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Search for new phenomena in events with three or more charged leptons in pp collisions at s√=8 TeV with the ATLAS detector

Aad, G. ; Abbott, B. ; Abdallah, J. ; Khalek, S. Abdel ; Abdinov, O. ; Aben, R. ; Abi, B. ; Abolins, M. ; AbouZeid, O. S. and Abramowicz, H. , et al. (2015) In Journal of High Energy Physics
Abstract
A generic search for anomalous production of events with at least three charged leptons is presented. The data sample consists of pp collisions at TeV collected in 2012 by the ATLAS experiment at the CERN Large Hadron Collider, and corresponds to an integrated luminosity of 20.3 fb(-1). Events are required to have at least three selected lepton candidates, at least two of which must be electrons or muons, while the third may be a hadronically decaying tau. Selected events are categorized based on their lepton flavour content and signal regions are constructed using several kinematic variables of interest. No significant deviations from Standard Model predictions are observed. Model-independent upper limits on contributions from beyond the... (More)
A generic search for anomalous production of events with at least three charged leptons is presented. The data sample consists of pp collisions at TeV collected in 2012 by the ATLAS experiment at the CERN Large Hadron Collider, and corresponds to an integrated luminosity of 20.3 fb(-1). Events are required to have at least three selected lepton candidates, at least two of which must be electrons or muons, while the third may be a hadronically decaying tau. Selected events are categorized based on their lepton flavour content and signal regions are constructed using several kinematic variables of interest. No significant deviations from Standard Model predictions are observed. Model-independent upper limits on contributions from beyond the Standard Model phenomena are provided for each signal region, along with prescription to re-interpret the limits for any model. Constraints are also placed on models predicting doubly charged Higgs bosons and excited leptons. For doubly charged Higgs bosons decaying to e tau or mu tau, lower limits on the mass are set at 400 GeV at 95% confidence level. For excited leptons, constraints are provided as functions of both the mass of the excited state and the compositeness scale I >, with the strongest mass constraints arising in regions where the mass equals I >. In such scenarios, lower mass limits are set at 3.0 TeV for excited electrons and muons, 2.5 TeV for excited taus, and 1.6 TeV for every excited-neutrino flavour. (Less)
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; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; and (Less)
organization
publishing date
type
Contribution to journal
publication status
published
subject
keywords
Hadron-Hadron Scattering
in
Journal of High Energy Physics
issue
8
article number
138
publisher
Springer
external identifiers
  • wos:000361002900001
  • scopus:84978025686
ISSN
1029-8479
DOI
10.1007/JHEP08(2015)138
language
English
LU publication?
yes
id
1e60a707-c23e-4ad9-8959-b559ffeb5de6 (old id 8071239)
date added to LUP
2016-04-01 11:14:38
date last changed
2023-01-02 19:44:40
@article{1e60a707-c23e-4ad9-8959-b559ffeb5de6,
  abstract     = {{A generic search for anomalous production of events with at least three charged leptons is presented. The data sample consists of pp collisions at TeV collected in 2012 by the ATLAS experiment at the CERN Large Hadron Collider, and corresponds to an integrated luminosity of 20.3 fb(-1). Events are required to have at least three selected lepton candidates, at least two of which must be electrons or muons, while the third may be a hadronically decaying tau. Selected events are categorized based on their lepton flavour content and signal regions are constructed using several kinematic variables of interest. No significant deviations from Standard Model predictions are observed. Model-independent upper limits on contributions from beyond the Standard Model phenomena are provided for each signal region, along with prescription to re-interpret the limits for any model. Constraints are also placed on models predicting doubly charged Higgs bosons and excited leptons. For doubly charged Higgs bosons decaying to e tau or mu tau, lower limits on the mass are set at 400 GeV at 95% confidence level. For excited leptons, constraints are provided as functions of both the mass of the excited state and the compositeness scale I >, with the strongest mass constraints arising in regions where the mass equals I >. In such scenarios, lower mass limits are set at 3.0 TeV for excited electrons and muons, 2.5 TeV for excited taus, and 1.6 TeV for every excited-neutrino flavour.}},
  author       = {{Aad, G. and Abbott, B. and Abdallah, J. and Khalek, S. Abdel and Abdinov, O. and Aben, R. and Abi, B. and Abolins, M. and AbouZeid, O. S. and Abramowicz, H. and Abreu, H. and Abreu, R. and Abulaiti, Y. and Acharya, B. S. and Adamczyk, L. and Adams, D. L. and Adelman, J. and Adomeit, S. and Adye, T. and Agatonovic-Jovin, T. and Aguilar-Saavedra, J. A. and Agustoni, M. and Ahlen, S. P. and Ahmadov, F. and Aielli, G. and Akerstedt, H. and Åkesson, Torsten and Akimoto, G. and Akimov, A. V. and Alberghi, G. L. and Albert, J. and Albrand, S. and Alconada Verzini, M. J. and Aleksa, M. and Aleksandrov, I. N. and Alexa, C. and Alexander, G. and Alexandre, G. and Alexopoulos, T. and Alhroob, M. and Alimonti, G. and Alio, L. and Alison, J. and Allbrooke, B. M. M. and Allison, L. J. and Allport, P. P. and Aloisio, A. and Alonso, A. and Alonso, F. and Alpigiani, C. and Altheimer, A. and Alvarez Gonzalez, B. and Alviggi, M. G. and Amako, K. and Amaral Coutinho, Y. and Amelung, C. and Amidei, D. and Amor Dos Santos, S. P. and Amorim, A. and Amoroso, S. and Amram, N. and Amundsen, G. and Anastopoulos, C. and Ancu, L. S. and Andari, N. and Andeen, T. and Anders, C. F. and Anders, G. and Anderson, K. J. and Andreazza, A. and Andrei, V. and Anduaga, X. S. and Angelidakis, S. and Angelozzi, I. and Anger, P. and Angerami, A. and Anghinolfi, F. and Anisenkov, A. V. and Anjos, N. and Annovi, A. and Antonelli, M. and Antonov, A. and Antos, J. and Anulli, F. and Aoki, M. and Aperio Bella, L. and Arabidze, G. and Arai, Y. and Araque, J. P. and Arce, A. T. H. and Arduh, F. A. and Arguin, J-F. and Argyropoulos, S. and Arik, M. and Armbruster, A. J. and Arnaez, O. and Arnal, V. and Arnold, H. and Arratia, M. and Arslan, O. and Artamonov, A. and Artoni, G. and Asai, S. and Asbah, N. and Ashkenazi, A. and Azuman, B. and Asquith, L. and Assamagan, K. and Astalos, R. and Atkinson, M. and Atlay, N. B. and Auerbach, B. and Augsten, K. and Aurousseau, M. and Avolio, G. and Axen, B. and Azuelos, G. and Azuma, Y. and Baak, M. A. and Baas, A. E. and Bacci, C. and Bachacou, H. and Bachas, K. and Backes, M. and Backhaus, M. and Badescu, E. and Bagiacchi, P. and Bagnaia, P. and Bai, Y. and Bain, T. and Baines, J. T. and Baker, O. K. and Balek, P. and Balli, F. and Banas, E. and Banerjee, Sw. and Bannoura, A. A. E. and Bansil, H. S. and Barak, L. and Baranov, S. P. and Barberio, E. L. and Barberis, D. and Barbero, M. and Barillari, T. and Barisonzi, M. and Barklow, T. and Barlow, N. and Barnes, S. L. and Barnett, B. M. and Barnett, R. M. and Barnovska, Z. and Baroncelli, A. and Barone, G. and Barr, A. J. and Barreiro, F. and Barreiro Guimares da Costa, J. and Bartoldus, R. and Barton, A. E. and Bartos, P. and Bartsch, V. and Bassalat, A. and Basye, A. and Bates, R. L. and Batista, S. J. and Batley, J. R. and Battaglia, M. and Battistin, M. and Bauer, F. and Bawa, H. S. and Beacham, J. B. and Beattie, M. D. and Beau, T. and Beauchemin, P. H. and Beccherle, R. and Bechtle, P. and Beck, H. P. and Becker, K. and Becker, S. and Beckingham, M. and Becot, C. and Beddall, A. J. and Beddall, A. and Bedikian, S. and Bednyakov, V. A. and Bee, C. P. and Beemster, L. J. and Beermann, T. A. and Begel, M. and Behr, K. and Belanger-Champagne, C. and Bell, P. J. and Bell, W. H. and Bella, G. and Bellagamba, L. and Bellerive, A. and Bellomo, M. and Belotskiy, K. and Beltramello, O. and Benary, O. and Benchekroun, D. and Bendtz, K. and Benekos, N. and Benhammou, Y. and Benhar Noccioli, E. and Benitez Garcia, J. A. and Benjamin, D. P. and Bensinger, J. R. and Bentvelsen, S. and Berge, D. and Bergeaas Kuutmann, E. and Berger, N. and Berghaus, F. and Beringer, J. and Bernard, C. and Bernard, N. R. and Bernius, C. and Bernlochner, F. U. and Berry, T. and Berta, P. and Bertella, C. and Bertoli, G. and Bertolucci, F. and Bertsche, C. and Bertsche, D. and Besana, M. I. and Besjes, G. J. and Bessidskaia Bylund, O. and Bessner, M. and Besson, N. and Betancourt, C. and Bethke, S. and Bevan, A. J. and Bhimji, W. and Bianchi, R. M. and Bianchini, L. and Bianco, M. and Biebel, O. and Bieniek, S. P. and Bierwagen, K. and Biglietti, M. and Bilbao De Mendizabal, J. and Bilokon, H. and Bindi, M. and Binet, S. and Bingul, A. and Bini, C. and Black, C. W. and Black, J. E. and Black, K. M. and Blackburn, D. and Blair, R. E. and Blanchard, J. -B. and Blazek, T. and Bloch, I. and Blocker, C. and Blum, W. and Blumenschein, U. and Bobbink, G. J. and Bobrovnikov, V. S. and Bocchetta, Simona and Bocci, A. and Bock, C. and Boddy, C. R. and Boehler, M. and Boek, T. T. and Bogaerts, J. A. and Bogdanchikov, A. G. and Bogouch, A. and Bohm, C. and Boisvert, V. and Bold, T. and Boldea, V. and Boldyrev, A. 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A. and Bruncko, D. and Bruneliere, R. and Brunet, S. and Bruni, A. and Bruni, G. and Bruschi, M. and Bryngemark, Lene and Buanes, T. and Buat, Q. and Bucci, F. and Buchholz, P. and Buckley, A. G. and Buda, S. I. and Budagov, I. A. and Buehrer, F. and Bugge, L. and Bugge, M. K. and Bulekov, O. and Bundock, A. C. and Burckhart, H. and Burdin, S. and Burghgrave, B. and Burke, S. and Burmeister, I. and Busato, E. and Buscher, D. and Buscher, V. and Bussey, P. and Buszello, C. P. and Butler, B. and Butler, J. M. and Butt, A. I. and Buttar, C. M. and Butterworth, J. M. and Butti, P. and Buttinger, W. and Buzatu, A. and Byszewski, M. and Cabrera Urban, S. and Caforio, D. and Cakir, O. and Calafiura, P. and Calandri, A. and Calderini, G. and Calfayan, P. and Caloba, L. P. and Calvet, D. and Calvet, S. and Camacho Toro, R. and Camarda, S. and Cameron, D. and Caminada, L. 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  issn         = {{1029-8479}},
  keywords     = {{Hadron-Hadron Scattering}},
  language     = {{eng}},
  number       = {{8}},
  publisher    = {{Springer}},
  series       = {{Journal of High Energy Physics}},
  title        = {{Search for new phenomena in events with three or more charged leptons in pp collisions at s√=8 TeV with the ATLAS detector}},
  url          = {{http://dx.doi.org/10.1007/JHEP08(2015)138}},
  doi          = {{10.1007/JHEP08(2015)138}},
  year         = {{2015}},
}