Search for doubly-charged Higgs bosons at LEP

Achard, P.; Адриани, О.; Benitez, M. Aguilar; Alcaraz, J.; Alemanni, G.; Allaby, J.; Aloisio, A.; Alviggi, M. G.; Anderhub, H.; Andreev, V.; Anselmo, F.; Arefiev, A.; Azemoon, T.; Aziz, T.; Bagnaia, P.; Bajo, A.; Baksay, G.; Baksay, L.; Baldew, S.V.; Banerjee, S.; Barczyk, A.; Barillère, R.; Bartalini, P.; Basile, M.; Batalova, N.; Battiston, R.; Bay, A.; Becattini, F.; Becker, U.; Behner, F.; Bellucci, L.; Berbeco, R.; Berdugo, J.; Berges, P.; Bertucci, B.; Betev, B.L.; Biasini, M.; Biglietti, M.; Biland, A.; Blaising, J. J.; Blyth, S.; Bobbink, G. J.; Böhm, A.; Boldizsár, L.; Borgia, B.; Bottai, S.; Bourilkov, D.; Bourquin, M.; Braccini, S.; Branson, J. G.; Brochu, F. M.; Bürger, J.; Burger, W. J.; Cai, X. D.; Capell, M.; Romeo, G. Cara; Carlino, G.; Cartacci, A. M.; Casaus, J.; Cavallari, F.; Cavallo, N.; Cecchi, C.; Cerrada, M.; Chamizo, M.; Chang, Y. H.; Chemarin, M.; Chen, A; Chen, G; Chen, GM; Chen, Hf; Chen, HS; Chiefari, G.; Cifarelli, L.; Cindolo, F.; Clare, I.; Clare, R.; Coignet, G.; Colino, N.; Costantini, S.; Cruz, B. De La; Cucciarelli, S.; Ja, van Dalen; Asmundis, R. de; Déglon, P.; Debreczeni, J.; Degré, A.; Dehmelt, K.; Deiters, K.; Volpe, D. della; Delmeire, E.; Denes, P.; Notaristefani, F. de; Salvo, A. De; Diemoz, M.; Dierckxsens, M.; Dionisi, C.; Dittmar, M.; Doria, A.; Dova, M. T.; Duchesneau, D.; Duda, M.; Echenard, B.; Eline, A.; Hage, A. El; Mamouni, H. El; Engler, A.; Eppling, F. J.; Extermann, P.; Falagán, M. A.; Falciano, S.; Favara, A.; Fay, J.; Fedin, O. L.; Felcini, M.; Ferguson, T.; Fesefeldt, H.; Fiandrini, E.; Field, J. H.; Filthaut, F.; Fisher, P. H.; Fisher, W.; Fisk, I.; Forconì, G.; Freudenreich, K.; Furetta, C.; Galaktionov, Yu.; Ganguli, S.N.; Abia, P. García; Gataullin, M.; Gentile, S.; Giagu, S.; Gong, Z. F.; Greco, Filippo; Grenier, G.; Grimm, O.; Gruenewald, M. W.; Guida, M.; Gulik, R. van; Gupta, V. K.; Gurtu, A.; Gutay, L.; Haas, D.; Hatzifotiadou, D.; Hebbeker, T.; Hervé, A.; Hirschfelder, J.; Höfer, H.; Hohlmann, M.; Holzner, G.; Hou,; Hu, Y.; Jin, B. N.; Jones, L.T.; Jong, P. de; Josa-Mutuberria, I.; Käfer, D.; Kaur, M.; Mn, Kienzle Focacci; Jk, Kim; Kirkby, J.; Kittel, W.; Klimentov, A.; König, A. C.; Kopál, M.; Koutsenko,; Kräber, M.; Kraemer, R.W.; Krüger, A.; Kunin, A.; Pl, de Guevara; Laktineh, I. B.; Landi, G.; Lebeau, M.; Lebedev, A.; Lebrun, P.; Lecomte, P.; Lecoq, P.; Coultre, P. Le; Jm, Le Goff; Leiste, R.; Levtchenko, M.; Levtchenko, P.; Li, C; Likhoded, S.; Lin, C. J.; Lin, W.; Linde, F.L.; Lista, L.; Liu, Za; Lohmann, W.; Longo, E.; Lu, Y.S.; Luci, C.; Luminari, L.; Lustermann, W.; Ma, W.G.; Malgeri, L.; Малинин, А.; Mañá, C.; Mans, J.; Martin, J. P.; Marzano, F.; Mazumdar, K.; McNeil, R. R.; Mele, S.; Merola, L.; Meschini, M.; Metzger, W. J.; Mihul, A.; Milcent, H.; Mirabelli, G.; Mnich, J.; Mohanty, G. B.; Muanza, G. S.; Muijs, A. J.M.; Musicar, B.; Musy, M.; Nagy, S.; Natale, Sonia; Napolitano, M.; Tedaldi, F Nessi; Newman, H. B.; Nisati, A.; Novák, T.; Nowak, H.; Ofierzynski, R. A.; Organtini, G.; Pal, I.; Palomares, C.; Paolucci, P.; Paramatti, R.; Passaleva, G.; Patricelli, S.; Paul, T.; Pauluzzi, M.; Paus, C.; Pauß, F.; Pedace, M.; Pensotti, S.; Gallix, D Perret; Petersen, B. A.; Piccolo, D.; Pierella, F.; Pioppí, M.; Piroué, P.; Pistolesi, E.; Plyaskin,; Pohl, M.; Pojidaev,; Pothier, J.; Prokofiev, D.; Quartieri, J.; Callot, G Rahal; Rahaman, M. A.; Raics, P.; Raja, N.; Ramelli, R.; Rancoita, P.G.; Ranieri, R.; Raspereza, A.; Razis, P. A.; Ren, D.; Rescigno, M.; Reucroft, S.; Riemann, S.; Riles, K.; Roe, B.P.; Romero, L.; Rosca, A.; Rosenbleck, C.; Lees, Sidney; Roth, Stefan; Rubio, J. A.; Ruggiero, G.; Rykaczewski, H.; Sakharov, A.; Saremi, S.; Sarkar, S.; Salicio, J.; Sánchez, E.; Schäfer, C.; Schegelsky,; Schopper, H.; Schotanus, D. J.; Sciacca, C.; Servoli, L.; Shevchenko, S.; Shivarov, N.; Shoutko,; Shumilov, E.; Shvorob, A.; Son, D. C.; Souga, C.; Спиллантини, П.; Steuer, M.; Stickland, D.; Stoyanov, B.; Straessner, A.; Sudhakar, K.; Sultanov, G.; Sun, L.; Sushkov, S.; Suter, H.; Swain, J. D.; Szillási, Z.; Tang, X. W.; Tarján, P.; Tauscher, L.; Taylor, L.; Tellili, B.; Teyssier, D.; Timmermans, C.; Ting, S. M.; Ting, Sm; Tonwar, S. C.; Töth, J.; Tully, C.; Tung, K. L.; Ulbricht, J.; Valente, E.; Rt, Van de Walle; Vasquez, Raymond; Veszprémi,; Vesztergombi, G.; Vetlitsky, I.; Vicinanza, D.; Viertel, G.; Villa, S.; Vivargent, M.; Vlachos, S.; Vodopianov, I.; Vogel, H.; Vogt, H.; Vorobiev, I.; Vorobyov, A.A.; Wadhwa, M.; Wang, Q; Xl, Wang; Zm, Wang; Weber, M.; Wienemann, P.; Wilkens, H. G.; Wynhoff, S.; Xia, L.; Xu, Z.; Yamamoto, J.; Yang, B. Z.; Yang, C. G.; Yang, H. J.; Yang, M.; Yeh, Sc; Zalite, A.; Zalite, Yu.; Zhang, ZP; Zhao, J. Y.; Zhu, G. Y.; Zhu, R. Y.; Zhuang, H.L.; Zichichi, A.; Zimmermann, B.; Zöller, Margot

doi:10.1016/j.physletb.2003.09.082

Cited by 67 publications

(40 citation statements)

References 48 publications

(10 reference statements)

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“…For all reasons above, models with Higgs triplet is very important for nowadays state of art in the searching for a more complete universal particle model. Important searches have been proposed, as for instance, in hadron colliders [12], in LEP at CERN, as OPAL detector, including Bhabha scattering [13] or in L3 and Delphi groups [14]. In HERA at DESY, through ep collision [15] and several others collision experiments as γγ collision [16], eγ collision [17] as in SLAC, or even via Z → H ++ H −− [18] or even through W fusion [19].…”

Section: Introductionmentioning

confidence: 99%

Probing doubly charged Higgs bosons ine+e−colliders at the ILC and the CLIC in a 3-3-1 model

Montalvo

Cortez²,

Tonasse

2008

Phys. Rev. D

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Section: Introductionmentioning

confidence: 99%

Probing doubly charged Higgs bosons ine+e−colliders at the ILC and the CLIC in a 3-3-1 model

Montalvo

Cortez²,

Tonasse

2008

Phys. Rev. D

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“…Therefore, the contributions of heavy gauge bosons to relic density and muon (g − 2) will be small in comparison to charged scalars. By choosing the coupling of ∆ ++ to e − e − to be much smaller than the coupling with µ − µ − , we can evade the precession constraints from LEP [69]. We have assumed no flavor mixing through ∆ R , otherwise it will give rise to large contribution to µ → eγ and µ → eee process, which is not observed [60].…”

Section: Discussionmentioning

confidence: 99%

Explaining AMS-02 positron excess and muon anomalous magnetic moment in dark left-right gauge model

Basak

Mohanty

Tomar

2016

J. High Energ. Phys.

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In a Dark left-right gauge model, the neutral component of right-handed lepton doublet is odd under generalized R-parity and thus the lightest one serves as the dark matter (DM) candidate. The coannihilation of the dark matter with the singly charged Higgs triplet produces the correct relic abundance. We explain AMS-02 positron excess by the annihilation of 800 GeV dark matter into µ + µ − γ, through a t-channel exchange of the additional charged triplet Higgs boson. The DM is leptophilic which is useful for explaining the non-observation of any antiproton excess which would generically be expected from DM annihilation. The large cross-section needed to explain AMS-02 also requires an astrophysical boost. In addition, we show that the muon (g − 2) receives required contribution from singly and doubly charged triplet Higgs in the loops.

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“…A search for doubly-charged Higgs bosons has been done at LEP [71], Tevatron [72] and LHC [73]. All these searches have been done under the assumption where doubly-charged Higgs bosons decay into the same sign dilepton.…”

Section: B Signature Of ∆ ±± At Lhcmentioning

confidence: 99%

Two-loop radiative seesaw model with inert triplet scalar field

Kajiyama¹,

Okada

Yagyu

2013

Nuclear Physics B

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We propose a radiative seesaw model with an inert triplet scalar field in which Majorana neutrino masses are generated at the two loop level. There are fermionic or bosonic dark matter candidates in the model. We find that each candidate can satisfy the WMAP data when its mass is taken to be around the half of the mass of the standard model like Higgs boson. We also discuss phenomenology of the inert triplet scalar bosons, especially focusing on the doubly-charged scalar bosons at Large Hadron Collider in parameter regions constrained by the electroweak precision data and WMAP data. We study how we can distinguish our model from the minimal Higgs triplet model.

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Search for doubly-charged Higgs bosons at LEP

Cited by 67 publications

References 48 publications

Probing doubly charged Higgs bosons ine+e−colliders at the ILC and the CLIC in a 3-3-1 model

Probing doubly charged Higgs bosons ine+e−colliders at the ILC and the CLIC in a 3-3-1 model

Explaining AMS-02 positron excess and muon anomalous magnetic moment in dark left-right gauge model

Two-loop radiative seesaw model with inert triplet scalar field

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