Search for flavor-changing neutral currents in top quark decays t→Hc and t→Hu in multilepton final states in proton-proton collisions at √s=13 TeV with the ATLAS detector

Flavor-changing neutral currents are not present in the Standard Model at tree level and are suppressed in loop processes by the unitarity of the Cabibbo-Kobayashi-Maskawa matrix; the corresponding rates for top quark decay processes are experimentally unobservable. Extensions of the Standard Model...

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Bibliographic Details
Published in:Physical Review D Vol. 98, № 3. P. 032002-1-032002-25
Other Authors: Aad, G., Abbott, B., Chelkov, G. A., Khodinov, A., Parida, B., Tsybychev, D., Vaniachine, A., Aaboud, M.
Format: Article
Language:English
Subjects:
Online Access:http://vital.lib.tsu.ru/vital/access/manager/Repository/vtls:000651143
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024 7 |a 10.1103/PhysRevD.98.032002  |2 doi 
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039 9 |a 201903261400  |b 100  |c 201903251714  |d VLOAD  |y 201903251635  |z Александр Эльверович Гилязов 
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245 1 0 |a Search for flavor-changing neutral currents in top quark decays t→Hc and t→Hu in multilepton final states in proton-proton collisions at √s=13 TeV with the ATLAS detector  |c M. Aaboud, G. Aad, B. Abbott [et al.] 
504 |a Библиогр.: 61 назв. 
520 3 |a Flavor-changing neutral currents are not present in the Standard Model at tree level and are suppressed in loop processes by the unitarity of the Cabibbo-Kobayashi-Maskawa matrix; the corresponding rates for top quark decay processes are experimentally unobservable. Extensions of the Standard Model can generate new flavor-changing neutral current processes, leading to signals which, if observed, would be unambiguous evidence of new interactions. A data set corresponding to an integrated luminosity of 36.1  fb-1 of pp collisions at a center-of-mass energy of s=13  TeV recorded with the ATLAS detector at the Large Hadron Collider is used to search for top quarks decaying to up or charm quarks with the emission of a Higgs boson, with subsequent Higgs boson decay to final states with at least one electron or muon. No signal is observed and limits on the branching fractions B(t→Hc)<0.16% and B(t→Hu)<0.19% at 95% confidence level are obtained (with expected limits of 0.15% in both cases). 
653 |a ATLAS, детектор 
653 |a Большой адронный коллайдер 
653 |a протон-протонные столкновения 
655 4 |a статьи в журналах  |9 879358 
700 1 |a Aad, G.  |9 116039 
700 1 |a Abbott, B.  |9 116041 
700 1 |a Chelkov, G. A.  |9 96983 
700 1 |a Khodinov, A.  |9 159187 
700 1 |a Parida, B.  |9 395729 
700 1 |a Tsybychev, D.  |9 395730 
700 1 |a Vaniachine, A.  |9 159188 
700 1 |a Aaboud, M.  |9 159186 
773 0 |t Physical Review D  |d 2018  |g Vol. 98, № 3. P. 032002-1-032002-25  |x 1550-7998 
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