich,Switzerland$$vINFN,Sezione di Firenze and Dipartimento di Fisica e Astronomia,Università di Firenze,I-50019 Sesto Fiorentino,Florence,Italy
001416519 700__ $$aTorrielli, P.$$uLPHE, Lausanne$$vITPP,Lausanne CH-1015 Lausanne,PHB - Ecublens,1015,Lausanne,Switzerland
001416519 700__ $$aTramontano, F.$$uINFN, Naples$$uNaples U.$$vUniversità di Napoli Federico II Dipartimento di Scienze Fisiche via Cintia I-80126 Napoli,Italy
001416519 700__ $$aTrócsányi, Z.$$uDebrecen U.$$uDebrecen, Inst. Nucl. Res.$$vInstitute of Physics,University of Debrecen H-4010 Debrecen P.O.Box 105,Hungary$$vInstitute of Nuclear Research of the Hungarian Academy of Sciences,Hungary
001416519 700__ $$aUbiali, M.$$uRWTH Aachen U.$$vInstitut für Theoretische Teilchenphysik und Kosmologie,RWTH Aachen University,D-52056 Aachen,Germany
001416519 700__ $$aUccirati, S.$$uWurzburg U.$$vInstitut für Theoretische Physik und Astrophysik,Universität Würzburg,Emil-Hilb-Weg 22,D-97074 Würzburg,Germany
001416519 700__ $$aVazquez Acosta, M.$$uImperial Coll., London$$vPhysics Dept.,Blackett Laboratory,Imperial College London,Prince Consort Rd,London SW7 2BW,UK
001416519 700__ $$aVickey, T.$$uU. Witwatersrand, Johannesburg, Sch. Phys.$$uJAI, UK$$vSchool of Physics,University of the Witwatersrand,Private Bag 3,Wits 2050,Johannesburg,South Africa$$vDepartment of Physics,University of Oxford,Denys Wilkinson Building,Keble Road,Oxford OX1 3RH,UK
001416519 700__ $$aVicini, A.$$uMilan U.$$vDipartimento di Fisica,Università degli Studi di Milano and INFN,Sezione di Milano,Via Celoria 16,I-20133 Milan,Italy
001416519 700__ $$aWaalewijn, W.J.$$uUC, San Diego$$vDepartment of Physics,University of California at San Diego,La Jolla,CA 92093,USA
001416519 700__ $$aWackeroth, D.$$uSUNY, Buffalo$$vDepartment of Physics,SUNY at Buffalo,Buffalo,NY 14260-1500,USA
001416519 700__ $$aWarsinsky, M.$$uFreiburg U.$$vPhysikalisches Institut,Albert-Ludwigs-Universität Freiburg,D-79104 Freiburg,Germany
001416519 700__ $$aWeber, M.$$uMunich, Max Planck Inst.$$vMax-Planck-Institut für Physik,Werner-Heisenberg-Institut,Föhringer Ring 6,D-80805 München,Germany
001416519 700__ $$aWiesemann, M.$$uWuppertal U.$$vBergische Universität Wuppertal,D-42097 Wuppertal,Germany
001416519 700__ $$aWeiglein, G.$$uDESY$$vDESY,Notkestrasse 85,D-22607 Hamburg,Germany
001416519 700__ $$aYu, J.$$uTexas U., Arlington$$vDepartment of Physics,Univ. of Texas at Arlington,SH108,University of Texas,Arlington,TX 76019,USA
001416519 700__ $$aZanderighi, G.$$uJAI, UK$$vDepartment of Physics,University of Oxford,Denys Wilkinson Building,Keble Road,Oxford OX1 3RH,UK
001416519 710__ $$gLHC Higgs Cross Section Working Group
001416519 852__ $$cCERN Depot 2, bldg. 2 (DE2)$$hCERN-2012-002
001416519 8564_ $$uhttps://lss.fnal.gov/archive/test-fn/1000/fermilab-fn-1221-t.pdf$$yFermilab Library Server
001416519 8564_ $$82204050$$s5295069$$uhttp://cds.cern.ch/record/1416519/files/arXiv:1201.3084.pdf
001416519 8564_ $$82203980$$s30496$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_generatorComparison_pto1_mh120.png$$y00142 Differential distributions (in arbitrary units) at $7\UTeV$ for Higgs-boson masses $200\UGeV$ (left) and $500 \UGeV$ (right) for three different Monte Carlo generators: \POWHEG{} (black), {\sc HNNLO} (red), \POWHEG{} reweighted with {\sc HqT} and {\sc HNNLO} (blue).
001416519 8564_ $$82203981$$s22703$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_ggZZ_comparison1.png$$y00163 (left) $\MZZ$ distributions for $\Pg\Pg \to \PZ(\PGg^\ast)\PZ(\PGg^\ast) \to \Pl\bar{\Pl}\Pl'\bar{\Pl'}$ calculated with {\sc MCFM}-6.1 (Cut 1: black, Cut 2: blue, Cut 3: red) and {\sc gg2ZZ}-2.0 (Cut 1: green dashed, Cut 2: cyan dashed, Cut 3: magenta dashed), other details as in \refT{tab_ggZZ_comparison:1}; (right) effects of finite $\Pb$ and $\Pt$ masses for the $\MZZ$ distribution of $\Pg\Pg \to \PZ(\PGg^\ast)\PZ(\PGg^\ast) \to \Pl\bar{\Pl}\Pl'\bar{\Pl'}$ when cut set Cut 1 is applied, other details as in \refT{tab_ggZZ_comparison:1}.
001416519 8564_ $$82203982$$s18908$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_ggZZ_comparison2.png$$y00164 (left) $\MZZ$ distributions for $\Pg\Pg \to \PZ(\PGg^\ast)\PZ(\PGg^\ast) \to \Pl\bar{\Pl}\Pl'\bar{\Pl'}$ calculated with {\sc MCFM}-6.1 (Cut 1: black, Cut 2: blue, Cut 3: red) and {\sc gg2ZZ}-2.0 (Cut 1: green dashed, Cut 2: cyan dashed, Cut 3: magenta dashed), other details as in \refT{tab_ggZZ_comparison:1}; (right) effects of finite $\Pb$ and $\Pt$ masses for the $\MZZ$ distribution of $\Pg\Pg \to \PZ(\PGg^\ast)\PZ(\PGg^\ast) \to \Pl\bar{\Pl}\Pl'\bar{\Pl'}$ when cut set Cut 1 is applied, other details as in \refT{tab_ggZZ_comparison:1}.
001416519 8564_ $$82203983$$s21248$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_tanb20-ma120-mu-minus-MSSMvsSM.png$$y00011 \small Left plots: ratio of the transverse momentum-distribution for the lightest scalar $\Ph$ in the MSSM over the distribution for a SM Higgs with the same mass. Right plots: ratio of the transverse-momentum distribution for $\Ph$ in the MSSM over the approximate distribution computed with only quarks running in the loops. The plots are obtained with $\mu&lt;0$, and with three different choices of $\MA$ and $\tan\beta$ for which the MSSM and SM predictions for the total cross section agree within $5\%$.
001416519 8564_ $$82203984$$s36051$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_ma500_tb3_mstw_dyH.png$$y00026 Distribution of Higgs transverse momentum (upper plots) and rapidity (lower plots) for $\tan \beta = 3$, $\MA = 500 \UGeV$ (left plots) and $\tan \beta = 50$, $\MA = 100 \UGeV$ (right plots), comparing the MSSM results with the rescaled SM values with the MSTW2008NLO PDF set.Caption not extracted
001416519 8564_ $$82203985$$s37928$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_VBF_YRHXS2_VBF_COMP_mjjmaxpt.png$$y00096 Di-jet invariant mass (left) and azimuthal separation between the two tagging jets (right). The top plots show the comparison between \HAWK{} (with and without EW corrections), \POWHEG{} QCD and \VBFNLO{} (with EW corrections) for $\MH = 120$\UGeV{} (upper set of curves) and $\MH = 600$\UGeV{} (lower set of curves) for MSTW2008NLO PDF set. The bottom plots display the percentage EW corrections for each of the two mass points.
001416519 8564_ $$82203986$$s77928$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_new-plus-mu-MSSMvsSM.png$$y00010 \small Ratio of the total cross section for $\Ph$ production in the MSSM over the cross section for the production of a SM Higgs boson with the same mass. The plot on the left is for $\mu>0$ while the plot on the right is for $\mu&lt;0$.
001416519 8564_ $$82203987$$s69552$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_BR_YRHXS2_BR_Fig2.png$$y00070 Higgs branching ratios and their uncertainties for the low mass range (left) and for the full mass range (right).
001416519 8564_ $$82203988$$s65299$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_BR_YRHXS2_BR_Fig3.png$$y00071 Higgs branching ratios for the different $\PH \to 4\Pl$ and $\PH \to 2\Pl2\PGn$ final states (left) and for $\PH \to 4\Pq$, $\PH \to 4\Pf$ and $\PH \to 2\Pq2\Pl, 2\Pq \Pl \PGn, 2\Pq 2 \PGn$ final states (right) and their uncertainties for the full mass range.
001416519 8564_ $$82203989$$s6594$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_pth_plot_incl3_7T_rel_Z_YR.png$$y00123 Relative EW corrections for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for the basic cuts at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82203990$$s6024$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_ptV_plot_PDF4LHC_7T_abs_Z_YR.png$$y00109 Predictions for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for boosted Higgs bosons at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82203991$$s40355$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_BR_YRHXS2_BR_Fig6.png$$y00074 Higgs branching ratios for the light MSSM Higgs boson for the relevant final states. The parameters are chosen according to the \mhmaxx\ scenario, see \Eref{YRHXS_MSSM_neutral_eq:mhmax}, with $\tb = 10 (50)$ in the left (right) plot.
001416519 8564_ $$82203992$$s40688$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_BR_YRHXS2_BR_Fig7.png$$y00075 Higgs branching ratios for the light MSSM Higgs boson for the relevant final states. The parameters are chosen according to the \mhmaxx\ scenario, see \Eref{YRHXS_MSSM_neutral_eq:mhmax}, with $\tb = 10 (50)$ in the left (right) plot.
001416519 8564_ $$82203993$$s63663$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_BR_YRHXS2_BR_Fig4.png$$y00072 Higgs branching ratios for the different $\PH \to 4\Pl$ and $\PH \to 2\Pl2\PGn$ final states (left) and for $\PH \to 4\Pq$, $\PH \to 4\Pf$ and $\PH \to 2\Pq2\Pl, 2\Pq \Pl \PGn, 2\Pq 2 \PGn$ final states (right) and their uncertainties for the full mass range.
001416519 8564_ $$82203994$$s67837$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_BR_YRHXS2_BR_Fig5.png$$y00073 The ratio between formula \refE{approx} and \Prophecy\ for $\PH \to \PZ\PZ \to \Pl\PAl\Pl\PAl$ (top-left), $\PH \to \PW\PW/\PZ\PZ \to \Pl\PGn\Pl\PGn$ (top-right), $\PH \to \PZ\PZ \to \Pl\PAl\PQq\PAQq, \PH \to \PW\PW \to \Pl\PGn\PQq\PAQq$ (bottom-left), and $\PH \to \PZ\PZ \to \PGn\PAGn\PQq\PAQq, \PH \to \PW\PW/\PZ\PZ \to \PQq\PAQq\PQq\PAQq$ (bottom-right).
001416519 8564_ $$82203995$$s36304$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_fig_DRbb_A_ps.png$$y00193 Separation in pseudo-rapidity and azimuthal angle of the two hardest lowest-lying B hadrons in the events (no-cut analysis) (\textit{left}) and invariant mass of all jet pairs passing the set 3) of cuts (\textit{right}). The different regions of the plots are defined as in Fig.~\protect\ref{fig:ttH_nlomc_fig1}. See text for more details.
001416519 8564_ $$82203996$$s28280$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_x_H.png$$y00169 (a) Distribution of $\cos(\theta^*_{\PH,\PZ})$ for Higgs events with $\MH=120 \UGeV$ and $\ZZ$ di-boson events. (b) Distribution of $x_{\PH}$ (the sum of the $\PZ$ masses divided by the Higgs mass) for the same samples.
001416519 8564_ $$82203997$$s25422$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_ptH_45FS_gnu.png$$y00056 \sloppy Normalised transverse-momentum distributions of the Higgs boson (a) and the top quark (b) for $\Pp\Pp \to {\rm t}\PAQb{\rm H}^-+X$ at the LHC ($14\UTeV$). Shown are results in the 4FS (NLO) and 5FS (NLO plus parton shower).
001416519 8564_ $$82203998$$s31941$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_generatorComparison_eta1_mh500.png$$y00151 Differential distributions (in arbitrary units) at $7\UTeV$ for Higgs-boson masses $200\UGeV$ (left) and $500\UGeV$ (right) for three different Monte Carlo generators: \POWHEG{} (black), {\sc HNNLO} (red), \POWHEG{} reweighted with {\sc HqT} and {\sc HNNLO} (blue).
001416519 8564_ $$82203999$$s19518$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_GG_azim.png$$y00086 Differential diphoton cross section as a function of $\Delta\phi_{\PGg\PGg}$ at NNLO (blue) and at NLO (dotted black) calculated with a preliminary result from the {\sc 2gammaNNLO} program, superimposed on results from CMS data (points) from 2010~\cite{Chatrchyan:2011qt}.
001416519 8564_ $$82204000$$s41043$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_ma500_tb3_mstw_dpTH.png$$y00024 None
001416519 8564_ $$82204001$$s42596$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_ZZ_fig2.png$$y00155 (Left) The cross sections for $\ZZ^{(*)}$ production as a function of ${\mathswitch {m_{2\Pe 2\PGm}}}$ at $7\UTeV$ from {\sc MCFM} at NLO; (right) cross sections for $\ZZ^{(*)}$ production as a function of ${\mathswitch {m_{2\Pe 2\PGm}}}$ at $7\UTeV$ from {\sc MCFM} at NLO for three different sets of cuts as described in the text.
001416519 8564_ $$82204002$$s23484$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_dsdR_ttb_perc_err_band.png$$y00180 Theoretical uncertainty on the top-antitop quark $(\eta,\phi)$ distance ($R(\PQt,\PAQt)$) distribution: the l.h.s.\ shows the actual distributions, the r.h.s.\ the spread around the central value in per cent. A detailed explanation of the red and blue bands is given in the text.
001416519 8564_ $$82204003$$s32021$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_YRHXS2_ZZ_Fig1_bottom.png$$y00138 (Left) $\pT$ spectrum of the SM Higgs boson of mass $\MH=130 \UGeV$ produced via gluon-gluon fusion as obtained by using the \POWHEG{} generator (and {\sc PYTHIA} for parton shower, hadronisation and underlying event) and {\sc HqT} tool. (Right) the ratio {\sc Hqt} vs \POWHEG{} as a function of the Higgs-boson $\pT$.
001416519 8564_ $$82204004$$s6278$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_pth_plot_PDF4LHC_7T_abs_Z_YR.png$$y00107 Predictions for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for boosted Higgs bosons at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82204005$$s31923$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_ggHAcceptancePtElec400.png$$y00017 Generated $\pT^{\Pe}$ and $\pT^{\PGt}$ distributions for $\MH = 140 \UGeV$ (left) and $\MH = 400 \UGeV$ (right) for the $\Pg\Pg \to \PH$ process generated with {\sc PYTHIA} (dashed) and after re-weighting (solid) to correct for $\Pg\Pg \to \PH$ production dominated by the $\Pb$-loop contribution.
001416519 8564_ $$82204006$$s32084$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_dsdpt_H_err_band.png$$y00175 Theoretical uncertainty on Higgs-boson transverse momentum ($\pT^{\PH}$) distribution: the l.h.s.\ shows the actual distributions, the r.h.s.\ the spread around the central value in per cent. A detailed explanation of the red and blue bands is given in the text.
001416519 8564_ $$82204007$$s12507$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_pTb400.png$$y00031 The $\pT$ distributions of the leading $\pT$ b-jet normalised on unity for $\MH=140\UGeV$ (left) and $\MH=400\UGeV$ (right) obtained with {\sc PYTHIA} (solid lines) and with NLO calculations (dashed lines).
001416519 8564_ $$82204008$$s31544$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_fig_rates_ps.png$$y00191 Total rates for pseudo-scalar Higgs boson production after the different cuts defined in the text (\textit{left}) and transverse momentum of the pseudo-scalar Higgs boson (\textit{right}) in the no-cut configuration. The different regions of the plots are defined as in Fig.~\protect\ref{fig:ttH_nlomc_fig1}. See text for more details.
001416519 8564_ $$82204009$$s41694$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_generatorComparison_mZ2_mh500.png$$y00147 Differential distributions (in arbitrary units) at $7\UTeV$ for Higgs-boson masses $200\UGeV$ (left) and $500 \UGeV$ (right) for three different Monte Carlo generators: \POWHEG{} (black), {\sc HNNLO} (red), \POWHEG{} reweighted with {\sc HqT} and {\sc HNNLO} (blue).
001416519 8564_ $$82204010$$s30892$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_xs4f5fhks.png$$y00007 \sloppy (a) Weight factor $w$, \eqn{eq::tn}, as a function of the Higgs-boson mass $\MH$. The bottom-quark pole mass has been set to $\Mb = 4.75 \UGeV$. (b) Central values for the total inclusive cross section in the 4FS (red, dashed), the 5FS (green, dotted), and for the Santander-matched cross section (blue, solid). Here and in the following we use the MSTW2008\, PDF set~\cite{Martin:2009iq} (NLO for the 4FS, NNLO for the 5FS).
001416519 8564_ $$82204011$$s20214$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_dsdeta_t_perc_err_band.png$$y00174 Theoretical uncertainty on top(antitop)-quark pseudorapidity ($\eta^{\PQt}$) distribution: the l.h.s.\ shows the actual distributions, the r.h.s.\ the spread around the central value in per cent. A detailed explanation of the red and blue bands is given in the text.
001416519 8564_ $$82204012$$s27377$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_dGammatHpb_01.png$$y00040 Caption not extracted
001416519 8564_ $$82204013$$s13265$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_yb400.png$$y00029 The rapidity distributions of the leading $\pT$ b-jet normalised on unity for $\MH=140\UGeV$ (left) and $\MH=400\UGeV$ (right) obtained with {\sc PYTHIA} (solid lines) and with NLO calculations (dashed lines).
001416519 8564_ $$82204014$$s31858$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_ggHAcceptancePtTau140.png$$y00018 Generated $\pT^{\Pe}$ and $\pT^{\PGt}$ distributions for $\MH = 140 \UGeV$ (left) and $\MH = 400 \UGeV$ (right) for the $\Pg\Pg \to \PH$ process generated with {\sc PYTHIA} (dashed) and after re-weighting (solid) to correct for $\Pg\Pg \to \PH$ production dominated by the $\Pb$-loop contribution.
001416519 8564_ $$82204015$$s39501$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_fig_mjj_cut3.png$$y00189 Invariant mass of all jet pairs passing the cuts of set 3) (\textit{left}) and transverse energy of the hardest positively-charged lepton (\textit{right}). The different regions of the plots are defined as in Fig.~\protect\ref{fig:ttH_nlomc_fig1}. See text for more details.
001416519 8564_ $$82204016$$s43816$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_YRHXS2_chiggs_fig4a.png$$y00042 The decay width of $\PSHpm$ calculated with {\sc FeynHiggs} and {\sc HDECAY} as a function of $\tan\beta$ for different values of $\mu$ and $\MHpm$.
001416519 8564_ $$82204017$$s20341$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_tanb44-ma140-mu-minus-MSSMvsMSSMONLYQUARKS.png$$y00013 \small Left plots: ratio of the transverse momentum-distribution for the lightest scalar $\Ph$ in the MSSM over the distribution for a SM Higgs with the same mass. Right plots: ratio of the transverse-momentum distribution for $\Ph$ in the MSSM over the approximate distribution computed with only quarks running in the loops. The plots are obtained with $\mu&lt;0$, and with three different choices of $\MA$ and $\tan\beta$ for which the MSSM and SM predictions for the total cross section agree within $5\%$.
001416519 8564_ $$82204018$$s12628$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_sm4_br_sm4_ratio.png$$y00060 Ratio of branching fractions in SM4 with respect to SM3 for $\PW\PW$, $\PZ\PZ$, $\Pg\Pg$, $\PQb\bar{\PQb}$, and $\PGg\PGg$ decay channels ($\PGg\PGg$ ratio multiplied with $100$).
001416519 8564_ $$82204019$$s21596$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_tanb20-ma120-mu-minus-MSSMvsMSSMONLYQUARKS.png$$y00017 \small Left plots: ratio of the transverse momentum-distribution for the lightest scalar $\Ph$ in the MSSM over the distribution for a SM Higgs with the same mass. Right plots: ratio of the transverse-momentum distribution for $\Ph$ in the MSSM over the approximate distribution computed with only quarks running in the loops. The plots are obtained with $\mu&lt;0$, and with three different choices of $\MA$ and $\tan\beta$ for which the MSSM and SM predictions for the total cross section agree within $5\%$.
001416519 8564_ $$82204020$$s5886$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_ptlp_plot_PDF4LHC_7T_abs_Z_YR.png$$y00111 Predictions for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for boosted Higgs bosons at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82204021$$s39700$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_matcheduncertaintyand4f5fcentral.png$$y00009 \sloppy (a) Theory uncertainty bands for the total inclusive cross section in the 4FS (red, dashed), the 5FS (green, dotted), and for the Santander-matched cross section (blue, solid). (b) Uncertainty bands and central values, relative to the central value of the Santander-matched result (same line coding as panel (a)).
001416519 8564_ $$82204022$$s35380$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_ma100_tb50_mstw_dpTH.png$$y00025 None
001416519 8564_ $$82204023$$s29178$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_Cos_theta_H_Z.png$$y00168 (a) Distribution of $\cos(\theta^*_{\PH,\PZ})$ for Higgs events with $\MH=120 \UGeV$ and $\ZZ$ di-boson events. (b) Distribution of $x_{\PH}$ (the sum of the $\PZ$ masses divided by the Higgs mass) for the same samples.
001416519 8564_ $$82204024$$s23158$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_dsdpt_H_perc_err_band.png$$y00176 Theoretical uncertainty on Higgs-boson transverse momentum ($\pT^{\PH}$) distribution: the l.h.s.\ shows the actual distributions, the r.h.s.\ the spread around the central value in per cent. A detailed explanation of the red and blue bands is given in the text.
001416519 8564_ $$82204025$$s53010$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_CUT1_POWHEG_MCFM_LHC.png$$y00156 $ZZ\rightarrow 2\Pe 2\PGm$ invariant-mass distributions at $7 \UTeV$ with \POWHEG{} and {\sc MCFM v6.1}. Two different PDF sets are used. The top-left plot is obtained applying only ${\mathswitch {m_{2l}}}>12 \UGeV$; the top-right plot asking $\mzonshell >50 \UGeV$, $\mzoffshell>12 \UGeV$, $\pT(\Pl)>5 \UGeV$, $|\eta(\Pl)|&lt;2.5$, and the bottom plot asking $60 &lt;\mzonshell&lt;120 \UGeV$ and $60 &lt;\mzoffshell&lt;120 \UGeV$.
001416519 8564_ $$82204026$$s6189$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_yh_plot_boosted3_7T_abs_W_YR.png$$y00112 Predictions for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for boosted Higgs bosons at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82204027$$s43899$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_totalxs_7TeV_santander_error_gnu.png$$y00055 \sloppy (a) Central values for the total inclusive cross section in the 5FS (red, dashed), the 4FS (green, dashed), and for the matched cross section (blue, solid). Here and in the following we use the MSTW2008\, PDF set~\cite{Martin:2009iq}. (b) Theory uncertainty bands for the total inclusive cross section in the 5FS (red, dashed), the 4FS (green, dashed), and for the matched cross section (blue, solid).
001416519 8564_ $$82204028$$s8952$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_ptlpm_plot_boosted3_7T_rel_W_YR.png$$y00118 Relative EW corrections for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for boosted Higgs bosons at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82204029$$s34125$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_generatorComparison_eta1_mh120.png$$y00150 Differential distributions (in arbitrary units) at $7\UTeV$ for Higgs-boson masses $200\UGeV$ (left) and $500\UGeV$ (right) for three different Monte Carlo generators: \POWHEG{} (black), {\sc HNNLO} (red), \POWHEG{} reweighted with {\sc HqT} and {\sc HNNLO} (blue).
001416519 8564_ $$82204030$$s37943$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_generatorComparison_mZ1_mh120.png$$y00144 Differential distributions (in arbitrary units) at $7\UTeV$ for Higgs-boson masses $200\UGeV$ (left) and $500 \UGeV$ (right) for three different Monte Carlo generators: \POWHEG{} (black), {\sc HNNLO} (red), \POWHEG{} reweighted with {\sc HqT} and {\sc HNNLO} (blue).
001416519 8564_ $$82204031$$s23731$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_dsdR_tH_perc_err_band.png$$y00182 Theoretical uncertainty on top-Higgs $(\eta,\phi)$ distance ($R(\PQt,\PH)$) distribution in the no-cut configuration: the l.h.s.\ shows the actual distributions, the r.h.s.\ the spread around the central value in per cent. A detailed explanation of the red and blue bands is given in the text.
001416519 8564_ $$82204032$$s40164$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_CUT1_CT10_MSTW_LHC.png$$y00159 $\ZZ\rightarrow 2\Pe 2\PGm$ and $\ZZ\rightarrow 4\Pe$ invariant-mass distributions and their ratio at $7\UTeV$ with \POWHEG{}. Two different PDF sets are used. The upper plots are obtained applying only ${\mathswitch {m_{2\Pl}}}>12 \UGeV$, the middle plots applying $\mzonshell>50 \UGeV$, $\mzoffshell>12 \UGeV$, $\pT(\Pl)>5 \UGeV$, $|\eta(\Pl)|&lt;2.5$, and the bottom plots applying $60 &lt;\mzonshell&lt;120 \UGeV$ and $60 &lt;\mzoffshell&lt;120 \UGeV$.
001416519 8564_ $$82204033$$s31382$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_generatorComparison_ptH_mh120.png$$y00140 Differential distributions (in arbitrary units) at $7\UTeV$ for Higgs-boson masses $200\UGeV$ (left) and $500 \UGeV$ (right) for three different Monte Carlo generators: \POWHEG{} (black), {\sc HNNLO} (red), \POWHEG{} reweighted with {\sc HqT} and {\sc HNNLO} (blue).
001416519 8564_ $$82204034$$s23372$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_VBF_YRHXS2_VBF_PWG_yj3.png$$y00100 Rapidity distribution of the third hardest jet, $y_{j_3}$ (left) and exclusive jet-multiplicity (right).  We show the comparison among NLO QCD and the \POWHEG{} interfaced to \HERWIG{} and \PYTHIA{} results.
001416519 8564_ $$82204035$$s21567$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_tanb44-ma140-mu-minus-MSSMvsSM.png$$y00020 \small Left plots: ratio of the transverse momentum-distribution for the lightest scalar $\Ph$ in the MSSM over the distribution for a SM Higgs with the same mass. Right plots: ratio of the transverse-momentum distribution for $\Ph$ in the MSSM over the approximate distribution computed with only quarks running in the loops. The plots are obtained with $\mu&lt;0$, and with three different choices of $\MA$ and $\tan\beta$ for which the MSSM and SM predictions for the total cross section agree within $5\%$.
001416519 8564_ $$82204036$$s42317$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_sm4_YRHXS2_HLS_fig3.png$$y00062 In the left figure we show a comparison of production cross section as computed with the OFFP-scheme of \eqn{offp} or with the OFFBW-scheme of \eqn{offbw}. The red curve gives Breit--Wigner parameters in the OS-scheme and the blue one in the Bar-scheme of \eqn{Bars}. In the right figure we show the effect of using dynamical QCD scales for the production cross section of \eqns{PDFprod_1}{PDFprod_3}.
001416519 8564_ $$82204037$$s53723$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_sm4_YRHXS2_HLS_fig2.png$$y00061 In the left figure we show a comparison of production cross section as computed with the OFFP-scheme of \eqn{offp} or with the OFFBW-scheme of \eqn{offbw}. The red curve gives Breit--Wigner parameters in the OS-scheme and the blue one in the Bar-scheme of \eqn{Bars}. In the right figure we show the effect of using dynamical QCD scales for the production cross section of \eqns{PDFprod_1}{PDFprod_3}.
001416519 8564_ $$82204038$$s62583$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_sm4_YRHXS2_HLS_fig4.png$$y00063 In the left figure the blue curve gives the off-shell production cross section sampled over the (complex) Higgs propagator while the red curves is sampled over a Breit--Wigner distribution The right figure showes differential $K$~factor for the process $\Pp\Pp \to (\PH \to 4\,\Pe) + \PX$, comparing the fixed scale option, $\muR = \muF = \MH/2$, and the running scale option, $\muR = \muF = M(4\,\Pe)/2$.
001416519 8564_ $$82204039$$s34640$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_sm4_YRHXS2_HLS_fig7.png$$y00065 The normalised invariant-mass distribution in the OFFP-scheme with running QCD scales (left) for $600\UGeV$ (black), $700\UGeV$ (blue), $800\UGeV$ (red) in the windows $M_{\peak} \pm 2\,\GOS$. The normalised invariant-mass distribution in the OFFP-scheme (blue) and OFFBW-scheme (red) with running QCD scales (right) at $800\UGeV$ in the window $M_{\peak} \pm 2\,\GOS$.
001416519 8564_ $$82204040$$s45112$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_sm4_YRHXS2_HLS_fig6.png$$y00064 In the left figure the blue curve gives the off-shell production cross section sampled over the (complex) Higgs propagator while the red curves is sampled over a Breit--Wigner distribution The right figure showes differential $K$~factor for the process $\Pp\Pp \to (\PH \to 4\,\Pe) + \PX$, comparing the fixed scale option, $\muR = \muF = \MH/2$, and the running scale option, $\muR = \muF = M(4\,\Pe)/2$.
001416519 8564_ $$82204041$$s39822$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_YR2HXS_figZZd.png$$y00003 Caption not extracted
001416519 8564_ $$82204042$$s31203$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_sm4_YRHXS2_HLS_fig8.png$$y00066 The normalised invariant-mass distribution in the OFFP-scheme with running QCD scales (left) for $600\UGeV$ (black), $700\UGeV$ (blue), $800\UGeV$ (red) in the windows $M_{\peak} \pm 2\,\GOS$. The normalised invariant-mass distribution in the OFFP-scheme (blue) and OFFBW-scheme (red) with running QCD scales (right) at $800\UGeV$ in the window $M_{\peak} \pm 2\,\GOS$.
001416519 8564_ $$82204043$$s53009$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_YRHXS2_chiggs_fig6c.png$$y00052 The decay width $\Gamma(\PH^{\pm} \to \PQc\PQs)$ calculated with {\sc FeynHiggs} and {\sc HDECAY} as a function of $\tan\beta$ for different values of $\mu$ and $M_{\PH^{\pm}}$. A discrepancy of $7{-}19\%$ is observed.
001416519 8564_ $$82204044$$s52882$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_YRHXS2_chiggs_fig6b.png$$y00051 The decay width $\Gamma(\PH^{\pm} \to \PQc\PQs)$ calculated with {\sc FeynHiggs} and {\sc HDECAY} as a function of $\tan\beta$ for different values of $\mu$ and $M_{\PH^{\pm}}$. A discrepancy of $7{-}19\%$ is observed.
001416519 8564_ $$82204045$$s26233$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_GenMHiggs_Powheg_v_Pythia_150GeV_gg_cut2.png$$y00132 Higgs-boson transverse momentum and mass spectrum derived with \PYTHIA~(LO) and \POWHEG\ (NLO) generators for the four-lepton final state from the decay of the Higgs boson with mass $\MH=150 \UGeV$, asking $\mzonshell >50 \UGeV$, $\mzoffshell >12 \UGeV$ and $\pT>5 \UGeV$, $|\eta|&lt;2.5$. Plots are normalised to the same area.
001416519 8564_ $$82204046$$s47483$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_YR2HXS_figZZa.png$$y00000 Caption not extracted
001416519 8564_ $$82204047$$s42698$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_YR2HXS_figZZb.png$$y00001 Caption not extracted
001416519 8564_ $$82204048$$s43063$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_YR2HXS_figZZc.png$$y00002 Ratios of the total MSSM production cross sections via gluon fusion and Higgs radiation off bottom quarks within the 5FS for $\sqrt{s}=7$\UTeV\ using NNLO and NLO MSTW2008 PDFs \cite{Martin:2009iq,Martin:2009bu} for the \mhmaxx\ scenario with different $\mu$ values relative to the central prediction with $\mu=200 \UGeV$; (a) gluon fusion for $\tanb=5$, (b) gluon fusion for $\tanb=30$, (c) Higgs radiation off bottom quarks for $\tanb=5$, (d) Higgs radiation off bottom quarks for $\tanb=30$.Caption not extracted
001416519 8564_ $$82204049$$s40034$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_fig_ptt_cut1.png$$y00187 Transverse momentum of the top quark in the boosted-Higgs scenario (\textit{left}) and scalar sum of transverse energies (\textit{right}) under the cuts of set 2). The different regions of the plots are defined as in Fig.~\protect\ref{fig:ttH_nlomc_fig1}. See text for more details.
001416519 8564_ $$82204051$$s5436$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_yh_plot_boosted3_7T_rel_Z_YR.png$$y00121 Relative EW corrections for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for boosted Higgs bosons at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82204052$$s23874$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_VBF_YRHXS2_VBF_PWG_ptrelj1.png$$y00102 Relative transverse momentum $\pT^{{\rm rel},j_1}$ of all the particles clustered inside the first tagging jet, in the reference frame where the jet has zero rapidity, defined according to \Eref{eq:VBF_def_ptrel} (left) and probability of finding a veto jet defined as in \Eref{eq:VBF_P_veto} as a function of $\pT{}_{\rm ,veto}$ (right). We show the comparison among NLO QCD and the \POWHEG{} interfaced to \HERWIG{} and \PYTHIA{} results. In addition, on the right plot, we show the NLO QCD results obtained with $\muR=\muF=\MW/2$ and $\muR=\muF=2\MW$.
001416519 8564_ $$82204053$$s33036$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_dsdR_ttb_err_band.png$$y00179 Theoretical uncertainty on the top-antitop quark $(\eta,\phi)$ distance ($R(\PQt,\PAQt)$) distribution: the l.h.s.\ shows the actual distributions, the r.h.s.\ the spread around the central value in per cent. A detailed explanation of the red and blue bands is given in the text.
001416519 8564_ $$82204054$$s13245$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_tTbB_mbb100_ptb-hard_abs.png$$y00195 Transverse momentum of the harder ($p_{\mathrm{T},\PQb_1}$) and softer ($p_{\mathrm{T},\PQb_2}$) $b$ jets at $14\UTeV$ CM energy: absolute LO and NLO prediction for the unboosted ($m_{\PQb\PAQb}>100\UGeV$, upper plots) and boosted regimes ($p_{T,\PQb\PAQb}>200\UGeV$, lower plots). The uncertainty bands correspond to a factor two scale variation. From \Bref{Bredenstein:2010rs}.
001416519 8564_ $$82204055$$s19781$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_GG_azimcms.png$$y00088 Differential diphoton cross section as a function of $\Delta\phi_{\PGg\PGg}$ at NNLO (blue) and at NLO (dotted black) calculated with a preliminary result from the {\sc 2gammaNNLO} program, for the 'ATLAS' (left) and 'CMS' (right) acceptance criteria.
001416519 8564_ $$82204056$$s38547$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_fig_ptH_ps.png$$y00192 Total rates for pseudo-scalar Higgs boson production after the different cuts defined in the text (\textit{left}) and transverse momentum of the pseudo-scalar Higgs boson (\textit{right}) in the no-cut configuration. The different regions of the plots are defined as in Fig.~\protect\ref{fig:ttH_nlomc_fig1}. See text for more details.
001416519 8564_ $$82204057$$s6403$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_pth_plot_boosted3_7T_abs_W_YR.png$$y00106 Predictions for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for boosted Higgs bosons at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82204058$$s19585$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_GG_azimatlas.png$$y00087 Differential diphoton cross section as a function of $\Delta\phi_{\PGg\PGg}$ at NNLO (blue) and at NLO (dotted black) calculated with a preliminary result from the {\sc 2gammaNNLO} program, for the 'ATLAS' (left) and 'CMS' (right) acceptance criteria.
001416519 8564_ $$82204059$$s19237$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_BDTResponse.png$$y00170 Separation between $\PH \rightarrow \ZZ$ and SM di-boson $\ZZ$ using five angular variables combined in a Boosted Decision Tree (BDT).
001416519 8564_ $$82204060$$s40417$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_fig_ptH.png$$y00184 Total rates for scalar-Higgs-boson production after the different cuts defined in the text (\textit{left}) and transverse momentum of the Higgs boson (\textit{right}) in the no-cut configuration. In the upper inset the scale and PDF uncertainties computed by a\MCNLO{} interfaced to \HERWIG{} are shown. The lower inset displays the ratio of \powheghelac{} over a\MCNLO{} and the ratio between the results computed by interfacing \powheghelac{} to \PYTHIA{} and \HERWIG{}. See text for more details.
001416519 8564_ $$82204061$$s6740$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_pth_plot_boosted3_7T_rel_W_YR.png$$y00114 Relative EW corrections for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for boosted Higgs bosons at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82204062$$s16419$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_pTbb_pp.png$$y00200 Distribution of the invariant mass $m_{\PQb\PAQb}$ of the bottom-anti-bottom pair (a), distribution in the transverse momentum $p_{\mathrm{T}_{\PQb\PAQb}}$ of the bottom-anti-bottom pair (b), distribution in the rapidity $y_{\PQb\PAQb}$ of the bottom--anti-bottom pair (c), and distribution in the transverse momentum $p_{\mathrm{T},\PQb}$ of the bottom quark (d) for $\Pp\Pp\rightarrow \PQt\PAQt\PH \rightarrow \PQt\PAQt\PQb\PAQb +X$ and $\Pp\Pp\rightarrow \PQt\PAQt\PQb\PAQb+X$ at the LHC for the CM energy of $14\UTeV$. The red solid line refers to the NLO QCD background, the blue dotted line to the LO QCD background, while the green dash-dotted and cyan dashed line to the NLO and LO signal, respectively. From \Bref{Binoth:2010ra}.
001416519 8564_ $$82204063$$s39829$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_YRHXS2_ZZ_Fig1_top.png$$y00137 (Left) $\pT$ spectrum of the SM Higgs boson of mass $\MH=130 \UGeV$ produced via gluon-gluon fusion as obtained by using the \POWHEG{} generator (and {\sc PYTHIA} for parton shower, hadronisation and underlying event) and {\sc HqT} tool. (Right) the ratio {\sc Hqt} vs \POWHEG{} as a function of the Higgs-boson $\pT$.
001416519 8564_ $$82204064$$s40728$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_fig_mbb_A.png$$y00186 Transverse momentum of the Higgs--top--antitop system (\textit{left}) and invariant mass of the two hardest lowest-lying B hadrons (\textit{right}). The different regions of the plots are defined as in \protect\refF{fig:ttH_nlomc_fig1}. See text for more details.
001416519 8564_ $$82204065$$s21352$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_tanb24-ma125-mu-minus-MSSMvsMSSMONLYQUARKS.png$$y00019 \small Left plots: ratio of the transverse momentum-distribution for the lightest scalar $\Ph$ in the MSSM over the distribution for a SM Higgs with the same mass. Right plots: ratio of the transverse-momentum distribution for $\Ph$ in the MSSM over the approximate distribution computed with only quarks running in the loops. The plots are obtained with $\mu&lt;0$, and with three different choices of $\MA$ and $\tan\beta$ for which the MSSM and SM predictions for the total cross section agree within $5\%$.
001416519 8564_ $$82204066$$s34907$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_ma500_tb3_mstw_dphi.png$$y00020 None
001416519 8564_ $$82204067$$s11895$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_tTbB_ptbb200_ptb-soft_abs.png$$y00198 Transverse momentum of the harder ($p_{\mathrm{T},\PQb_1}$) and softer ($p_{\mathrm{T},\PQb_2}$) $b$ jets at $14\UTeV$ CM energy: absolute LO and NLO prediction for the unboosted ($m_{\PQb\PAQb}>100\UGeV$, upper plots) and boosted regimes ($p_{T,\PQb\PAQb}>200\UGeV$, lower plots). The uncertainty bands correspond to a factor two scale variation. From \Bref{Bredenstein:2010rs}.
001416519 8564_ $$82204068$$s6034$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_pth_plot_boosted3_7T_rel_Z_YR.png$$y00115 Relative EW corrections for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for boosted Higgs bosons at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82204069$$s94473$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_qqZZ.png$$y00153 (left) The cross sections for $\PQq\PAQq\rightarrow \ZZ^{(*)}\rightarrow{2\Pe 2\PGm}$ as a function of ${\mathswitch {m_{2\Pe 2\PGm}}}$ at $7\UTeV$ from {\sc MCFM} for the full calculation and without the singly-resonant contribution; (right) LO cross sections for $\PQq\PAQq\rightarrow \ZZ^{(*)}\rightarrow {2\Pe 2\PGm}$ as a function of ${\mathswitch {m_{2\Pe 2\PGm}}}$ at $7\UTeV$ from {\sc MCFM} at LO.
001416519 8564_ $$82204070$$s25348$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_GG_KfactorApplied_HNNLO_POWHEG_H120_qt.png$$y00081 Differential cross sections of the $\Pg\Pg\rightarrow \PH\rightarrow \PGg\PGg$ process for $\MH=120\UGeV$: Higgs-boson transverse momentum (top left), Higgs-boson rapidity (top right), and $\cos\theta^{*}$ (bottom) for HNNLO, {\sc POWHEG}, and {\sc POWHEG} reweighted with $K(\qTH,\YH)$.
001416519 8564_ $$82204071$$s26860$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_SignalAcc_Pdf+alphas_uncertainty.png$$y00134 The difference between the central value of the acceptance for four-lepton events and the acceptance computed with plus and minus $1\,\sigma$ of the total PDF+$\alphas$ variation (blue markers), following the PDF4LHC prescription; the circles markers correspond to the ratio between central value of CT10, MSTW, and NNPDF and the middle value of the envelope.
001416519 8564_ $$82204072$$s32142$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_generatorComparison_pto1_mh500.png$$y00143 Differential distributions (in arbitrary units) at $7\UTeV$ for Higgs-boson masses $200\UGeV$ (left) and $500 \UGeV$ (right) for three different Monte Carlo generators: \POWHEG{} (black), {\sc HNNLO} (red), \POWHEG{} reweighted with {\sc HqT} and {\sc HNNLO} (blue).
001416519 8564_ $$82204073$$s23013$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_GG_KfactorApplied_PromptPromptNLO_mgg.png$$y00090 Differential cross sections for diphoton production from the sum of the quark--antiquark annihilation, gluon-fusion, and gluon--(anti)quark scattering processes: Diphoton transverse momentum (top left), diphoton invariant mass (top right), and $\cos\theta^{*}$ (bottom) for a combination of {\sc Diphox} and {\sc Gamma2MC}, a combination of {\sc Madgraph} and {\sc PYTHIA}, and the latter combination reweighted with $K(M_{\PGg\PGg},\qTH)$.
001416519 8564_ $$82204074$$s41296$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_fig_Ht_cut2.png$$y00188 Transverse momentum of the top quark in the boosted-Higgs scenario (\textit{left}) and scalar sum of transverse energies (\textit{right}) under the cuts of set 2). The different regions of the plots are defined as in Fig.~\protect\ref{fig:ttH_nlomc_fig1}. See text for more details.
001416519 8564_ $$82204075$$s5134$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_yh_plot_incl3_7T_rel_Z_YR.png$$y00129 Relative EW corrections for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for the basic cuts at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82204076$$s11766$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_tTbB_ptbb200_ptb-hard_abs.png$$y00197 Transverse momentum of the harder ($p_{\mathrm{T},\PQb_1}$) and softer ($p_{\mathrm{T},\PQb_2}$) $b$ jets at $14\UTeV$ CM energy: absolute LO and NLO prediction for the unboosted ($m_{\PQb\PAQb}>100\UGeV$, upper plots) and boosted regimes ($p_{T,\PQb\PAQb}>200\UGeV$, lower plots). The uncertainty bands correspond to a factor two scale variation. From \Bref{Bredenstein:2010rs}.
001416519 8564_ $$82204077$$s49617$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_VBF_YRHXS2_VBF_VBFNLO_xsecvspt.png$$y00104 The NLO QCD cross section for $\MH=120\UGeV$ after all cuts as a function of $\pT{}_{\rm ,veto}$ (left) and the efficiency of the forward jet tagging and central-jet-veto cuts as a function of $\pT{}_{\rm ,veto}$ (right). Results obtained with \VBFNLO.
001416519 8564_ $$82204078$$s45144$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_Correlation_mH400.png$$y00136 Scatter plots of the signal four-lepton acceptance as a function of the total cross section for signal events with $\MH=120 \UGeV$ (left) and $\MH=400 \UGeV$ (right), for different PDF sets. The three PDF sets are shown in different colours/symbols.
001416519 8564_ $$82204079$$s32204$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_ggHAcceptancePtElec140.png$$y00016 Generated $\pT^{\Pe}$ and $\pT^{\PGt}$ distributions for $\MH = 140 \UGeV$ (left) and $\MH = 400 \UGeV$ (right) for the $\Pg\Pg \to \PH$ process generated with {\sc PYTHIA} (dashed) and after re-weighting (solid) to correct for $\Pg\Pg \to \PH$ production dominated by the $\Pb$-loop contribution.
001416519 8564_ $$82204080$$s23953$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_GG_KfactorApplied_HNNLO_POWHEG_H120_ygg.png$$y00082 Differential cross sections of the $\Pg\Pg\rightarrow \PH\rightarrow \PGg\PGg$ process for $\MH=120\UGeV$: Higgs-boson transverse momentum (top left), Higgs-boson rapidity (top right), and $\cos\theta^{*}$ (bottom) for HNNLO, {\sc POWHEG}, and {\sc POWHEG} reweighted with $K(\qTH,\YH)$.
001416519 8564_ $$82204081$$s31410$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_ggHAcceptancePtH400.png$$y00015 Generated $\pT^{\PH}$ distributions for $\MH = 140 \UGeV$ (left) and $\MH = 400 \UGeV$ (right) for the $\Pg\Pg \to \PH$ process generated with {\sc PYTHIA} (dashed) and after re-weighting (solid) to correct for $\Pg\Pg \to \PH$ production dominated by the $\Pb$-loop contribution.
001416519 8564_ $$82204082$$s24246$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_generatorComparison_yH_mh120.png$$y00148 Differential distributions (in arbitrary units) at $7\UTeV$ for Higgs-boson masses $200\UGeV$ (left) and $500\UGeV$ (right) for three different Monte Carlo generators: \POWHEG{} (black), {\sc HNNLO} (red), \POWHEG{} reweighted with {\sc HqT} and {\sc HNNLO} (blue).
001416519 8564_ $$82204083$$s43958$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_YRHXS2_chiggs_fig1a.png$$y00032 The decay width $\Gamma(\PQt \to \PQb \PSHpm)$ calculated with {\sc FeynHiggs} and {\sc HDECAY} as a function of $\tan\beta$ for different values of $\mu$ and $\MHpm$.
001416519 8564_ $$82204084$$s54259$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_YRHXS2_chiggs_fig1b.png$$y00033 The decay width $\Gamma(\PQt \to \PQb \PSHpm)$ calculated with {\sc FeynHiggs} and {\sc HDECAY} as a function of $\tan\beta$ for different values of $\mu$ and $\MHpm$.
001416519 8564_ $$82204085$$s23022$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_tanb10-ma-200-mu-plus-ratio-shapes.png$$y00015 \small Left: ratio of the transverse-momentum distribution of the lightest scalar $\Ph$ in the MSSM over the transverse-momentum distribution of a SM Higgs boson with the same mass. Right: ratio of the corresponding shapes.
001416519 8564_ $$82204086$$s60851$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_MSSMvsONLYQUARKS_mu+.png$$y00012 \small Ratio of the full cross section for $\Ph$ production in the MSSM over the approximated cross section computed with only quarks running in the loops. The plot on the left is for $\mu>0$ while the plot on the right is for $\mu&lt;0$.
001416519 8564_ $$82204087$$s71985$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_MSSMvsONLYQUARKS_mu-.png$$y00013 \small Ratio of the full cross section for $\Ph$ production in the MSSM over the approximated cross section computed with only quarks running in the loops. The plot on the left is for $\mu>0$ while the plot on the right is for $\mu&lt;0$.
001416519 8564_ $$82204088$$s22864$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_GG_KfactorApplied_HNNLO_POWHEG_H120_costhetastar.png$$y00083 Differential cross sections of the $\Pg\Pg\rightarrow \PH\rightarrow \PGg\PGg$ process for $\MH=120\UGeV$: Higgs-boson transverse momentum (top left), Higgs-boson rapidity (top right), and $\cos\theta^{*}$ (bottom) for HNNLO, {\sc POWHEG}, and {\sc POWHEG} reweighted with $K(\qTH,\YH)$.
001416519 8564_ $$82204089$$s30297$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_VBF_YRHXS2_VBF_PWG_pveto.png$$y00103 Relative transverse momentum $\pT^{{\rm rel},j_1}$ of all the particles clustered inside the first tagging jet, in the reference frame where the jet has zero rapidity, defined according to \Eref{eq:VBF_def_ptrel} (left) and probability of finding a veto jet defined as in \Eref{eq:VBF_P_veto} as a function of $\pT{}_{\rm ,veto}$ (right). We show the comparison among NLO QCD and the \POWHEG{} interfaced to \HERWIG{} and \PYTHIA{} results. In addition, on the right plot, we show the NLO QCD results obtained with $\muR=\muF=\MW/2$ and $\muR=\muF=2\MW$.
001416519 8564_ $$82204090$$s36174$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_GG_SergueiMingHqt_Powheg_ratio_enFonctiondePTHm120.png$$y00076 (Left) Distribution of relative {\sc HqT}/\POWHEG{} event weights as a function of Higgs-boson $\pT$ for $\MH=120\UGeV$ with fit superposed. (Right) Fitted event weight functions for $\MH=110,120,130,140\UGeV$ as a function of Higgs-boson $\pT$.
001416519 8564_ $$82204091$$s22427$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_VBF_YRHXS2_VBF_PWG_absdelyjj.png$$y00099 Invariant mass of the two tagging jets, $m_{jj}$, (left) and absolute value of the distance in rapidity of the two tagging jets, $\abs{y_{j_1}-y_{j_2}}$, (right). We show the comparison among NLO QCD and the \POWHEG{} interfaced to \HERWIG{} and \PYTHIA{} results.
001416519 8564_ $$82204092$$s14160$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_mbb_pp.png$$y00199 Distribution of the invariant mass $m_{\PQb\PAQb}$ of the bottom-anti-bottom pair (a), distribution in the transverse momentum $p_{\mathrm{T}_{\PQb\PAQb}}$ of the bottom-anti-bottom pair (b), distribution in the rapidity $y_{\PQb\PAQb}$ of the bottom--anti-bottom pair (c), and distribution in the transverse momentum $p_{\mathrm{T},\PQb}$ of the bottom quark (d) for $\Pp\Pp\rightarrow \PQt\PAQt\PH \rightarrow \PQt\PAQt\PQb\PAQb +X$ and $\Pp\Pp\rightarrow \PQt\PAQt\PQb\PAQb+X$ at the LHC for the CM energy of $14\UTeV$. The red solid line refers to the NLO QCD background, the blue dotted line to the LO QCD background, while the green dash-dotted and cyan dashed line to the NLO and LO signal, respectively. From \Bref{Binoth:2010ra}.
001416519 8564_ $$82204093$$s6602$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_yh_plot_boosted3_7T_rel_W_YR.png$$y00120 Relative EW corrections for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for boosted Higgs bosons at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82204094$$s37357$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_VBF_YRHXS2_VBF_COMP_yh.png$$y00092 Higgs-boson rapidity (left) and transverse momentum (right). The top plots show the comparison between \HAWK{} (with and without EW corrections), \POWHEG{} at NLO QCD and \VBFNLO{} (with EW corrections) for $\MH = 120$\UGeV{} (upper set of curves) and $\MH = 600$\UGeV{} (lower set of curves) for MSTW2008NLO PDF set. The bottom plots display the percentage EW corrections, for each of the two mass points.
001416519 8564_ $$82204095$$s6780$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_ptV_plot_incl3_7T_rel_Z_YR.png$$y00125 Relative EW corrections for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for the basic cuts at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82204096$$s20866$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_sm4_YRHXS2_HLS_lf.png$$y00068 The resonant part of the process $i j \to \PH + k$ where $i,j$ and $k$ are partons ($\Pg$ or $\PQq$). We distinguish between production, propagation and decay, indicating the explicit dependence on Mandelstam invariants. If $s$ denotes the $\Pp\Pp$ invariant mass we distinguish between $v s$, the $i j$ invariant mass, $z s$, the Higgs-boson virtuality and ${\hat t}$ which is related to the Higgs-boson transverse momentum. Within NR we include the non-resonant contributions as well as their interference with the signal. NR includes those terms that are of higher order in the Laurent expansion of the signal around the complex pole. At NNLO QCD the parton $k$ is a pair $k_1{-}k_2$, and more invariants are needed to characterise the production mechanism.
001416519 8564_ $$82204097$$s31642$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_ggHAcceptancePtTau400.png$$y00019 Generated $\pT^{\Pe}$ and $\pT^{\PGt}$ distributions for $\MH = 140 \UGeV$ (left) and $\MH = 400 \UGeV$ (right) for the $\Pg\Pg \to \PH$ process generated with {\sc PYTHIA} (dashed) and after re-weighting (solid) to correct for $\Pg\Pg \to \PH$ production dominated by the $\Pb$-loop contribution.
001416519 8564_ $$82204098$$s37185$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_ZZ_fig1.png$$y00154 (Left) The cross sections for $\ZZ^{(*)}$ production as a function of ${\mathswitch {m_{2\Pe 2\PGm}}}$ at $7\UTeV$ from {\sc MCFM} at NLO; (right) cross sections for $\ZZ^{(*)}$ production as a function of ${\mathswitch {m_{2\Pe 2\PGm}}}$ at $7\UTeV$ from {\sc MCFM} at NLO for three different sets of cuts as described in the text.
001416519 8564_ $$82204099$$s27598$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_sm4_8TeV_800_NS.png$$y00067 The invariant-mass distribution in the OFFP-scheme with running QCD scales for $800\UGeV$ in the window $M_{\peak} \pm 2\,\GOS$. The blue line refers to $8\UTeV$, the red one to $7\UTeV$.
001416519 8564_ $$82204100$$s19812$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_sm4_DeltaGluGlu-NotCompletelyDegenerate-zoom.png$$y00059 Relative corrections in SM4 ($\PQtpr{-}\PQbpr$ and $\Pl'{-}\PGnl'$ doublets) due to 2-loop EW corrections to $\Pg \Pg \to \PH$.   The masses of the 4th-generation fermions are chosen according to \Eref{eq:masses}. In the inset a blow-up of the small-$\MH$ region is shown.
001416519 8564_ $$82204101$$s47136$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_CUT3_MCFM_POWHEG_LHC.png$$y00158 $ZZ\rightarrow 2\Pe 2\PGm$ invariant-mass distributions at $7 \UTeV$ with \POWHEG{} and {\sc MCFM v6.1}. Two different PDF sets are used. The top-left plot is obtained applying only ${\mathswitch {m_{2l}}}>12 \UGeV$; the top-right plot asking $\mzonshell >50 \UGeV$, $\mzoffshell>12 \UGeV$, $\pT(\Pl)>5 \UGeV$, $|\eta(\Pl)|&lt;2.5$, and the bottom plot asking $60 &lt;\mzonshell&lt;120 \UGeV$ and $60 &lt;\mzoffshell&lt;120 \UGeV$.
001416519 8564_ $$82204102$$s55867$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_YRHXS2_chiggs_fig4d.png$$y00045 The decay width of $\PSHpm$ calculated with {\sc FeynHiggs} and {\sc HDECAY} as a function of $\tan\beta$ for different values of $\mu$ and $\MHpm$.
001416519 8564_ $$82204103$$s55586$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_YRHXS2_chiggs_fig4c.png$$y00044 The decay width of $\PSHpm$ calculated with {\sc FeynHiggs} and {\sc HDECAY} as a function of $\tan\beta$ for different values of $\mu$ and $\MHpm$.
001416519 8564_ $$82204104$$s54454$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_YRHXS2_chiggs_fig4b.png$$y00043 The decay width of $\PSHpm$ calculated with {\sc FeynHiggs} and {\sc HDECAY} as a function of $\tan\beta$ for different values of $\mu$ and $\MHpm$.
001416519 8564_ $$82204105$$s37267$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_fig_Et_lp1_cut3.png$$y00190 Invariant mass of all jet pairs passing the cuts of set 3) (\textit{left}) and transverse energy of the hardest positively-charged lepton (\textit{right}). The different regions of the plots are defined as in Fig.~\protect\ref{fig:ttH_nlomc_fig1}. See text for more details.
001416519 8564_ $$82204106$$s30910$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_totalxs_7TeV_santander_gnu.png$$y00054 \sloppy (a) Central values for the total inclusive cross section in the 5FS (red, dashed), the 4FS (green, dashed), and for the matched cross section (blue, solid). Here and in the following we use the MSTW2008\, PDF set~\cite{Martin:2009iq}. (b) Theory uncertainty bands for the total inclusive cross section in the 5FS (red, dashed), the 4FS (green, dashed), and for the matched cross section (blue, solid).
001416519 8564_ $$82204107$$s20948$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_tanb24-ma125-mu-minus-MSSMvsSM.png$$y00012 \small Left plots: ratio of the transverse momentum-distribution for the lightest scalar $\Ph$ in the MSSM over the distribution for a SM Higgs with the same mass. Right plots: ratio of the transverse-momentum distribution for $\Ph$ in the MSSM over the approximate distribution computed with only quarks running in the loops. The plots are obtained with $\mu&lt;0$, and with three different choices of $\MA$ and $\tan\beta$ for which the MSSM and SM predictions for the total cross section agree within $5\%$.
001416519 8564_ $$82204108$$s19382$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_mZZ_PYTHIA_POWHEG.png$$y00162 $\ZZ\rightarrow 4\mu$ invariant-mass distributions at $7\UTeV$ as derived by {\sc PYTHIA} and \POWHEG
001416519 8564_ $$82204109$$s36334$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_CUT3_CT10vsMSTW_LHC.png$$y00161 $\ZZ\rightarrow 2\Pe 2\PGm$ and $\ZZ\rightarrow 4\Pe$ invariant-mass distributions and their ratio at $7\UTeV$ with \POWHEG{}. Two different PDF sets are used. The upper plots are obtained applying only ${\mathswitch {m_{2\Pl}}}>12 \UGeV$, the middle plots applying $\mzonshell>50 \UGeV$, $\mzoffshell>12 \UGeV$, $\pT(\Pl)>5 \UGeV$, $|\eta(\Pl)|&lt;2.5$, and the bottom plots applying $60 &lt;\mzonshell&lt;120 \UGeV$ and $60 &lt;\mzoffshell&lt;120 \UGeV$.
001416519 8564_ $$82204110$$s16368$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_pTb_pp.png$$y00202 Distribution of the invariant mass $m_{\PQb\PAQb}$ of the bottom-anti-bottom pair (a), distribution in the transverse momentum $p_{\mathrm{T}_{\PQb\PAQb}}$ of the bottom-anti-bottom pair (b), distribution in the rapidity $y_{\PQb\PAQb}$ of the bottom--anti-bottom pair (c), and distribution in the transverse momentum $p_{\mathrm{T},\PQb}$ of the bottom quark (d) for $\Pp\Pp\rightarrow \PQt\PAQt\PH \rightarrow \PQt\PAQt\PQb\PAQb +X$ and $\Pp\Pp\rightarrow \PQt\PAQt\PQb\PAQb+X$ at the LHC for the CM energy of $14\UTeV$. The red solid line refers to the NLO QCD background, the blue dotted line to the LO QCD background, while the green dash-dotted and cyan dashed line to the NLO and LO signal, respectively. From \Bref{Binoth:2010ra}.
001416519 8564_ $$82204111$$s41518$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_VBF_YRHXS2_VBF_COMP_ptjmax1pt.png$$y00094 Transverse momentum of the leading (left) and sub-leading jet (right). The top plots show the comparison between \HAWK{} (with and without EW corrections), \POWHEG{} at NLO QCD and \VBFNLO{} (with EW corrections) for $\MH = 120$\UGeV{} (upper set of curves) and $\MH = 600$\UGeV{} (lower set of curves) for MSTW2008NLO PDF set. The bottom plots display the percentage EW corrections, for each of the two mass points.
001416519 8564_ $$82204112$$s74804$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_BR_YRHXS2_BR_Fig1.png$$y00069 Higgs branching ratios and their uncertainties for the low mass range (left) and for the full mass range (right).
001416519 8564_ $$82204113$$s68798$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_sigmatt_BRtHpb_03B.png$$y00041 Caption not extracted
001416519 8564_ $$82204114$$s10996$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_weight.png$$y00006 \sloppy (a) Weight factor $w$, \eqn{eq::tn}, as a function of the Higgs-boson mass $\MH$. The bottom-quark pole mass has been set to $\Mb = 4.75 \UGeV$. (b) Central values for the total inclusive cross section in the 4FS (red, dashed), the 5FS (green, dotted), and for the Santander-matched cross section (blue, solid). Here and in the following we use the MSTW2008\, PDF set~\cite{Martin:2009iq} (NLO for the 4FS, NNLO for the 5FS).
001416519 8564_ $$82204115$$s94074$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_old-minus-mu-MSSMvsSM.png$$y00010 \small Ratio of the total cross section for $\Ph$ production in the MSSM over the cross section for the production of a SM Higgs boson with the same mass. The plot on the left is for $\mu>0$ while the plot on the right is for $\mu&lt;0$.
001416519 8564_ $$82204116$$s31574$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_ggHAcceptancePtH140.png$$y00014 Generated $\pT^{\PH}$ distributions for $\MH = 140 \UGeV$ (left) and $\MH = 400 \UGeV$ (right) for the $\Pg\Pg \to \PH$ process generated with {\sc PYTHIA} (dashed) and after re-weighting (solid) to correct for $\Pg\Pg \to \PH$ production dominated by the $\Pb$-loop contribution.
001416519 8564_ $$82204117$$s37961$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_fig_mjj_cut3_ps.png$$y00194 Separation in pseudo-rapidity and azimuthal angle of the two hardest lowest-lying B hadrons in the events (no-cut analysis) (\textit{left}) and invariant mass of all jet pairs passing the set 3) of cuts (\textit{right}). The different regions of the plots are defined as in Fig.~\protect\ref{fig:ttH_nlomc_fig1}. See text for more details.
001416519 8564_ $$82204118$$s48936$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_YRHXS2_chiggs_fig1c.png$$y00034 The decay width $\Gamma(\PQt \to \PQb \PSHpm)$ calculated with {\sc FeynHiggs} and {\sc HDECAY} as a function of $\tan\beta$ for different values of $\mu$ and $\MHpm$.
001416519 8564_ $$82204119$$s24273$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_GG_Ming_Serguei_comparison_dPhi_gg.png$$y00078 Distributions of kinematical observables potentially important for the $\PH\rightarrow \PGg\PGg$ search, for $\MH=120\UGeV$, after application of 'CMS' acceptance criteria, before (red histogram) and after (blue dots) reweighting of the Higgs-boson $\pT$ spectrum to that of {\sc HqT}. Top left: $\Delta\phi^{\PGg\PGg}$; top right: $\eta^{\PGg\PGg}$; bottom: $\cos\theta^*$.
001416519 8564_ $$82204120$$s25450$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_GenMHiggs_Powheg_v_Pythia_150GeV_VBF_cut2.png$$y00133 Higgs-boson transverse momentum and mass spectrum derived with \PYTHIA~(LO) and \POWHEG\ (NLO) generators for the four-lepton final state from the decay of the Higgs boson with mass $\MH=150 \UGeV$, asking $\mzonshell >50 \UGeV$, $\mzoffshell >12 \UGeV$ and $\pT>5 \UGeV$, $|\eta|&lt;2.5$. Plots are normalised to the same area.
001416519 8564_ $$82204121$$s13530$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_yb140.png$$y00028 The rapidity distributions of the leading $\pT$ b-jet normalised on unity for $\MH=140\UGeV$ (left) and $\MH=400\UGeV$ (right) obtained with {\sc PYTHIA} (solid lines) and with NLO calculations (dashed lines).
001416519 8564_ $$82204122$$s23671$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_ptb_lo_nlo_ps_gnu.png$$y00058 \sloppy Transverse-momentum distributions of the bottom quark in the 4FS for $\Pp\Pp \to {\rm t}\PAQb{\rm H}^-+X$ at the LHC ($14\UTeV$). Shown are results at LO and NLO.
001416519 8564_ $$82204123$$s27597$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_GG_Lorenzodelta_vs_thetaStar.png$$y00085 Absolute value of the destructive interference factor $\delta$ (left) and its value as a function of $\theta^*$, for $\MH=120\UGeV$ using the 'ATLAS' acceptance criteria.
001416519 8564_ $$82204124$$s48659$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_VBF_YRHXS2_VBF_VBFNLO_effvspt.png$$y00105 The NLO QCD cross section for $\MH=120\UGeV$ after all cuts as a function of $\pT{}_{\rm ,veto}$ (left) and the efficiency of the forward jet tagging and central-jet-veto cuts as a function of $\pT{}_{\rm ,veto}$ (right). Results obtained with \VBFNLO.
001416519 8564_ $$82204125$$s38464$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_generatorComparison_mZ1_mh500.png$$y00145 Differential distributions (in arbitrary units) at $7\UTeV$ for Higgs-boson masses $200\UGeV$ (left) and $500 \UGeV$ (right) for three different Monte Carlo generators: \POWHEG{} (black), {\sc HNNLO} (red), \POWHEG{} reweighted with {\sc HqT} and {\sc HNNLO} (blue).
001416519 8564_ $$82204126$$s5964$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_yh_plot_PDF4LHC_7T_abs_Z_YR.png$$y00113 Predictions for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for boosted Higgs bosons at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82204127$$s29933$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_dsdeta_H_err_band.png$$y00177 Theoretical uncertainty on Higgs-boson pseudorapidity ($\eta^{\PH}$) distribution: the l.h.s.\ shows the actual distributions, the r.h.s.\ the spread around the central value in per cent. A detailed explanation of the red and blue bands is given in the text.
001416519 8564_ $$82204128$$s46371$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_YR2HXS_figXXa_nomix.png$$y00004 Caption not extracted
001416519 8564_ $$82204129$$s40971$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_fig_pthtt.png$$y00185 Transverse momentum of the Higgs--top--antitop system (\textit{left}) and invariant mass of the two hardest lowest-lying B hadrons (\textit{right}). The different regions of the plots are defined as in \protect\refF{fig:ttH_nlomc_fig1}. See text for more details.
001416519 8564_ $$82204130$$s11968$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_tTbB_mbb100_ptb-soft_abs.png$$y00196 Transverse momentum of the harder ($p_{\mathrm{T},\PQb_1}$) and softer ($p_{\mathrm{T},\PQb_2}$) $b$ jets at $14\UTeV$ CM energy: absolute LO and NLO prediction for the unboosted ($m_{\PQb\PAQb}>100\UGeV$, upper plots) and boosted regimes ($p_{T,\PQb\PAQb}>200\UGeV$, lower plots). The uncertainty bands correspond to a factor two scale variation. From \Bref{Bredenstein:2010rs}.
001416519 8564_ $$82204131$$s11306$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_GG_Lorenzodist_Rinterf_m120_logx.png$$y00084 Absolute value of the destructive interference factor $\delta$ (left) and its value as a function of $\theta^*$, for $\MH=120\UGeV$ using the 'ATLAS' acceptance criteria.
001416519 8564_ $$82204132$$s8649$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_pth_plot_incl3_7T_rel_W_YR.png$$y00122 Relative EW corrections for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for the basic cuts at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82204133$$s14064$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_ybb_pp.png$$y00201 Distribution of the invariant mass $m_{\PQb\PAQb}$ of the bottom-anti-bottom pair (a), distribution in the transverse momentum $p_{\mathrm{T}_{\PQb\PAQb}}$ of the bottom-anti-bottom pair (b), distribution in the rapidity $y_{\PQb\PAQb}$ of the bottom--anti-bottom pair (c), and distribution in the transverse momentum $p_{\mathrm{T},\PQb}$ of the bottom quark (d) for $\Pp\Pp\rightarrow \PQt\PAQt\PH \rightarrow \PQt\PAQt\PQb\PAQb +X$ and $\Pp\Pp\rightarrow \PQt\PAQt\PQb\PAQb+X$ at the LHC for the CM energy of $14\UTeV$. The red solid line refers to the NLO QCD background, the blue dotted line to the LO QCD background, while the green dash-dotted and cyan dashed line to the NLO and LO signal, respectively. From \Bref{Binoth:2010ra}.
001416519 8564_ $$82204134$$s20639$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_tanb10-ma-200-mu-plus-ratio.png$$y00014 \small Left: ratio of the transverse-momentum distribution of the lightest scalar $\Ph$ in the MSSM over the transverse-momentum distribution of a SM Higgs boson with the same mass. Right: ratio of the corresponding shapes.
001416519 8564_ $$82204135$$s45871$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_YRHXS2_chiggs_fig6a.png$$y00050 The decay width $\Gamma(\PH^{\pm} \to \PQc\PQs)$ calculated with {\sc FeynHiggs} and {\sc HDECAY} as a function of $\tan\beta$ for different values of $\mu$ and $M_{\PH^{\pm}}$. A discrepancy of $7{-}19\%$ is observed.
001416519 8564_ $$82204136$$s51885$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_YR2HXS_figXXb_nomix.png$$y00005 Central predictions for the total MSSM production cross sections via gluon fusion and Higgs radiation off bottom quarks within the 5FS for $\sqrt{s}=7$\UTeV\ using NNLO and NLO MSTW2008 PDFs \cite{Martin:2009iq,Martin:2009bu} for the no-mixing scenario; (a) $\tanb=5$, (b) $\tanb=30$.Caption not extracted
001416519 8564_ $$82204137$$s44540$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_uncertaintyband.png$$y00008 \sloppy (a) Theory uncertainty bands for the total inclusive cross section in the 4FS (red, dashed), the 5FS (green, dotted), and for the Santander-matched cross section (blue, solid). (b) Uncertainty bands and central values, relative to the central value of the Santander-matched result (same line coding as panel (a)).
001416519 8564_ $$82204138$$s30371$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_Acceptance_w_now_powheg_4l.png$$y00139 Ratio between the acceptance values for \POWHEG{} events with four electrons, four muons, and two electrons and two muons final state from $\PH\rightarrow \ZZ$ decay, when turning on/off the reweighting with {\sc HqT}.
001416519 8564_ $$82204139$$s21478$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_generatorComparison_yH_mh500.png$$y00149 Differential distributions (in arbitrary units) at $7\UTeV$ for Higgs-boson masses $200\UGeV$ (left) and $500\UGeV$ (right) for three different Monte Carlo generators: \POWHEG{} (black), {\sc HNNLO} (red), \POWHEG{} reweighted with {\sc HqT} and {\sc HNNLO} (blue).
001416519 8564_ $$82204140$$s46039$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_GG_SergueiMingHqt_powheg_weight_functionsFourMasses.png$$y00077 (Left) Distribution of relative {\sc HqT}/\POWHEG{} event weights as a function of Higgs-boson $\pT$ for $\MH=120\UGeV$ with fit superposed. (Right) Fitted event weight functions for $\MH=110,120,130,140\UGeV$ as a function of Higgs-boson $\pT$.
001416519 8564_ $$82204141$$s18291$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_VBF_YRHXS2_VBF_PWG_jetmult.png$$y00101 Rapidity distribution of the third hardest jet, $y_{j_3}$ (left) and exclusive jet-multiplicity (right).  We show the comparison among NLO QCD and the \POWHEG{} interfaced to \HERWIG{} and \PYTHIA{} results.
001416519 8564_ $$82204142$$s41822$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_CrossSection_qcd.png$$y00166 The cross section for $\PQq\PAQq \rightarrow \ZZ^{(*)}\rightarrow {2\Pe 2\PGm}$ (left) and for $\Pg\Pg \rightarrow \ZZ^{(*)}\rightarrow {2\Pe 2\PGm}$ (right) as a function of ${\mathswitch {m_{2\Pe 2\PGm}}}$ at $7\UTeV$ from {\sc MCFM} computed with the CT10 PDF and varying the QCD scale by a factor of two.
001416519 8564_ $$82204143$$s39461$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_VBF_YRHXS2_VBF_COMP_ptjmax2pt.png$$y00095 Transverse momentum of the leading (left) and sub-leading jet (right). The top plots show the comparison between \HAWK{} (with and without EW corrections), \POWHEG{} at NLO QCD and \VBFNLO{} (with EW corrections) for $\MH = 120$\UGeV{} (upper set of curves) and $\MH = 600$\UGeV{} (lower set of curves) for MSTW2008NLO PDF set. The bottom plots display the percentage EW corrections, for each of the two mass points.
001416519 8564_ $$82204144$$s50372$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_YRHXS2_chiggs_fig2d.png$$y00039 Caption not extracted
001416519 8564_ $$82204145$$s9312$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_ptV_plot_incl3_7T_rel_W_YR.png$$y00124 Relative EW corrections for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for the basic cuts at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82204146$$s48580$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_YRHXS2_chiggs_fig2a.png$$y00036 The branching fraction BR$(\PQt \to \PQb \PSHpm)$ calculated with {\sc FeynHiggs} and {\sc HDECAY} as a function of $\tan\beta$ for different values of $\mu$ and $\MHpm$.Caption not extracted
001416519 8564_ $$82204147$$s52218$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_YRHXS2_chiggs_fig2c.png$$y00038 Caption not extracted
001416519 8564_ $$82204148$$s56823$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_YRHXS2_chiggs_fig2b.png$$y00037 Caption not extracted
001416519 8564_ $$82204149$$s45472$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_YRHXS2_chiggs_fig1d.png$$y00035 The decay width $\Gamma(\PQt \to \PQb \PSHpm)$ calculated with {\sc FeynHiggs} and {\sc HDECAY} as a function of $\tan\beta$ for different values of $\mu$ and $\MHpm$.
001416519 8564_ $$82204150$$s22735$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_GenHiggsPt_Powheg_v_Pythia_150GeV_gg_cut2.png$$y00130 Higgs-boson transverse momentum and mass spectrum derived with \PYTHIA~(LO) and \POWHEG\ (NLO) generators for the four-lepton final state from the decay of the Higgs boson with mass $\MH=150 \UGeV$, asking $\mzonshell >50 \UGeV$, $\mzoffshell >12 \UGeV$ and $\pT>5 \UGeV$, $|\eta|&lt;2.5$. Plots are normalised to the same area.
001416519 8564_ $$82204151$$s22076$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_dsdpt_t_perc_err_band.png$$y00172 Theoretical uncertainty on top(antitop)-quark transverse-momentum ($\pT^{\PQt}$) distribution: the l.h.s.\ shows the actual distributions, the r.h.s.\ the spread around the central value in per cent. A detailed explanation of the red and blue bands is given in the text.
001416519 8564_ $$82204152$$s22449$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_VBF_YRHXS2_VBF_PWG_mjj.png$$y00098 Invariant mass of the two tagging jets, $m_{jj}$, (left) and absolute value of the distance in rapidity of the two tagging jets, $\abs{y_{j_1}-y_{j_2}}$, (right). We show the comparison among NLO QCD and the \POWHEG{} interfaced to \HERWIG{} and \PYTHIA{} results.
001416519 8564_ $$82204153$$s32615$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_dsdR_tH_err_band.png$$y00181 Theoretical uncertainty on top-Higgs $(\eta,\phi)$ distance ($R(\PQt,\PH)$) distribution in the no-cut configuration: the l.h.s.\ shows the actual distributions, the r.h.s.\ the spread around the central value in per cent. A detailed explanation of the red and blue bands is given in the text.
001416519 8564_ $$82204154$$s6398$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_yh_plot_incl3_7T_rel_W_YR.png$$y00128 Relative EW corrections for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for the basic cuts at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82204155$$s99647$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_ZZ_M4l_MCFM.png$$y00152 (left) The cross sections for $\PQq\PAQq\rightarrow \ZZ^{(*)}\rightarrow{2\Pe 2\PGm}$ as a function of ${\mathswitch {m_{2\Pe 2\PGm}}}$ at $7\UTeV$ from {\sc MCFM} for the full calculation and without the singly-resonant contribution; (right) LO cross sections for $\PQq\PAQq\rightarrow \ZZ^{(*)}\rightarrow {2\Pe 2\PGm}$ as a function of ${\mathswitch {m_{2\Pe 2\PGm}}}$ at $7\UTeV$ from {\sc MCFM} at LO.
001416519 8564_ $$82204156$$s31010$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_fig_rates.png$$y00183 Total rates for scalar-Higgs-boson production after the different cuts defined in the text (\textit{left}) and transverse momentum of the Higgs boson (\textit{right}) in the no-cut configuration. In the upper inset the scale and PDF uncertainties computed by a\MCNLO{} interfaced to \HERWIG{} are shown. The lower inset displays the ratio of \powheghelac{} over a\MCNLO{} and the ratio between the results computed by interfacing \powheghelac{} to \PYTHIA{} and \HERWIG{}. See text for more details.
001416519 8564_ $$82204157$$s51755$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_CUT2_MCFM_POWHEG_LHC.png$$y00157 $ZZ\rightarrow 2\Pe 2\PGm$ invariant-mass distributions at $7 \UTeV$ with \POWHEG{} and {\sc MCFM v6.1}. Two different PDF sets are used. The top-left plot is obtained applying only ${\mathswitch {m_{2l}}}>12 \UGeV$; the top-right plot asking $\mzonshell >50 \UGeV$, $\mzoffshell>12 \UGeV$, $\pT(\Pl)>5 \UGeV$, $|\eta(\Pl)|&lt;2.5$, and the bottom plot asking $60 &lt;\mzonshell&lt;120 \UGeV$ and $60 &lt;\mzoffshell&lt;120 \UGeV$.
001416519 8564_ $$82204158$$s22851$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_GG_KfactorApplied_PromptPromptNLO_qt.png$$y00089 Differential cross sections for diphoton production from the sum of the quark--antiquark annihilation, gluon-fusion, and gluon--(anti)quark scattering processes: Diphoton transverse momentum (top left), diphoton invariant mass (top right), and $\cos\theta^{*}$ (bottom) for a combination of {\sc Diphox} and {\sc Gamma2MC}, a combination of {\sc Madgraph} and {\sc PYTHIA}, and the latter combination reweighted with $K(M_{\PGg\PGg},\qTH)$.
001416519 8564_ $$82204159$$s10208$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_ptlpm_plot_incl3_7T_rel_W_YR.png$$y00126 Relative EW corrections for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for the basic cuts at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82204160$$s23488$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_GG_KfactorApplied_PromptPromptNLO_costhetastar.png$$y00091 Differential cross sections for diphoton production from the sum of the quark--antiquark annihilation, gluon-fusion, and gluon--(anti)quark scattering processes: Diphoton transverse momentum (top left), diphoton invariant mass (top right), and $\cos\theta^{*}$ (bottom) for a combination of {\sc Diphox} and {\sc Gamma2MC}, a combination of {\sc Madgraph} and {\sc PYTHIA}, and the latter combination reweighted with $K(M_{\PGg\PGg},\qTH)$.
001416519 8564_ $$82204161$$s28972$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_generatorComparison_ptH_mh500.png$$y00141 Differential distributions (in arbitrary units) at $7\UTeV$ for Higgs-boson masses $200\UGeV$ (left) and $500 \UGeV$ (right) for three different Monte Carlo generators: \POWHEG{} (black), {\sc HNNLO} (red), \POWHEG{} reweighted with {\sc HqT} and {\sc HNNLO} (blue).
001416519 8564_ $$82204162$$s30904$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_dsdeta_t_err_band.png$$y00173 Theoretical uncertainty on top(antitop)-quark pseudorapidity ($\eta^{\PQt}$) distribution: the l.h.s.\ shows the actual distributions, the r.h.s.\ the spread around the central value in per cent. A detailed explanation of the red and blue bands is given in the text.
001416519 8564_ $$82204163$$s46924$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_YRHXS2_chiggs_fig6d.png$$y00053 The decay width $\Gamma(\PH^{\pm} \to \PQc\PQs)$ calculated with {\sc FeynHiggs} and {\sc HDECAY} as a function of $\tan\beta$ for different values of $\mu$ and $M_{\PH^{\pm}}$. A discrepancy of $7{-}19\%$ is observed.
001416519 8564_ $$82204164$$s12780$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_pTb140.png$$y00030 The $\pT$ distributions of the leading $\pT$ b-jet normalised on unity for $\MH=140\UGeV$ (left) and $\MH=400\UGeV$ (right) obtained with {\sc PYTHIA} (solid lines) and with NLO calculations (dashed lines).
001416519 8564_ $$82204165$$s25324$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_ptt_45FS_gnu.png$$y00057 \sloppy Normalised transverse-momentum distributions of the Higgs boson (a) and the top quark (b) for $\Pp\Pp \to {\rm t}\PAQb{\rm H}^-+X$ at the LHC ($14\UTeV$). Shown are results in the 4FS (NLO) and 5FS (NLO plus parton shower).
001416519 8564_ $$82204166$$s42640$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_ma500_tb3_mstw_dpTj1.png$$y00022 None
001416519 8564_ $$82204167$$s7210$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_ptlpm_plot_boosted3_7T_abs_W_YR.png$$y00110 Predictions for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for boosted Higgs bosons at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82204168$$s39827$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_ma100_tb50_mstw_dpTj1.png$$y00023 Transverse momentum of the leading jet for $\tan \beta = 3$, $\MA = 500 \UGeV$ (left plot) and $\tan \beta = 50$, $\MA = 100 \UGeV$ (right plot), comparing the MSSM results with the rescaled SM values with the MSTW2008NLO PDF set.Caption not extracted
001416519 8564_ $$82204169$$s24342$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_GG_MingSerguei_comparison_eta_gg.png$$y00079 Distributions of kinematical observables potentially important for the $\PH\rightarrow \PGg\PGg$ search, for $\MH=120\UGeV$, after application of 'CMS' acceptance criteria, before (red histogram) and after (blue dots) reweighting of the Higgs-boson $\pT$ spectrum to that of {\sc HqT}. Top left: $\Delta\phi^{\PGg\PGg}$; top right: $\eta^{\PGg\PGg}$; bottom: $\cos\theta^*$.
001416519 8564_ $$82204170$$s29449$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_generatorComparison_mZ2_mh120.png$$y00146 Differential distributions (in arbitrary units) at $7\UTeV$ for Higgs-boson masses $200\UGeV$ (left) and $500 \UGeV$ (right) for three different Monte Carlo generators: \POWHEG{} (black), {\sc HNNLO} (red), \POWHEG{} reweighted with {\sc HqT} and {\sc HNNLO} (blue).
001416519 8564_ $$82204171$$s44527$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_YRHXS2_chiggs_fig5a.png$$y00046 The decay width $\Gamma(\PH^{\pm} \to \PGt\PGn_{\PGt})$ calculated with {\sc FeynHiggs} and {\sc HDECAY} as a function of $\tan\beta$ for different values of $\mu$ and $M_{\PH^{\pm}}$.
001416519 8564_ $$82204172$$s55032$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_YRHXS2_chiggs_fig5b.png$$y00047 The decay width $\Gamma(\PH^{\pm} \to \PGt\PGn_{\PGt})$ calculated with {\sc FeynHiggs} and {\sc HDECAY} as a function of $\tan\beta$ for different values of $\mu$ and $M_{\PH^{\pm}}$.
001416519 8564_ $$82204173$$s55574$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_YRHXS2_chiggs_fig5c.png$$y00048 The decay width $\Gamma(\PH^{\pm} \to \PGt\PGn_{\PGt})$ calculated with {\sc FeynHiggs} and {\sc HDECAY} as a function of $\tan\beta$ for different values of $\mu$ and $M_{\PH^{\pm}}$.
001416519 8564_ $$82204174$$s55577$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_chiggs_YRHXS2_chiggs_fig5d.png$$y00049 The decay width $\Gamma(\PH^{\pm} \to \PGt\PGn_{\PGt})$ calculated with {\sc FeynHiggs} and {\sc HDECAY} as a function of $\tan\beta$ for different values of $\mu$ and $M_{\PH^{\pm}}$.
001416519 8564_ $$82204175$$s24222$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_GG_MingSerguei_comparison_costheta.png$$y00080 Distributions of kinematical observables potentially important for the $\PH\rightarrow \PGg\PGg$ search, for $\MH=120\UGeV$, after application of 'CMS' acceptance criteria, before (red histogram) and after (blue dots) reweighting of the Higgs-boson $\pT$ spectrum to that of {\sc HqT}. Top left: $\Delta\phi^{\PGg\PGg}$; top right: $\eta^{\PGg\PGg}$; bottom: $\cos\theta^*$.
001416519 8564_ $$82204176$$s29365$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_VBF_YRHXS2_VBF_COMP_dphijjmaxpt.png$$y00097 Di-jet invariant mass (left) and azimuthal separation between the two tagging jets (right). The top plots show the comparison between \HAWK{} (with and without EW corrections), \POWHEG{} QCD and \VBFNLO{} (with EW corrections) for $\MH = 120$\UGeV{} (upper set of curves) and $\MH = 600$\UGeV{} (lower set of curves) for MSTW2008NLO PDF set. The bottom plots display the percentage EW corrections for each of the two mass points.
001416519 8564_ $$82204177$$s28406$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_QcdScale.png$$y00167 The ratio of the cross sections computed at different scales and the cross section computed at central value of the QCD scale for $\PQq\PAQq \rightarrow \ZZ^{(*)}\rightarrow {2\Pe 2\PGm}$ (left) and $\Pg\Pg \rightarrow \ZZ^{(*)}\rightarrow {2\Pe 2\PGm}$ (right) as a function of ${\mathswitch {m_{2\Pe 2\PGm}}}$ at $7\UTeV$ from {\sc MCFM}. The red line is the parametrisation described in the text
001416519 8564_ $$82204178$$s6663$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_ptlp_plot_incl3_7T_rel_Z_YR.png$$y00127 Relative EW corrections for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for the basic cuts at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82204179$$s27634$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_pdf+alphas1.png$$y00165 The difference between the central value of the cross section and the cross section computed with 3 different PDF sets and the total PDF$+\alphas$ variation (blue markers) varying them by plus and minus $1 \sigma$ for $\PQq\PAQq \rightarrow \ZZ^{(*)}\rightarrow {2\Pe 2\PGm}$ (left) and for $\Pg\Pg \rightarrow \ZZ^{(*)}\rightarrow {2\Pe 2\PGm}$ (right) as a function of ${\mathswitch {m_{2\Pe 2\PGm}}}$ at $7\UTeV$ from {\sc MCFM}.
001416519 8564_ $$82204180$$s26850$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_ma100_tb50_mstw_dphi.png$$y00021 Azimuthal-angle distributions for $\tan \beta = 3$, $\MA = 500 \UGeV$ (left plot) and $\tan \beta = 50$, $\MA = 100 \UGeV$ (right plot), comparing the MSSM results with the rescaled SM values with the MSTW2008NLO PDF set.Caption not extracted
001416519 8564_ $$82204181$$s20840$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_dsdeta_H_perc_err_band.png$$y00178 Theoretical uncertainty on Higgs-boson pseudorapidity ($\eta^{\PH}$) distribution: the l.h.s.\ shows the actual distributions, the r.h.s.\ the spread around the central value in per cent. A detailed explanation of the red and blue bands is given in the text.
001416519 8564_ $$82204182$$s30968$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ttH_dsdpt_t_err_band.png$$y00171 Theoretical uncertainty on top(antitop)-quark transverse-momentum ($\pT^{\PQt}$) distribution: the l.h.s.\ shows the actual distributions, the r.h.s.\ the spread around the central value in per cent. A detailed explanation of the red and blue bands is given in the text.
001416519 8564_ $$82204183$$s6113$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_ptlp_plot_boosted3_7T_rel_Z_YR.png$$y00119 Relative EW corrections for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for boosted Higgs bosons at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82204184$$s6043$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_ptV_plot_boosted3_7T_abs_W_YR.png$$y00108 Predictions for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for boosted Higgs bosons at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82204185$$s33694$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_Correlation_mH120.png$$y00135 Scatter plots of the signal four-lepton acceptance as a function of the total cross section for signal events with $\MH=120 \UGeV$ (left) and $\MH=400 \UGeV$ (right), for different PDF sets. The three PDF sets are shown in different colours/symbols.
001416519 8564_ $$82204186$$s44107$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_VBF_YRHXS2_VBF_COMP_pth.png$$y00093 Higgs-boson rapidity (left) and transverse momentum (right). The top plots show the comparison between \HAWK{} (with and without EW corrections), \POWHEG{} at NLO QCD and \VBFNLO{} (with EW corrections) for $\MH = 120$\UGeV{} (upper set of curves) and $\MH = 600$\UGeV{} (lower set of curves) for MSTW2008NLO PDF set. The bottom plots display the percentage EW corrections, for each of the two mass points.
001416519 8564_ $$82204187$$s39902$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_CUT2_CT10_MSTW_LHC.png$$y00160 $\ZZ\rightarrow 2\Pe 2\PGm$ and $\ZZ\rightarrow 4\Pe$ invariant-mass distributions and their ratio at $7\UTeV$ with \POWHEG{}. Two different PDF sets are used. The upper plots are obtained applying only ${\mathswitch {m_{2\Pl}}}>12 \UGeV$, the middle plots applying $\mzonshell>50 \UGeV$, $\mzoffshell>12 \UGeV$, $\pT(\Pl)>5 \UGeV$, $|\eta(\Pl)|&lt;2.5$, and the bottom plots applying $60 &lt;\mzonshell&lt;120 \UGeV$ and $60 &lt;\mzoffshell&lt;120 \UGeV$.
001416519 8564_ $$82204188$$s6172$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_ptV_plot_boosted3_7T_rel_Z_YR.png$$y00117 Relative EW corrections for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for boosted Higgs bosons at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82204189$$s7201$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_WHZH_ptV_plot_boosted3_7T_rel_W_YR.png$$y00116 Relative EW corrections for the $p_{\mathrm{T},\PH}$, $p_{\mathrm{T},\PV}$, $p_{\mathrm{T},\Pl}$, and $y_{\PH}$ distributions (top to bottom) for Higgs strahlung off \PW\ bosons (left) and \PZ\ bosons (right) for boosted Higgs bosons at the $7\UTeV$ LHC for $\MH=120\UGeV$.
001416519 8564_ $$82204190$$s24623$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_ZZ_GenHiggsPt_Powheg_v_Pythia_150GeV_VBF_cut2.png$$y00131 Higgs-boson transverse momentum and mass spectrum derived with \PYTHIA~(LO) and \POWHEG\ (NLO) generators for the four-lepton final state from the decay of the Higgs boson with mass $\MH=150 \UGeV$, asking $\mzonshell >50 \UGeV$, $\mzoffshell >12 \UGeV$ and $\pT>5 \UGeV$, $|\eta|&lt;2.5$. Plots are normalised to the same area.
001416519 8564_ $$82204191$$s30690$$uhttp://cds.cern.ch/record/1416519/files/YRHXS2_mssm_ma100_tb50_mstw_dyH.png$$y00027 Caption not extracted
001416519 8564_ $$82477203$$s34027290$$uhttp://cds.cern.ch/record/1416519/files/80dbdd3120e556ea7b2d212da120b593.pdf$$yFulltext
001416519 8564_ $$8635724$$s8272910$$uhttp://cds.cern.ch/record/1416519/files/CERN-2012-002.pdf$$yFulltext
001416519 8564_ $$8803809$$s9563$$uhttp://cds.cern.ch/record/1416519/files/fig00009.png$$y00009 \sloppy (a) Theory uncertainty bands for the total inclusive cross section in the 4FS (red, dashed), the 5FS (green, dotted), and for the Santander-matched cross section (blue, solid). (b) Uncertainty bands and central values, relative to the central value of the Santander-matched result (same line coding as panel (a)).
001416519 8564_ $$8635724$$s10270$$uhttp://cds.cern.ch/record/1416519/files/CERN-2012-002.gif?subformat=icon-700$$xicon-700$$yFulltext
001416519 8564_ $$8635724$$s3564$$uhttp://cds.cern.ch/record/1416519/files/CERN-2012-002.gif?subformat=icon$$xicon$$yFulltext
001416519 8564_ $$8635724$$s7183171$$uhttp://cds.cern.ch/record/1416519/files/CERN-2012-002.pdf?subformat=pdfa$$xpdfa$$yFulltext
001416519 916__ $$sn$$w201203$$ya2012
001416519 960__ $$a21
001416519 980__ $$aBOOK
001416519 980__ $$bREPORT
001416519 980__ $$aPREPRINT
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