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We explore, in a concrete example, to which extent new particle mass determinations are practicable with LHC data. Our chosen example is that of Yukawa-unified SUSY GUTs, whose viability has been recently studied for two general patterns of…

High Energy Physics - Phenomenology · Physics 2015-03-17 Kiwoon Choi , Diego Guadagnoli , Sang Hui Im , Chan Beom Park

The observation of three events for the decay $\Sigma^+ \to p \mu^+ \mu^-$ with a dimuon invariant mass of $214.3\pm0.5$MeV by the HyperCP collaboration imply that a new particle X may be needed to explain the observed dimuon invariant mass…

High Energy Physics - Phenomenology · Physics 2008-11-26 Gao Xiangdong , Chong Sheng Li , Zhao Li , Hao Zhang

We present a detailed study of the collider observable $m_{T2}$ applied for pair-produced superparticles decaying to visible particles and a pair of invisible lightest supersymmetric particles (LSPs). Analytic expressions of the maximum of…

High Energy Physics - Phenomenology · Physics 2008-11-26 Won Sang Cho , Kiwoon Choi , Yeong Gyun Kim , Chan Beom Park

Machine-learning (ML) techniques are explored to identify and classify hadronic decays of highly Lorentz-boosted W/Z/Higgs bosons and top quarks. Techniques without ML have also been evaluated and are included for comparison. The…

High Energy Physics - Experiment · Physics 2020-06-09 CMS Collaboration

Measurements of b-hadron masses are performed with the exclusive decay modes B+ -> J/psi K+, B0 -> J/psi K*0, B0 -> J/psi K0S, B0_s -> J/psi phi and Lambda_b -> J/psi Lambda using an integrated luminosity of 35 pb-1 collected in pp…

High Energy Physics - Experiment · Physics 2012-02-13 LHCb Collaboration , R. Aaij , C. Abellan Beteta , B. Adeva , M. Adinolfi , C. Adrover , A. Affolder , Z. Ajaltouni , J. Albrecht , F. Alessio , M. Alexander , G. Alkhazov , P. Alvarez Cartelle , A. A. Alves , S. Amato , Y. Amhis , J. Anderson , R. B. Appleby , O. Aquines Gutierrez , F. Archilli , L. Arrabito , A. Artamonov , M. Artuso , E. Aslanides , G. Auriemma , S. Bachmann , J. J. Back , D. S. Bailey , V. Balagura , W. Baldini , R. J. Barlow , C. Barschel , S. Barsuk , W. Barter , A. Bates , C. Bauer , Th. Bauer , A. Bay , I. Bediaga , S. Belogurov , K. Belous , I. Belyaev , E. Ben-Haim , M. Benayoun , G. Bencivenni , S. Benson , J. Benton , R. Bernet , M. -O. Bettler , M. van Beuzekom , A. Bien , S. Bifani , T. Bird , A. Bizzeti , P. M. Bjørnstad , T. Blake , F. Blanc , C. Blanks , J. Blouw , S. Blusk , A. Bobrov , V. Bocci , A. Bondar , N. Bondar , W. Bonivento , S. Borghi , A. Borgia , T. J. V. Bowcock , C. Bozzi , T. Brambach , J. van den Brand , J. Bressieux , D. Brett , M. Britsch , T. Britton , N. H. Brook , A. Büchler-Germann , I. Burducea , A. Bursche , J. Buytaert , S. Cadeddu , O. Callot , M. Calvi , M. Calvo Gomez , A. Camboni , P. Campana , A. Carbone , G. Carboni , R. Cardinale , A. Cardini , L. Carson , K. Carvalho Akiba , G. Casse , M. Cattaneo , Ch. Cauet , M. Charles , Ph. Charpentier , N. Chiapolini , K. Ciba , X. Cid Vidal , G. Ciezarek , P. E. L. Clarke , M. Clemencic , H. V. Cliff , J. Closier , C. Coca , V. Coco , J. Cogan , P. Collins , A. Comerma-Montells , F. Constantin , A. Contu , A. Cook , M. Coombes , G. Corti , G. A. Cowan , R. Currie , C. D'Ambrosio , P. David , P. N. Y. David , I. De Bonis , S. De Capua , M. De Cian , F. De Lorenzi , J. M. De Miranda , L. De Paula , P. De Simone , D. Decamp , M. Deckenhoff , H. Degaudenzi , L. Del Buono , C. Deplano , D. Derkach , O. Deschamps , F. Dettori , J. Dickens , H. Dijkstra , P. Diniz Batista , F. Domingo Bonal , S. Donleavy , F. Dordei , A. Dosil Suárez , D. Dossett , A. Dovbnya , F. Dupertuis , R. Dzhelyadin , A. Dziurda , S. Easo , U. Egede , V. Egorychev , S. Eidelman , D. van Eijk , F. Eisele , S. Eisenhardt , R. Ekelhof , L. Eklund , Ch. Elsasser , D. Elsby , D. Esperante Pereira , L. Estève , A. Falabella , E. Fanchini , C. Färber , G. Fardell , C. Farinelli , S. Farry , V. Fave , V. Fernandez Albor , M. Ferro-Luzzi , S. Filippov , C. Fitzpatrick , M. Fontana , F. Fontanelli , R. Forty , M. Frank , C. Frei , M. Frosini , S. Furcas , A. Gallas Torreira , D. Galli , M. Gandelman , P. Gandini , Y. Gao , J-C. Garnier , J. Garofoli , J. Garra Tico , L. Garrido , D. Gascon , C. Gaspar , N. Gauvin , M. Gersabeck , T. Gershon , Ph. Ghez , V. Gibson , V. V. Gligorov , C. Göbel , D. Golubkov , A. Golutvin , A. Gomes , H. Gordon , M. Grabalosa Gándara , R. Graciani Diaz , L. A. Granado Cardoso , E. Graugés , G. Graziani , A. Grecu , E. Greening , S. Gregson , B. Gui , E. Gushchin , Yu. Guz , T. Gys , G. Haefeli , C. Haen , S. C. Haines , T. Hampson , S. Hansmann-Menzemer , R. Harji , N. Harnew , J. Harrison , P. F. Harrison , T. Hartmann , J. He , V. Heijne , K. Hennessy , P. Henrard , J. A. Hernando Morata , E. van Herwijnen , E. Hicks , K. Holubyev , P. Hopchev , W. Hulsbergen , P. Hunt , T. Huse , R. S. Huston , D. Hutchcroft , D. Hynds , V. Iakovenko , P. Ilten , J. Imong , R. Jacobsson , A. Jaeger , M. Jahjah Hussein , E. Jans , F. Jansen , P. Jaton , B. Jean-Marie , F. Jing , M. John , D. Johnson , C. R. Jones , B. Jost , M. Kaballo , S. Kandybei , M. Karacson , T. M. Karbach , J. Keaveney , I. R. Kenyon , U. Kerzel , T. Ketel , A. Keune , B. Khanji , Y. M. Kim , M. Knecht , A. Kozlinskiy , L. Kravchuk , K. Kreplin , M. Kreps , G. Krocker , P. Krokovny , F. Kruse , K. Kruzelecki , M. Kucharczyk , T. Kvaratskheliya , V. N. La Thi , D. Lacarrere , G. Lafferty , A. Lai , D. Lambert , R. W. Lambert , E. Lanciotti , G. Lanfranchi , C. Langenbruch , T. Latham , C. Lazzeroni , R. Le Gac , J. van Leerdam , J. -P. Lees , R. Lefèvre , A. Leflat , J. Lefrançois , O. Leroy , T. Lesiak , L. Li , L. Li Gioi , M. Lieng , M. Liles , R. Lindner , C. Linn , B. Liu , G. Liu , J. von Loeben , J. H. Lopes , E. Lopez Asamar , N. Lopez-March , H. Lu , J. Luisier , A. Mac Raighne , F. Machefert , I. V. Machikhiliyan , F. Maciuc , O. Maev , J. Magnin , S. Malde , R. M. D. Mamunur , G. Manca , G. Mancinelli , N. Mangiafave , U. Marconi , R. Märki , J. Marks , G. Martellotti , A. Martens , L. Martin , A. Martín Sánchez , D. Martinez Santos , A. Massafferri , Z. Mathe , C. Matteuzzi , M. Matveev , E. Maurice , B. Maynard , A. Mazurov , G. McGregor , R. McNulty , M. Meissner , M. Merk , J. Merkel , R. Messi , S. Miglioranzi , D. A. Milanes , M. -N. Minard , J. Molina Rodriguez , S. Monteil , D. Moran , P. Morawski , R. Mountain , I. Mous , F. Muheim , K. Müller , R. Muresan , B. Muryn , B. Muster , M. Musy , J. Mylroie-Smith , P. Naik , T. Nakada , R. Nandakumar , I. Nasteva , M. Nedos , M. Needham , N. Neufeld , C. Nguyen-Mau , M. Nicol , V. Niess , N. Nikitin , A. Nomerotski , A. Novoselov , A. Oblakowska-Mucha , V. Obraztsov , S. Oggero , S. Ogilvy , O. Okhrimenko , R. Oldeman , M. Orlandea , J. M. Otalora Goicochea , P. Owen , K. Pal , J. Palacios , A. Palano , M. Palutan , J. Panman , A. Papanestis , M. Pappagallo , C. Parkes , C. J. Parkinson , G. Passaleva , G. D. Patel , M. Patel , S. K. Paterson , G. N. Patrick , C. Patrignani , C. Pavel-Nicorescu , A. Pazos Alvarez , A. Pellegrino , G. Penso , M. Pepe Altarelli , S. Perazzini , D. L. Perego , E. Perez Trigo , A. Pérez-Calero Yzquierdo , P. Perret , M. Perrin-Terrin , G. Pessina , A. Petrella , A. Petrolini , A. Phan , E. Picatoste Olloqui , B. Pie Valls , B. Pietrzyk , T. Pilař , D. Pinci , R. Plackett , S. Playfer , M. Plo Casasus , G. Polok , A. Poluektov , E. Polycarpo , D. Popov , B. Popovici , C. Potterat , A. Powell , J. Prisciandaro , V. Pugatch , A. Puig Navarro , W. Qian , J. H. Rademacker , B. Rakotomiaramanana , M. S. Rangel , I. Raniuk , G. Raven , S. Redford , M. M. Reid , A. C. dos Reis , S. Ricciardi , K. Rinnert , D. A. Roa Romero , P. Robbe , E. Rodrigues , F. Rodrigues , P. Rodriguez Perez , G. J. Rogers , S. Roiser , V. Romanovsky , M. Rosello , J. Rouvinet , T. Ruf , H. Ruiz , G. Sabatino , J. J. Saborido Silva , N. Sagidova , P. Sail , B. Saitta , C. Salzmann , M. Sannino , R. Santacesaria , C. Santamarina Rios , R. Santinelli , E. Santovetti , M. Sapunov , A. Sarti , C. Satriano , A. Satta , M. Savrie , D. Savrina , P. Schaack , M. Schiller , S. Schleich , M. Schlupp , M. Schmelling , B. Schmidt , O. Schneider , A. Schopper , M. -H. Schune , R. Schwemmer , B. Sciascia , A. Sciubba , M. Seco , A. Semennikov , K. Senderowska , I. Sepp , N. Serra , J. Serrano , P. Seyfert , M. Shapkin , I. Shapoval , P. Shatalov , Y. Shcheglov , T. Shears , L. Shekhtman , O. Shevchenko , V. Shevchenko , A. Shires , R. Silva Coutinho , T. Skwarnicki , A. C. Smith , N. A. Smith , E. Smith , K. Sobczak , F. J. P. Soler , A. Solomin , F. Soomro , B. Souza De Paula , B. Spaan , A. Sparkes , P. Spradlin , F. Stagni , S. Stahl , O. Steinkamp , S. Stoica , S. Stone , B. Storaci , M. Straticiuc , U. Straumann , V. K. Subbiah , S. Swientek , M. Szczekowski , P. Szczypka , T. Szumlak , S. T'Jampens , E. Teodorescu , F. Teubert , C. Thomas , E. Thomas , J. van Tilburg , V. Tisserand , M. Tobin , S. Topp-Joergensen , N. Torr , E. Tournefier , M. T. Tran , A. Tsaregorodtsev , N. Tuning , M. Ubeda Garcia , A. Ukleja , P. Urquijo , U. Uwer , V. Vagnoni , G. Valenti , R. Vazquez Gomez , P. Vazquez Regueiro , S. Vecchi , J. J. Velthuis , M. Veltri , B. Viaud , I. Videau , X. Vilasis-Cardona , J. Visniakov , A. Vollhardt , D. Volyanskyy , D. Voong , A. Vorobyev , H. Voss , S. Wandernoth , J. Wang , D. R. Ward , N. K. Watson , A. D. Webber , D. Websdale , M. Whitehead , D. Wiedner , L. Wiggers , G. Wilkinson , M. P. Williams , M. Williams , F. F. Wilson , J. Wishahi , M. Witek , W. Witzeling , S. A. Wotton , K. Wyllie , Y. Xie , F. Xing , Z. Xing , Z. Yang , R. Young , O. Yushchenko , M. Zavertyaev , F. Zhang , L. Zhang , W. C. Zhang , Y. Zhang , A. Zhelezov , L. Zhong , E. Zverev , A. Zvyagin

We review several methods for determining the Kobayashi-Maskawa phase $\gamma={\rm Arg} V^*_{ub}$ from rate and CP asymmetry measurements in hadronic B decays. We focus on the processes $B\to DK, B_s\to D_s K$, and on charmless decays to…

High Energy Physics - Phenomenology · Physics 2016-11-23 Michael Gronau

The bulk of visible mass is supposed to emerge from nonperturbative dynamics within quantum chromodynamics (QCD). Following years of development and refinement, continuum and lattice Schwinger function methods have recently joined in…

High Energy Physics - Phenomenology · Physics 2026-01-15 Daniele Binosi , Craig D. Roberts , Zhao-Qian Yao

We present a technique for estimating the number of future neutrinoless double-beta decay results using several distinct nuclei to optimize the physics reach of upcoming experiments. We use presently available matrix element calculations…

High Energy Physics - Phenomenology · Physics 2008-11-26 V. M. Gehman , S. R. Elliott

We investigate the extent to which theories of collective motion can capture the physics that determines the nuclear matrix elements governing neutrinoless double-beta decay. To that end we calculate the matrix elements for a series of…

Nuclear Theory · Physics 2016-02-17 J. Menéndez , N. Hinohara , J. Engel , G. Martínez-Pinedo , T. R. Rodríguez

Kinematic edges in the invariant mass distributions of different final state particles are typically a signal of new physics. In this work we propose a scenario wherein these edges could be utilised in discriminating between different…

High Energy Physics - Phenomenology · Physics 2017-03-08 Abhishek M. Iyer , Ushoshi Maitra

New light bosons that couple weakly to the standard model (SM) particles are predicted in various extensions of the standard model (BSM). Examples include supersymmetric (SUSY) theories with extended Higgs sectors or with a hidden valleys…

The production of invisible particles plays great importance in high energy physics. Large part of interesting electroweak processes include production of neutrinos, while many new physics scenarios predict the existence of similarly…

High Energy Physics - Experiment · Physics 2012-05-22 Marco Bentivegna , Qiuguang Liu , Fabrizio Margaroli , Karolos Potamianos

Several physical systems in condensed matter have been modeled approximating their constituent particles as hard objects. The hard spheres model has been indeed one of the cornerstones of the computational and theoretical description in…

Computational Physics · Physics 2015-05-13 Cristiano De Michele

We present a method of analyzing invariant-mass spectra of kaon pairs resulting from decay of $\phi$ mesons produced in high-energy heavy-ion collisions. It can be used to extract the shifts in the mass and the width ($\Delta M$ and $\Delta…

High Energy Physics - Phenomenology · Physics 2015-06-25 R. S. Bhalerao , S. K. Gupta

We study the implications for $B_s - \bar B_s$ mixing and the neutron electric dipole moment (EDM) in a light dark matter model with sizable invisible rare meson decays to accommodate the recent possible deviations from Standard Model (SM)…

High Energy Physics - Phenomenology · Physics 2026-03-26 Xuan Hong , Xiao-Gang He , Ming-Wei Li

We present a new method for resolving combinatorial ambiguities that arise in multi-particle decay chains at hadron colliders where the assignment of visible particles to the different decay chains has ambiguities. Our method, based on…

High Energy Physics - Phenomenology · Physics 2011-05-25 Arvind Rajaraman , Felix Yu

An instructional laboratory experiment to measure the muon mass is described. Using coincidence-anticoincidence detection, the decay of a cosmic-ray muon into an electron (or positron) is observed in a multiplate spark chamber, and recorded…

Physics Education · Physics 2010-02-05 Benjamin Brau , Christopher May , Robert Ormond , John Essick

These lectures review some of the progress made in the quantitative understanding of B decays. The emphasis here is on applications of QCD using perturbative and non-perturbative techniques. In some cases, however, phenomenological models…

High Energy Physics - Phenomenology · Physics 2011-04-15 A. Ali

There are three observables related to neutrino mass, namely the kinematic mass in direct searches, the effective mass in neutrino-less double beta decay, and the sum of neutrino masses in cosmology. In the limit of exactly degenerate…

High Energy Physics - Phenomenology · Physics 2010-05-12 Werner Rodejohann

A long standing problem in kinematics at the hadron colliders is to determine the mass of invisible particles. This issue is particularly important for the signals of dark matter, which becomes one of the prominent targets of future…

High Energy Physics - Phenomenology · Physics 2020-04-01 Zachary Flowers , Dong Woo Kang , Quinn Meier , Seong Chan Park , Christopher Rogan