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If supersymmetry is discovered at the LHC, the measured spectrum of superpartner masses and couplings will allow us to probe the origins of supersymmetry breaking. However, to connect the collider-scale Lagrangian soft parameters to the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Gordon L. Kane , Piyush Kumar , David E. Morrissey , Manuel Toharia

Extending the sensitivity to New Physics beyond the anticipated reach of the LHC is a prime aim of future colliders. This paper summarises the potential of an e+e- linear collider, at and beyond 1 TeV, using a realistic simulation of the…

High Energy Physics - Phenomenology · Physics 2009-09-25 M. Battaglia , S. De Curtis , D. Dominici , S. Riemann

LHCb is a dedicated heavy flavour physics precision experiment at the LHC searching for New Physics (NP) beyond the Standard Model (SM) through the study of very rare decays of beauty and charm-flavoured hadrons and precision measurements…

High Energy Physics - Experiment · Physics 2015-06-12 Monica Pepe Altarelli

Fundamental particle physics is at a cross road. On the one hand the Standard Model successfully accounts for all experimental observations to date. On the other hand the ElectroWeak symmetry breaking mechanism is poorly understood and…

High Energy Physics - Phenomenology · Physics 2025-04-30 Alon E. Faraggi

We present a pedagogical, but by no means complete, review of weak scale supersymmetry phenomenology. After a general introduction to the new particles that must be present in any supersymmetric framework, we describe how to write down…

High Energy Physics - Phenomenology · Physics 2008-02-03 Xerxes Tata

A strong candidate for the Standard Model Scalar boson, H(126), has been discovered by the Large Hadron Collider (LHC) experiments. In order to study this fundamental particle with unprecedented precision, and to perform precision tests of…

The Standard Model (SM) is the best description of fundamental particles and their interactions we have to date. From this theory, all phenomena in the macroscopic world (except for gravity) can be explained, and it has successfully…

High Energy Physics - Phenomenology · Physics 2024-07-30 Joan Ruiz-Vidal

If the mechanism of Supersymmetry breaking is not flavour blind, some flavour symmetry is likely to be needed to prevent excessive flavour changing neutral current effects. We discuss two flavour models (based respectively on a U(2) and on…

High Energy Physics - Phenomenology · Physics 2014-11-17 A. Masiero , M. Piai , A. Romanino , L. Silvestrini

In this Technical Design Report (TDR) we describe the SuperB detector that was to be installed on the SuperB e+e- high luminosity collider. The SuperB asymmetric collider, which was to be constructed on the Tor Vergata campus near the INFN…

Instrumentation and Detectors · Physics 2013-06-25 SuperB Collaboration , M. Baszczyk , P. Dorosz , J. Kolodziej , W. Kucewicz , M. Sapor , A. Jeremie , E. Grauges Pous , G. E. Bruno , G. De Robertis , D. Diacono , G. Donvito , P. Fusco , F. Gargano , F. Giordano , F. Loddo , F. Loparco , G. P. Maggi , V. Manzari , M. N. Mazziotta , E. Nappi , A. Palano , B. Santeramo , I. Sgura , L. Silvestris , V. Spinoso , G. Eigen , J. Zalieckas , Z. Zhuo , L. Jenkovszky , G. Balbi , M. Boldini , D. Bonacorsi , V. Cafaro , I. D'Antone , G. M. Dallavalle , R. Di Sipio , F. Fabbri , L. Fabbri , A. Gabrielli , D. Galli , P. Giacomelli , V. Giordano , F. M. Giorgi , C. Grandi , I. Lax , S. Lo Meo , U. Marconi , A. Montanari , G. Pellegrini , M. Piccinini , T. Rovelli , N. Semprini Cesari , G. Torromeo , N. Tosi , R. Travaglini , V. M. Vagnoni , S. Valentinetti , M. Villa , A. Zoccoli , J. -F. Caron , C. Hearty , P. F. -T. Lu , T. S. Mattison , J. A. McKenna , R. Y. -C. So , M. Yu. Barnyakov , V. E. Blinov , A. A. Botov , V. P. Druzhinin , V. B. Golubev , S. A. Kononov , E. A. Kravchenko , E. B. Levichev , A. P. Onuchin , S. I. Serednyakov , D. A. Shtol , Y. I. Skovpen , E. P. Solodov , A. Cardini , M. Carpinelli , D. S. -T. Chao , C. H. Cheng , D. A. Doll , B. Echenard , K. Flood , J. Hanson , D. G. Hitlin , P. Ongmongkolkul , F. C. Porter , R. Y. Zhu , N. Randazzo , E. De La Cruz Burelo , Y. Zheng , P. Campos , M. De Silva , A. Kathirgamaraju , B. Meadows , B. Pushpawela , Y. Shi , M. Sokoloff , G. Lopez Castro , V. Ciaschini , P. Franchini , F. Giacomini , A. Paolini , G. A. Calderon Polania , S. Laczek , P. Romanowicz , B. Szybinski , M. Czuchry , L. Flis , D. Harezlak , J. Kocot , M. Radecki , M. Sterzel , T. Szepieniec , T. Szymocha , P. Wójcik , M. Andreotti , W. Baldini , R. Calabrese , V. Carassiti , G. Cibinetto , A. Cotta Ramusino , F. Evangelisti , A. Gianoli , E. Luppi , R. Malaguti , M. Manzali , M. Melchiorri , M. Munerato , C. Padoan , V. Santoro , L. Tomassetti , M. M. Beretta , M. Biagini , M. Boscolo , E. Capitolo , R. de Sangro , M. Esposito , G. Felici , G. Finocchiaro , M. Gatta , C. Gatti , S. Guiducci , S. Lauciani , P. Patteri , I. Peruzzi , M. Piccolo , P. Raimondi , M. Rama , C. Sanelli , S. Tomassini , P. Fabbricatore , D. Delepine , M. A. Reyes Santos , M. Chrzaszcz , R. Grzymkowski , P. Knap , J. Kotula , T. Lesiak , J. Ludwin , J. Michalowski , B. Pawlik , B. Rachwal , M. Stodulski , J. Wiechczynski , M. Witek , L. Zawiejski , M. Zdybal , V. Y. Aushev , A. Ustynov , N. Arnaud , P. Bambade , C. Beigbeder , F. Bogard , M. Borsato , D. Breton , J. Brossard , L. Burmistrov , D. Charlet , V. Chaumat , O. Dadoun , M. El Berni , J. Maalmi , V. Puill , C. Rimbault , A. Stocchi , V. Tocut , A. Variola , S. Wallon , G. Wormser , F. Grancagnolo , E. Ben-Haim , S. Sitt , M. Baylac , O. Bourrion , J. -M. Deconto , Y. Gomez Martinez , N. Monseu , J. -F. Muraz , J. -S. Real , C. Vescovi , R. Cenci , A. Jawahery , D. Roberts , E. W. Twedt , R. Cheaib , D. Lindemann , S. Nderitu , P. Patel , S. H. Robertson , D. Swersky , A. Warburton , E. Cuautle Flores , G. Toledo Sanchez , P. Biassoni , L. Bombelli , M. Citterio , S. Coelli , C. Fiorini , V. Liberali , M. Monti , B. Nasri , N. Neri , F. Palombo , F. Sabatini , A. Stabile , A. Berra , A. Giachero , C. Gotti , D. Lietti , M. Maino , G. Pessina , M. Prest , J. -P. Martin , M. Simard , N. Starinski , P. Taras , A. Drutskoy , S. Makarychev , A. V. Nefediev , A. Aloisio , S. Cavaliere , G. De Nardo , M. Della Pietra , A. Doria , R. Giordano , A. Ordine , S. Pardi , G. Russo , C. Sciacca , I. I. Bigi , C. P. Jessop , W. Wang , M. Bellato , M. Benettoni , M. Corvo , A. Crescente , F. Dal Corso , U. Dosselli , C. Fanin , A. Gianelle , S. Longo , M. Michelotto , F. Montecassiano , M. Morandin , R. Pengo , M. Posocco , M. Rotondo , G. Simi , R. Stroili , L. Gaioni , A. Manazza , M. Manghisoni , L. Ratti , V. Re , G. Traversi , S. Zucca , S. Bizzaglia , M. Bizzarri , C. Cecchi , S. Germani , M. Lebeau , P. Lubrano , E. Manoni , A. Papi , A. Rossi , G. Scolieri , G. Batignani , S. Bettarini , G. Casarosa , A. Cervelli , A. Fella , F. Forti , M. Giorgi , L. Lilli , A. Lusiani , B. Oberhof , A. Paladino , F. Pantaleo , E. Paoloni , A. L. Perez Perez , G. Rizzo , J. Walsh , A. Fernández Téllez , G. Beck , M. Berman , A. Bevan , F. Gannaway , G. Inguglia , A. J. Martin , J. Morris , V. Bocci , M. Capodiferro , G. Chiodi , I. Dafinei , N. V. Drenska , R. Faccini , F. Ferroni , C. Gargiulo , P. Gauzzi , C. Luci , R. Lunadei , G. Martellotti , F. Pellegrino , V. Pettinacci , D. Pinci , L. Recchia , D. Ruggeri , A. Zullo , P. Camarri , R. Cardarelli , C. De Santis , A. Di Ciaccio , V. Di Felice , F. Di Palma , A. Di Simone , L. Marcelli , R. Messi , D. Moricciani , R. Sparvoli , S. Tammaro , P. Branchini , A. Budano , S. Bussino , M. Ciuchini , F. Nguyen , A. Passeri , F. Ruggieri , E. Spiriti , F. Wilson , I. Leon Monzon , J. R. Millan-Almaraz , P. L. M. Podesta-Lerma , D. Aston , B. Dey , A. Fisher , P. D. Jackson , D. W. G. S. Leith , S. Luitz , D. MacFarlane , M. McCulloch , S. Metcalfe , A. Novokhatski , S. Osier , R. Prepost , B. Ratcliff , J. Seeman , M. Sullivan , J. Va'vra , U. Wienands , W. Wisniewski , B. D. Altschul , M. V. Purohit , J. Baudot , I. Ripp-Baudot , G. A. P. Cirrone , G. Cuttone , O. Bezshyyko , G. Dolinska , A. Soffer , F. Bianchi , F. De Mori , A. Filippi , D. Gamba , S. Marcello , M. Bomben , L. Bosisio , P. Cristaudo , L. Lanceri , B. Liberti , I. Rashevskaya , C. Stella , E. S. Vallazza , L. Vitale , G. Auriemma , C. Satriano , F. Martinez Vidal , J. Mazorra de Cos , A. Oyanguren , P. Ruiz Valls , A. Beaulieu , S. Dejong , J. Franta , M. J. Lewczuk , M. Roney , R. Sobie

Belle II experiment at the SuperKEKB collider is a major upgrade of the Belle experiment at the KEKB asymmetric e^+e^- collider at the KEK. The experiment will focus on the search for new physics beyond the standard model via high precision…

Instrumentation and Detectors · Physics 2012-08-21 C. Z. Yuan

We describe the physics potential of $e^+e^-$ linear colliders in this report. These machines are planned to operate in the first phase at a center-of --mass energy of 500 GeV, before being scaled up to about 1 TeV. In the second phase of…

High Energy Physics - Phenomenology · Physics 2009-09-25 E. Accomando

Can the Large Hadron Collider explain the masses and mixings of the known fermions? A promising possibility is that these masses and mixings are determined by flavor symmetries that also govern new particles that will appear at the LHC. We…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jonathan L. Feng , Christopher G. Lester , Yosef Nir , Yael Shadmi

The LHCb detector has been designed to study CP violation and other rare phenomena in B-meson decays up to a luminosity of $\sim 5.10^{32}\rm cm^{-2}s^{-1}$. This paper will describe what is limiting LHCb to exploit the much higher…

High Energy Physics - Experiment · Physics 2008-11-26 H. Dijkstra

Flavour changing neutral currents are only allowed via loop diagrams in the Standard Model (SM). Electroweak penguin processes are therefore sensitive probes for new physics, as physics beyond the Standard Model can enter via virtual…

High Energy Physics - Experiment · Physics 2013-01-01 Michel De Cian

The standard model of particle physics is an extremely successful theory of fundamental interactions, but it has many known limitations. It is therefore widely believed to be an effective field theory that describes interactions near the…

High Energy Physics - Experiment · Physics 2019-02-04 Salvatore Rappoccio

The next 20 years will be the golden age of flavour physics, with the operation of the LHCb and Belle II experiments. After that an $e^+e^-$ collider could further improve the precision with sizeable $Z$, $W^+W^-$ and $t\bar{t}$ runs.

High Energy Physics - Experiment · Physics 2026-04-23 Patrick Koppenburg

LHCb is the dedicated B physics experiment at the LHC and is due to start data taking later this year. Its goal is to search for new physics in very rare processes and make precision measurements of CP violation in B decays. The CKM angle…

High Energy Physics - Experiment · Physics 2009-06-01 Ying Ying Li

The next-generation experiments on Heavy Flavour Physics must be performed at the hadron colliders to exploit the superior production cross-section and availability of all the species of b and c flavored hadrons. The particularly hostile…

High Energy Physics - Phenomenology · Physics 2019-08-14 Luigi Moroni

The next generation of $e^{-}e^{+}$ colliders, particularly the CEPC and FCC-ee, will offer unprecedented precision to probe Higgs boson properties. In this work, we investigate the flavor-changing decay $h \rightarrow bs$ produced via…

High Energy Physics - Phenomenology · Physics 2025-07-03 M. A. Arroyo-Ureña , Diego Carreño , A. I. García-Gutierrez , M. G. Villanueva-Utrilla , T. A. Valencia-Pérez

With the nearing completion of the first-generation experiments at asymmetric $e^+ e^-$ colliders running at the $\Upsilon(4S)$ resonance ("B-Factories") a new era of high luminosity machines is at the horizon. We report here on the plans…

High Energy Physics - Experiment · Physics 2010-01-15 Christian Kiesling