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Related papers: Vector dark matter at the LHC

200 papers

We systematically study models with light scalar and pseudoscalar dark matter candidates and their potential signals at the LHC. First, we derive cosmological bounds on models with the Standard Model Higgs mediator and with a new weak-scale…

High Energy Physics - Phenomenology · Physics 2021-02-10 Martin Bauer , Patrick Foldenauer , Peter Reimitz , Tilman Plehn

This article reports on a search for dark matter pair production in association with bottom or top quarks in 20.3 fb$^{-1}$ of $pp$ collisions collected at $\sqrt{s} = 8$ TeV by the ATLAS detector at the LHC. Events with large missing…

High Energy Physics - Experiment · Physics 2015-03-26 ATLAS Collaboration

Direct detection of dark matter (DM) requires an interaction of dark matter particles with nucleons. The same interaction can lead to dark matter pair production at a hadron collider, and with the addition of initial state radiation this…

High Energy Physics - Phenomenology · Physics 2011-01-05 Yang Bai , Patrick J. Fox , Roni Harnik

We consider dark sector particles (DSPs) that obtain sizeable interactions with Standard Model fermions from a new mediator. While these particles can avoid observation in direct detection experiments, they are strongly constrained by LHC…

High Energy Physics - Phenomenology · Physics 2015-07-28 Mikael Chala , Felix Kahlhoefer , Matthew McCullough , Germano Nardini , Kai Schmidt-Hoberg

We consider the proposal that dark matter (DM) is composed of a spin-3/2 particle that is a singlet of the standard model (SM). Its leading effective interactions with ordinary matter involve a pair of their fields and a pair of SM…

High Energy Physics - Phenomenology · Physics 2013-05-31 Ran Ding , Yi Liao , Ji-Yuan Liu , Kai Wang

We study the interactions of a new spin-1 mediator that connects the Standard Model to dark matter. We constrain its decay channels using monojet and monophoton searches, as well as searches for resonances in dijet, dilepton and diboson…

High Energy Physics - Phenomenology · Physics 2012-07-27 Mads T. Frandsen , Felix Kahlhoefer , Anthony Preston , Subir Sarkar , Kai Schmidt-Hoberg

A search for dark matter and unparticle production at the LHC has been performed using events containing two charged leptons (electrons or muons), consistent with the decay of a Z boson, and large missing transverse momentum. This study is…

High Energy Physics - Experiment · Physics 2018-01-23 CMS Collaboration

This paper presents a search for dark matter in the context of a two-Higgs-doublet model together with an additional pseudoscalar mediator, $a$, which decays into the dark-matter particles. Processes where the pseudoscalar mediator is…

High Energy Physics - Experiment · Physics 2021-12-03 ATLAS Collaboration

We investigate a mono-Z process as a potential dark matter search strategy at the LHC. In this channel a single Z boson recoils against missing transverse momentum, attributed to dark matter particles, $\chi$, which escape the detector.…

High Energy Physics - Phenomenology · Physics 2012-12-20 Nicole F. Bell , James B. Dent , Ahmad J. Galea , Thomas D. Jacques , Lawrence M. Krauss , Thomas J. Weiler

In a large class of scenarios, dark matter (DM) particles that belong to a multiplet of the standard model (SM) weak interactions are challenging to probe in direct detection experiments due to loop-suppressed cross-sections. Direct…

High Energy Physics - Phenomenology · Physics 2019-04-15 Tao Han , Satyanarayan Mukhopadhyay , Xing Wang

Searches for dark matter at colliders typically involve signatures with energetic initial-state radiation without visible recoil particles. Searches for mono-jet or mono-photon signatures have yielded powerful constraints on dark matter…

High Energy Physics - Experiment · Physics 2015-06-12 Linda M. Carpenter , Andrew Nelson , Chase Shimmin , Tim M. P. Tait , Daniel Whiteson

Many models containing particles which are candidates for dark matter, assume the standard model particles and the dark matter candidates are mediated by a spin-0 particle. At the LHC, one can use these models for dark matter searches. One…

High Energy Physics - Experiment · Physics 2019-03-20 Yoav Afik , Eitan Gozani , Yoram Rozen

A weakly interacting dark-matter particle may be difficult to discover at an accelerator because it either (1) is too massive, (2) has no standard-model gauge interactions, or (3) is almost degenerate with other states. In each of these…

Astrophysics · Physics 2007-05-23 James D. Wells

We introduce a set of minimal simplified models for dark matter interactions with the Standard Model, connecting the two sectors via either a scalar or pseudoscalar particle. These models have a wider regime of validity for dark matter…

High Energy Physics - Phenomenology · Physics 2015-06-23 Matthew R. Buckley , David Feld , Dorival Goncalves

A search for evidence of particle dark matter (DM) and unparticle production at the LHC has been performed using events containing two charged leptons, consistent with the decay of a Z boson, and large missing transverse momentum. This…

High Energy Physics - Experiment · Physics 2016-04-14 CMS Collaboration

We present the results of a search for dark matter production in the monojet signature. We analyze a sample of Tevatron pp-bar collisions at sqrt(s)=1.96 TeV corresponding to an integrated luminosity of 6.7/fb recorded by the CDF II…

High Energy Physics - Experiment · Physics 2015-06-04 The CDF Collaboration , T. Aaltonen , B. Álvarez González , S. Amerio , D. Amidei , A. Anastassov , 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 , Y. Bai , A. Barbaro-Galtieri , V. E. Barnes , B. A. Barnett , P. Barria , P. Bartos , M. Bauce , F. Bedeschi , S. Behari , G. Bellettini , J. Bellinger , D. Benjamin , A. Beretvas , A. Bhatti , D. Bisello , I. Bizjak , K. R. Bland , B. Blumenfeld , A. Bocci , A. Bodek , D. Bortoletto , J. Boudreau , A. Boveia , L. Brigliadori , 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. Carrillo , S. Carron , B. Casal , M. Casarsa , A. Castro , P. Catastini , D. Cauz , V. Cavaliere , M. Cavalli-Sforza , A. Cerri , L. Cerrito , Y. C. Chen , M. Chertok , G. Chiarelli , G. Chlachidze , F. Chlebana , K. Cho , D. Chokheli , W. H. Chung , Y. S. Chung , M. A. Ciocci , A. Clark , C. Clarke , G. Compostella , M. E. Convery , J. Conway , M. Corbo , M. Cordelli , C. A. Cox , D. J. Cox , F. Crescioli , J. Cuevas , R. Culbertson , D. Dagenhart , N. d'Ascenzo , M. Datta , P. de Barbaro , M. Dell'Orso , L. Demortier , M. Deninno , F. Devoto , M. d'Errico , A. Di Canto , B. Di Ruzza , J. R. Dittmann , M. D'Onofrio , S. Donati , P. Dong , M. Dorigo , T. Dorigo , K. Ebina , A. Elagin , A. Eppig , R. Erbacher , S. Errede , N. Ershaidat , R. Eusebi , S. Farrington , M. Feindt , J. P. Fernandez , R. Field , G. Flanagan , R. Forrest , P. J. Fox , M. J. Frank , M. Franklin , J. C. Freeman , Y. Funakoshi , I. Furic , M. Gallinaro , J. E. Garcia , A. F. Garfinkel , P. Garosi , 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. Harnik , R. F. Harr , K. Hatakeyama , C. Hays , M. Heck , J. Heinrich , M. Herndon , S. Hewamanage , A. Hocker , W. Hopkins , D. Horn , S. Hou , R. E. Hughes , M. Hurwitz , U. Husemann , N. Hussain , M. Hussein , J. Huston , G. Introzzi , M. Iori , A. Ivanov , 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. Kato , 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. Krutelyov , T. Kuhr , M. Kurata , S. Kwang , A. T. Laasanen , S. Lami , S. Lammel , M. Lancaster , R. L. Lander , K. Lannon , A. Lath , G. Latino , T. LeCompte , E. Lee , H. S. Lee , J. S. Lee , S. W. Lee , S. Leo , S. Leone , J. D. Lewis , A. Limosani , 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. Lysak , R. Madrak , K. Maeshima , P. Maestro , S. Malik , G. Manca , 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. McNulty , A. Mehta , P. Mehtala , C. Mesropian , T. Miao , D. Mietlicki , A. Mitra , H. Miyake , S. Moed , N. Moggi , M. N. Mondragon , C. S. Moon , R. Moore , M. J. Morello , J. Morlock , P. Movilla Fernandez , A. Mukherjee , Th. Muller , P. Murat , M. Mussini , J. Nachtman , Y. Nagai , J. Naganoma , I. Nakano , A. Napier , J. Nett , C. Neu , M. S. Neubauer , J. Nielsen , 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. Palencia , V. Papadimitriou , A. A. Paramonov , J. Patrick , G. Pauletta , C. Paus , D. E. Pellett , A. Penzo , T. J. Phillips , G. Piacentino , E. Pianori , J. Pilot , K. Pitts , C. Plager , L. Pondrom , S. Poprocki , K. Potamianos , F. Prokoshin , A. Pranko , F. Ptohos , G. Punzi , A. Rahaman , V. Ramakrishnan , N. Ranjan , I. Redondo , P. Renton , M. Rescigno , T. Riddick , F. Rimondi , L. Ristori , A. Robson , T. Rodrigo , T. Rodriguez , E. Rogers , S. Rolli , R. Roser , F. Ruffini , A. Ruiz , J. Russ , V. Rusu , A. Safonov , W. K. Sakumoto , Y. Sakurai , L. Santi , K. Sato , V. Saveliev , A. Savoy-Navarro , P. Schlabach , A. Schmidt , E. E. Schmidt , T. Schwarz , L. Scodellaro , A. Scribano , F. Scuri , S. Seidel , Y. Seiya , A. Semenov , F. Sforza , S. Z. Shalhout , T. Shears , P. F. Shepard , M. Shimojima , M. Shochet , I. Shreyber-Tecker , A. Simonenko , P. Sinervo , K. Sliwa , J. R. Smith , F. D. Snider , A. Soha , V. Sorin , H. Song , P. Squillacioti , M. Stancari , R. St. Denis , B. Stelzer , O. Stelzer-Chilton , D. Stentz , J. Strologas , G. L. Strycker , Y. Sudo , A. Sukhanov , I. Suslov , K. Takemasa , Y. Takeuchi , J. Tang , M. Tecchio , P. K. Teng , J. Thom , J. Thome , G. A. Thompson , E. Thomson , D. Toback , S. Tokar , K. Tollefson , T. Tomura , D. Tonelli , S. Torre , D. Torretta , P. Totaro , M. Trovato , F. Ukegawa , S. Uozumi , 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. Wittich , S. Wolbers , H. Wolfe , T. Wright , X. Wu , Z. Wu , K. Yamamoto , D. Yamato , T. Yang , U. K. Yang , Y. C. Yang , W. -M. Yao , G. P. Yeh , K. Yi , J. Yoh , K. Yorita , T. Yoshida , G. B. Yu , I. Yu , S. S. Yu , J. C. Yun , A. Zanetti , Y. Zeng , C. Zhou , S. Zucchelli

We explore the properties of self-conjugate dark matter (DM) particles that predominantly interact with Standard Model electroweak gauge bosons, using an effective field theory approach. The study emphasizes effective contact interactions,…

High Energy Physics - Phenomenology · Physics 2025-06-06 Hrishabh Bharadwaj

The perturbative unitarity bound is studied in the monojet process at LHC. The production of the dark matter is described by the low-energy effective theory. The analysis of the dark matter signal is not validated, if the unitarity…

High Energy Physics - Phenomenology · Physics 2014-06-24 Motoi Endo , Yasuhiro Yamamoto

A consistent model for vector mediators to dark matter needs to be anomaly-free and include a scalar mode from mass generation. For the leading U(1) extensions we review the structure and constraints, including kinetic mixing at loop level.…

High Energy Physics - Phenomenology · Physics 2018-10-24 Martin Bauer , Sascha Diefenbacher , Tilman Plehn , Michael Russell , Daniel A. Camargo

We examine the sensitivity of the Large Hadron Collider (LHC) to light lepton portal dark matter with its mass below 10$\,$GeV. The model features an extra doublet scalar field and singlet Dirac dark matter, which have Yukawa interactions…

High Energy Physics - Phenomenology · Physics 2023-06-09 Syuhei Iguro , Shohei Okawa , Yuji Omura