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Related papers: Z' Reservation at LC2000

200 papers

We propose an extended 2HDM with $Q_6\times Z_4\times Z_2$ symmetry that can successfully accommodate the SM fermion mass and mixing hierarchy. The tiny masses of the active neutrinos are generated from a type-I seesaw mechanism mediated by…

High Energy Physics - Phenomenology · Physics 2024-10-30 V. V. Vien , H. N. Long , A. E. Cárcamo Hernández , Juan Marchant González

We consider a new physics model, where the Standard Model (SM) is extended by hyperchargeless $Y=0$ triplet fermions and Higgs triplet with hypercharge $Y=2$. The first two generation fermion triplets are even under the $Z_2$…

High Energy Physics - Phenomenology · Physics 2023-04-21 Pritam Das , Najimuddin Khan

Many new physics models predict the existence of extra neutral gauge bosons ($Z'$). Inspired by the recent development on Higgs search, we study the properties of $Z'$ via the Higgs and $Z$ boson associated production. The couplings of $Z'$…

High Energy Physics - Phenomenology · Physics 2013-06-26 Hong-Lei Li , Zong-Guo Si , Xiu-Yi Yang , Zhong-Juan Yang , Ya-Juan Zheng

We study the implications of an approximate $U(2)^5$ flavor symmetry at the TeV scale, under the assumption of new physics predominantly coupled to the third-generation fermions, focusing on the breaking of the $U(2)_\ell$ subgroup…

High Energy Physics - Phenomenology · Physics 2025-11-21 Sebastiano Covone , Pol Morell , Arianna Tinari

I comment on the proposal that the stability of dark matter may be due to an unbroken Z_2 symmetry contained in the partially broken lepton flavour symmetry group. I remark that (1) there is no Z_2 symmetry apparent in the lepton mass…

High Energy Physics - Phenomenology · Physics 2015-05-30 L. Lavoura

Using a low-energy effective field theory approach, we study some properties of models with large extra dimensions, in which quarks and leptons have localized wave functions in the extra dimensions. We consider models with two types of…

High Energy Physics - Phenomenology · Physics 2021-01-22 S. Girmohanta , R. N. Mohapatra , R. Shrock

Certain string-inspired Z' models have non-universal interactions to three families of fermions and induced tree-level flavor-changing couplings. We use recent results on B_s-anti-B_s mixing to constrain the size of the flavor-changing…

High Energy Physics - Phenomenology · Physics 2008-11-26 Kingman Cheung , Cheng-Wei Chiang , N. G. Deshpande , J. Jiang

The Fermilab Tevatron collider experiments, CDF and \dz, have collected over 200 ${\rm pb}^{-1}$ of data at $\sqrt{s}=1.96$ TeV since March 2002 (RunII). Both experiments have investigated physics beyond the Standard Model; this paper…

High Energy Physics - Experiment · Physics 2007-05-23 By CDF , D0 collaborations

A lepton-flavor violating (LFV) Z' boson may mimic some of the phenomena usually attributed to supersymmetric theories. Using a conservative model of LFV Z' bosons, the recent BNL E821 muon g-2 deviation allows for a LFV Z' interpretation…

High Energy Physics - Phenomenology · Physics 2009-11-07 Brandon Murakami

We discuss a simple renormalisable, gauge invariant model with a fermiophobic $Z'$ boson: it has no couplings to the three Standard Model (SM) chiral families, but does couple to a fourth vector-like (VL) family. The SM Higgs couples to the…

High Energy Physics - Phenomenology · Physics 2022-02-16 Mario Fernández Navarro , Stephen F. King

Naturally small neutrino masses can arise in some grand unified models. The mechanism of neutrino mass generation in these models typically requires the existence of neutral heavy leptons. We study the low-energy phenomenology of these new…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ivan Melo

We present a search for supersymmetry in the R-parity violating resonant production and decay of smuons and muon-sneutrinos in the channels smuon->neutralino_1 muon, smuon->neutralino_2 muon, and muon-sneutrino->chargino muon. We analyzed…

High Energy Physics - Experiment · Physics 2008-11-26 D0 Collaboration , V. Abazov

We recently proposed a spontaneous A$_{4}$ flavor symmetry breaking scheme implemented in a warped extra dimensional setup to explain the observed pattern of quark and lepton masses and mixings. The main features of this choice are the…

High Energy Physics - Phenomenology · Physics 2013-07-05 Avihay Kadosh

We revisit the dark matter phenomenology of a flavor-dependent $U(1)_X$ gauge extension of the Standard Model, where anomaly cancellation predicts the existence of exactly three fermion generations and requires the presence of three…

High Energy Physics - Phenomenology · Physics 2026-03-26 N. T. Duy , Duy H. Nguyen , Do Thi Ha , Duong Van Loi

We attempt to explain recent anomalies in semileptonic $B$ decays at LHCb via a composite Higgs model, in which both the Higgs and an $SU(2)_L$-triplet leptoquark arise as pseudo-Goldstone bosons of the strong dynamics. Fermion masses are…

High Energy Physics - Phenomenology · Physics 2015-06-12 Ben Gripaios , Marco Nardecchia , S. A. Renner

In this work we will extend the inert-doublet model (IDM) by adding a new $U(1)_{F}$ gauge symmetry to it, under which, a $Z_{2}$ even scalar ($\phi_{2}$) and $Z_{2}$ odd right handed component of two exotic charged leptons $(F_{eR},\…

High Energy Physics - Phenomenology · Physics 2018-04-25 Lobsang Dhargyal

This Letter describes the current most precise measurement of the $WZ$ production cross section as well as limits on anomalous $WWZ$ couplings at a center-of-mass energy of 1.96 TeV in proton-antiproton collisions for the Collider Detector…

High Energy Physics - Experiment · Physics 2013-05-30 CDF Collaboration , T. Aaltonen , B. Alvarez González , S. Amerio , D. Amidei , A. Anastassovx , A. Annovi , J. Antos , G. Apollinari , J. A. Appel , T. Arisawa , A. Artikov , J. Asaadi , W. Ashmanskas , B. Auerbach , A. Aurisano , F. Azfar , W. Badgett , T. Bae , A. Barbaro-Galtieri , V. E. Barnes , B. A. Barnett , P. Barriahh , P. Bartos , M. Bauce , F. Bedeschi , S. Behari , G. Bellettinig , J. Bellinger , D. Benjamin , A. Beretvas , A. Bhatti , D. Bisellof , I. Bizjak , K. R. Bland , B. Blumenfeld , A. Bocci , A. Bodek , D. Bortoletto , J. Boudreau , A. Boveia , L. Brigliadoriee , C. Bromberg , E. Brucken , J. Budagov , H. S. Budd , K. Burkett , G. Busetto , P. Bussey , A. Buzatu , A. Calamba , C. Calancha , S. Camarda , M. Campanelli , M. Campbell , F. Canelli , B. Carls , D. Carlsmith , R. Carosi , S. Carrillom , S. Carron , B. Casalk , M. Casarsa , A. Castroee , P. Catastini , D. Cauz , V. Cavaliere , M. Cavalli-Sforza , A. Cerrif , L. Cerritos , Y. C. Chen , M. Chertok , G. Chiarelli , G. Chlachidze , F. Chlebana , K. Cho , D. Chokheli , W. H. Chung , Y. S. Chung , M. A. Cioccihh , A. Clark , C. Clarke , G. Compostella , M. E. Convery , J. Conway , M. Corbo , M. Cordelli , C. A. Cox , D. J. Cox , F. Crescioligg , J. Cuevasz , R. Culbertson , D. Dagenhart , N. d'Ascenzo , M. Datta , P. de Barbaro , M. Del'Orso , L. Demortier , M. Deninno , F. Devoto , M. d'Errico , A. Di Cantogg , B. Di Ruzza , J. R. Dittmann , M. D'Onofrio , S. Donatigg , P. Dong , M. Dorigo , T. Dorigo , K. Ebina , A. Elagin , A. Eppig , R. Erbacher , S. Errede , N. Ershaidatdd , R. Eusebi , S. Farrington , M. Feindt , J. P. Fernandez , R. Field , G. Flanaganu , R. Forrest , M. J. Frank , M. Franklin , J. C. Freeman , Y. Funakoshi , I. Furic , M. Gallinaro , J. E. Garcia , A. F. Garfinkel , P. Garosihh , H. Gerberich , E. Gerchtein , S. Giagu , V. Giakoumopoulou , P. Giannetti , K. Gibson , C. M. Ginsburg , N. Giokaris , P. Giromini , G. Giurgiu , V. Glagolev , D. Glenzinski , M. Gold , D. Goldin , N. Goldschmidt , A. Golossanov , G. Gomez , G. Gomez-Ceballos , M. Goncharov , O. González , I. Gorelov , A. T. Goshaw , K. Goulianos , S. Grinstein , C. Grosso-Pilcher , R. C. Group , J. Guimaraes da Costa , S. R. Hahn , E. Halkiadakis , A. Hamaguchi , J. Y. Han , F. Happacher , K. Hara , D. Hare , M. Hare , R. F. Harr , K. Hatakeyama , C. Hays , M. Heck , J. Heinrich , M. Herndon , S. Hewamanage , D. Hidas , A. Hocker , W. Hopkinsg , D. Horn , S. Hou , R. E. Hughes , M. Hurwitz , U. Husemann , N. Hussain , M. Hussein , J. Huston , G. Introzzi , M. Iorijj , A. Ivanovp , E. James , D. Jang , B. Jayatilaka , E. J. Jeon , S. Jindariani , M. Jones , K. K. Joo , S. Y. Jun , T. R. Junk , T. Kamon , P. E. Karchin , A. Kasmi , Y. Katoo , W. Ketchum , J. Keung , V. Khotilovich , B. Kilminster , D. H. Kim , H. S. Kim , J. E. Kim , M. J. Kim , S. B. Kim , S. H. Kim , Y. K. Kim , Y. J. Kim , N. Kimura , M. Kirby , S. Klimenko , K. Knoepfel , K. Kondo , D. J. Kong , J. Konigsberg , A. V. Kotwal , M. Kreps , J. Kroll , D. Krop , M. Kruse , V. Krutelyovc , T. Kuhr , M. Kurata , S. Kwang , A. T. Laasanen , S. Lami , S. Lammel , M. Lancaster , R. L. Lander , K. Lannony , A. Lath , G. Latinohh , T. LeCompte , E. Lee , H. S. Leeq , J. S. Lee , S. W. Leebb , S. Leogg , S. Leone , J. D. Lewis , A. Limosanit , C. -J. Lin , M. Lindgren , E. Lipeles , A. Lister , D. O. Litvintsev , C. Liu , H. Liu , Q. Liu , T. Liu , S. Lockwitz , A. Loginov , D. Lucchesi , J. Lueck , P. Lujan , P. Lukens , G. Lungu , J. Lys , R. Lysake , R. Madrak , K. Maeshima , P. Maestrohh , S. Malik , G. Mancaa , A. Manousakis-Katsikakis , F. Margaroli , C. Marino , M. Martínez , P. Mastrandrea , K. Matera , M. E. Mattson , A. Mazzacane , P. Mazzanti , K. S. McFarland , P. McIntyre , R. McNultyj , A. Mehta , P. Mehtala , C. Mesropian , T. Miao , D. Mietlicki , A. Mitra , H. Miyake , S. Moed , N. Moggi , M. N. Mondragonm , C. S. Moon , R. Moore , M. J. Morelloii , J. Morlock , P. Movilla Fernandez , A. Mukherjee , Th. Muller , P. Murat , M. Mussiniee , J. Nachtmann , Y. Nagai , J. Naganoma , I. Nakano , A. Napier , J. Nett , C. Neu , M. S. Neubauer , J. Nielsend , L. Nodulman , S. Y. Noh , O. Norniella , L. Oakes , S. H. Oh , Y. D. Oh , I. Oksuzian , T. Okusawa , R. Orava , L. Ortolan , S. Pagan Griso , C. Pagliarone , E. Palenciaf , V. Papadimitriou , A. A. Paramonov , J. Patrick , G. Paulettakk , M. Paulini , C. Paus , D. E. Pellett , A. Penzo , T. J. Phillips , G. Piacentino , E. Pianori , J. Pilot , K. Pitts , C. Plager , L. Pondrom , S. Poprockig , K. Potamianos , F. Prokoshincc , A. Pranko , F. Ptohosh , G. Punzigg , J. Pursley , A. Rahaman , V. Ramakrishnan , N. Ranjan , I. Redondo , P. Renton , M. Rescigno , T. Riddick , F. Rimondiee , L. Ristori , A. Robson , T. Rodrigo , T. Rodriguez , E. Rogers , S. Rollii , R. Roser , F. Ruffinihh , A. Ruiz , J. Russ , V. Rusu , A. Safonov , W. K. Sakumoto , Y. Sakurai , L. Santikk , K. Sato , V. Savelievw , A. Savoy-Navarroaa , P. Schlabach , A. Schmidt , E. E. Schmidt , T. Schwarz , L. Scodellaro , A. Scribanohh , F. Scuri , S. Seidel , Y. Seiya , A. Semenov , F. Sforzahh , S. Z. Shalhout , T. Shears , P. F. Shepard , M. Shimojimav , M. Shochet , I. Shreyber-Tecker , A. Simonenko , P. Sinervo , K. Sliwa , J. R. Smith , F. D. Snider , A. Soha , V. Sorin , H. Song , P. Squillaciotihh , M. Stancari , R. St. Denis , B. Stelzer , O. Stelzer-Chilton , D. Stentzx , J. Strologas , G. L. Strycker , Y. Sudo , A. Sukhanov , I. Suslov , K. Takemasa , Y. Takeuchi , J. Tang , M. Tecchio , P. K. Teng , J. Thomg , J. Thome , G. A. Thompson , E. Thomson , D. Toback , S. Tokar , K. Tollefson , T. Tomura , D. Tonelli , S. Torre , D. Torretta , P. Totaro , M. Trovatoii , F. Ukegawa , S. Uozumi , R. Vanguri , A. Varganov , F. Vázquez , G. Velev , C. Vellidis , M. Vidal , I. Vila , R. Vilar , J. Vizán , M. Vogel , G. Volpi , P. Wagner , R. L. Wagner , T. Wakisaka , R. Wallny , S. M. Wang , A. Warburton , D. Waters , W. C. Wester , D. Whiteson , A. B. Wicklund , E. Wicklund , S. Wilbur , F. Wick , H. H. Williams , J. S. Wilson , P. Wilson , B. L. Winer , P. Wittichg , S. Wolbers , H. Wolfe , T. Wright , X. Wu , Z. Wu , K. Yamamoto , D. Yamato , T. Yang , U. K. Yangr , Y. C. Yang , W. -M. Yao , G. P. Yeh , K. Yin , J. Yoh , K. Yorita , T. Yoshidal , G. B. Yu , I. Yu , S. S. Yu , J. C. Yun , A. Zanetti , Y. Zeng , C. Zhou , S. Zucchelli

In this work, the standard model (SM) is extended with two right-handed (RH) neutrinos and two singlet neutral fermions to yield active neutrino masses via (2,2) inverse see-saw mechanism. We first validate the multi-dimensional model…

High Energy Physics - Phenomenology · Physics 2023-04-26 Indrani Chakraborty , Himadri Roy , Tripurari Srivastava

Lattice gauge theories are a powerful language to theoretically describe a variety of strongly correlated systems, including frustrated magnets, high-$T_c$ superconductors, and topological phases. However, in many cases gauge fields couple…

Strongly Correlated Electrons · Physics 2017-11-07 Christian Prosko , Shu-Ping Lee , Joseph Maciejko

Many extensions of the standard model, especially grand unified theories and superstring models, predict the existence of additional Z' bosons and associated exotic chiral supermultiplets. It has recently been argued that for classes of…

High Energy Physics - Phenomenology · Physics 2007-05-23 Paul Langacker