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Search for flavour-changing neutral current top quark decays t -> Hq in pp collisions at root s=8 TeV with the ATLAS detector

Aad, G. ; Abbott, B. ; Abdallah, J. ; Abdinov, O. ; Aben, R. ; Abolins, M. ; AbouZeid, O. S. ; Abramowicz, H. ; Abreu, H. and Abreu, R. , et al. (2015) In Journal of High Energy Physics
Abstract
A search for flavour-changing neutral current decays of a top quark to an up-type quark (q = u; c) and the Standard Model Higgs boson, where the Higgs boson decays to b (b) over bar, is presented. The analysis searches for top quark pair events in which one top quark decays to W b, with the W boson decaying leptonically, and the other top quark decays to Hq. The search is based on pp collisions at root s = 8TeV recorded in 2012 with the ATLAS detector at the CERN Large Hadron Collider and uses an integrated luminosity of 20.3 fb(-1). Data are analysed in the lepton-plus-jets final state, characterised by an isolated electron or muon and at least four jets. The search exploits the high multiplicity of b quark jets characteristic of signal... (More)
A search for flavour-changing neutral current decays of a top quark to an up-type quark (q = u; c) and the Standard Model Higgs boson, where the Higgs boson decays to b (b) over bar, is presented. The analysis searches for top quark pair events in which one top quark decays to W b, with the W boson decaying leptonically, and the other top quark decays to Hq. The search is based on pp collisions at root s = 8TeV recorded in 2012 with the ATLAS detector at the CERN Large Hadron Collider and uses an integrated luminosity of 20.3 fb(-1). Data are analysed in the lepton-plus-jets final state, characterised by an isolated electron or muon and at least four jets. The search exploits the high multiplicity of b quark jets characteristic of signal events, and employs a likelihood discriminant that uses the kinematic differences between the signal and the background, which is dominated by t (t) over bar -> WbWb decays. No significant excess of events above the background expectation is found, and observed (expected) 95% CL upper limits of 0.56% (0.42%) and 0.61% (0.64%) are derived for the t -> Hc and t -> Hu branching ratios respectively. The combination of this search with other ATLAS searches in the H -> gamma gamma and H -> WW*, tau tau decay modes significantly improves the sensitivity, yielding observed (expected) 95% CL upper limits on the t -> Hc and t -> Hu branching ratios of 0.46% (0.25%) and 0.45% (0.29%) respectively. The corresponding combined observed (expected) upper limits on the vertical bar lambda(tcH)vertical bar and vertical bar lambda(tuH)vertical bar couplings are 0.13 (0.10) and 0.13 (0.10) respectively. These are the most restrictive direct bounds on t q H interactions measured so far. (Less)
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; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; and (Less)
organization
publishing date
type
Contribution to journal
publication status
published
subject
keywords
Hadron-Hadron Scattering, Top Physics, Higgs Physics, FCNC Interactions
in
Journal of High Energy Physics
issue
12
article number
061
publisher
Springer
external identifiers
  • wos:000366831600001
  • scopus:84950323417
ISSN
1029-8479
DOI
10.1007/JHEP12(2015)061
language
English
LU publication?
yes
id
51fc6aec-eff5-4bdc-a9c7-27d06c37919a (old id 8542848)
date added to LUP
2016-04-01 10:36:59
date last changed
2023-01-10 01:22:50
@article{51fc6aec-eff5-4bdc-a9c7-27d06c37919a,
  abstract     = {{A search for flavour-changing neutral current decays of a top quark to an up-type quark (q = u; c) and the Standard Model Higgs boson, where the Higgs boson decays to b (b) over bar, is presented. The analysis searches for top quark pair events in which one top quark decays to W b, with the W boson decaying leptonically, and the other top quark decays to Hq. The search is based on pp collisions at root s = 8TeV recorded in 2012 with the ATLAS detector at the CERN Large Hadron Collider and uses an integrated luminosity of 20.3 fb(-1). Data are analysed in the lepton-plus-jets final state, characterised by an isolated electron or muon and at least four jets. The search exploits the high multiplicity of b quark jets characteristic of signal events, and employs a likelihood discriminant that uses the kinematic differences between the signal and the background, which is dominated by t (t) over bar -> WbWb decays. No significant excess of events above the background expectation is found, and observed (expected) 95% CL upper limits of 0.56% (0.42%) and 0.61% (0.64%) are derived for the t -> Hc and t -> Hu branching ratios respectively. The combination of this search with other ATLAS searches in the H -> gamma gamma and H -> WW*, tau tau decay modes significantly improves the sensitivity, yielding observed (expected) 95% CL upper limits on the t -> Hc and t -> Hu branching ratios of 0.46% (0.25%) and 0.45% (0.29%) respectively. The corresponding combined observed (expected) upper limits on the vertical bar lambda(tcH)vertical bar and vertical bar lambda(tuH)vertical bar couplings are 0.13 (0.10) and 0.13 (0.10) respectively. These are the most restrictive direct bounds on t q H interactions measured so far.}},
  author       = {{Aad, G. and Abbott, B. and Abdallah, J. and Abdinov, O. and Aben, R. 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 Affolder, A. A. and Agatonovic-Jovin, T. and Agricola, J. and Aguilar-Saavedra, J. A. and Ahlen, S. P. and Ahmadov, F. and Aielli, G. and Akerstedt, H. and Åkesson, Torsten and Akimov, A. V. and Alberghi, G. L. and Albert, J. and Albrand, S. and Verzini, M. J. Alconada and Aleksa, M. and Aleksandrov, I. N. and Alexa, C. and Alexander, G. and Alexopoulos, T. and Alhroob, M. and Alimonti, G. and Alio, L. and Alison, J. and Alkire, S. P. and Allbrooke, B. M. M. and Allport, P. P. and Aloisio, A. and Alonso, A. and Alonso, F. and Alpigiani, C. and Altheimer, A. and Gonzalez, B. Alvarez and Piqueras, D. Alvarez and Alviggi, M. G. and Amadio, B. T. and Amako, K. and Coutinho, Y. Amaral and Amelung, C. and Amidei, D. and Dos Santos, S. P. Amor 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 Anders, J. K. and Anderson, K. J. and Andreazza, A. and Andrei, V. 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 Bella, L. Aperio 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 Arnold, H. and Arratia, M. and Arslan, O. and Artamonov, A. and Artoni, G. and Asai, S. and Asbah, N. and Ashkenazi, A. and Asman, B. and Asquith, L. and Assamagan, K. and Astalos, R. and Atkinson, M. and Atlay, N. B. and Augsten, K. and Aurousseau, M. and Avolio, G. and Axen, B. and Ayoub, M. K. and Azuelos, G. and Baak, M. A. and Baas, A. E. and Baca, M. J. and Bacci, C. and Bachacou, H. and Bachas, K. and Backes, M. and Backhaus, M. and Bagiacchi, P. and Bagnaia, P. and Bai, Y. and Bain, T. and Baines, J. T. and Baker, O. K. and Baldin, E. M. and Balek, P. and Balestri, T. and Balli, F. and Balunas, W. K. and Banas, E. and Banerjee, S. W. and Bannoura, A. A. E. and Barak, L. 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 da Costa, J. Barreiro Guimaraes and Bartoldus, R. and Barton, A. E. and Bartos, P. and Basalaev, A. and Bassalat, A. and Basye, A. and Bates, R. L. and Batista, S. J. and Batley, J. R. and Battaglia, M. and Bauce, 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, M. and Beckingham, M. and Becot, C. and Beddall, A. J. and Beddall, A. and Bednyakov, V. A. and Bee, C. P. and Beemster, L. J. and Beermann, T. A. and Begel, M. and Behr, J. K. and Belanger-Champagne, C. 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 Bender, M. and Bendtz, K. and Benekos, N. and Benhammou, Y. and Noccioli, E. Benhar and Garcia, J. A. Benitez and Benjamin, D. P. and Bensinger, J. R. and Bentvelsen, S. and Beresford, L. and Beretta, M. and Berge, D. and Kuutmann, E. Bergeaas 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. 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S. and Bomben, M. and Bona, M. and Boonekamp, M. and Borisov, A. and Borissov, G. and Borroni, S. and Bortfeldt, J. and Bortolotto, V. and Bos, K. and Boscherini, D. and Bosman, M. and Boudreau, J. and Bouffard, J. and Bouhova-Thacker, E. V. and Boumediene, D. and Bourdarios, C. and Bousson, N. and Boutle, S. K. and Boveia, A. and Boyd, J. and Boyko, I. R. and Bozic, I. and Bracinik, J. and Brandt, A. and Brandt, G. and Brandt, O. and Bratzler, U. and Brau, B. and Brau, J. E. and Braun, H. M. and Madden, W. D. Breaden and Brendlinger, K. and Brennan, A. J. and Brenner, L. and Brenner, R. and Bressler, S. and Bristow, T. M. and Britton, D. and Britzger, D. and Brochu, F. M. and Brock, I. and Brock, R. and Bronner, J. and Brooijmans, G. and Brooks, T. and Brooks, W. K. and Brosamer, J. and Brost, E. and de Renstrom, P. A. Bruckman and Bruncko, D. and Bruneliere, R. and Bruni, A. and Bruni, G. and Bruschi, M. and Bruscino, N. and Bryngemark, Lene and Buanes, T. and Buat, Q. and Buchholz, P. and Buckley, A. G. and Budagov, I. A. and Buehrer, F. and Bugge, L. and Bugge, M. K. and Bulekov, O. and Bullock, D. and Burckhart, H. and Burdin, S. and Burgard, C. D. and Burghgrave, B. and Burke, S. and Burmeister, I. and Busato, E. and Buscher, D. and Buscher, V. and Bussey, P. 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 Buzykaev, A. R. and Urban, S. Cabrera and Caforio, D. and Cairo, V. M. and Cakir, O. and Calace, N. and Calafiura, P. and Calandri, A. and Calderini, G. and Calfayan, P. and Caloba, L. P. and Calvet, D. and Calvet, S. and Toro, R. Camacho and Camarda, S. and Camarri, P. and Cameron, D. and Armadans, R. Caminal and Campana, S. and Campanelli, M. and Campoverde, A. and Canale, V. and Canepa, A. and Bret, M. 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  issn         = {{1029-8479}},
  keywords     = {{Hadron-Hadron Scattering; Top Physics; Higgs Physics; FCNC Interactions}},
  language     = {{eng}},
  number       = {{12}},
  publisher    = {{Springer}},
  series       = {{Journal of High Energy Physics}},
  title        = {{Search for flavour-changing neutral current top quark decays t -> Hq in pp collisions at root s=8 TeV with the ATLAS detector}},
  url          = {{http://dx.doi.org/10.1007/JHEP12(2015)061}},
  doi          = {{10.1007/JHEP12(2015)061}},
  year         = {{2015}},
}