Search for Higgs bosons decaying to aa in the μμττ final state in pp collisions at √s = 8  TeV with the ATLAS experiment

A search for the decay to a pair of new particles of either the 125 GeV Higgs boson (h) or a second charge parity (CP)-even Higgs boson (H) is presented. The data set corresponds to an integrated luminosity of 20.3  fb[superscript −1] of pp collisions at √s = 8  TeV recorded by the ATLAS experiment...

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Bibliographic Details
Main Author: Taylor, Frank E. (Contributor)
Other Authors: Massachusetts Institute of Technology. Department of Physics (Contributor)
Format: Article
Language:English
Published: American Physical Society, 2016-02-05T01:42:01Z.
Subjects:
Online Access:Get fulltext
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042 |a dc 
100 1 0 |a Taylor, Frank E.  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Physics  |e contributor 
100 1 0 |a Taylor, Frank E.  |e contributor 
245 0 0 |a Search for Higgs bosons decaying to aa in the μμττ final state in pp collisions at √s = 8  TeV with the ATLAS experiment 
260 |b American Physical Society,   |c 2016-02-05T01:42:01Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/101103 
520 |a A search for the decay to a pair of new particles of either the 125 GeV Higgs boson (h) or a second charge parity (CP)-even Higgs boson (H) is presented. The data set corresponds to an integrated luminosity of 20.3  fb[superscript −1] of pp collisions at √s = 8  TeV recorded by the ATLAS experiment at the LHC in 2012. The search was done in the context of the next-to-minimal supersymmetric standard model, in which the new particles are the lightest neutral pseudoscalar Higgs bosons (a). One of the two a bosons is required to decay to two muons while the other is required to decay to two τ leptons. No significant excess is observed above the expected backgrounds in the dimuon invariant mass range from 3.7 to 50 GeV. Upper limits are placed on the production of h → aa relative to the standard model gg → h production, assuming no coupling of the a boson to quarks. The most stringent limit is placed at 3.5% for m[subscript a] = 3.75  GeV. Upper limits are also placed on the production cross section of H → aa from 2.33 to 0.72 pb, for fixed m[subscript a] = 5  GeV with mH ranging from 100 to 500 GeV. 
520 |a United States. Dept. of Energy 
520 |a National Science Foundation (U.S.) 
520 |a Brookhaven National Laboratory 
546 |a en_US 
655 7 |a Article 
773 |t Physical Review D