Search for heavy Majorana neutrinos in e(+/-)e(+/-)+ jets and e(+/-) mu(+/-)+jetseventsinproton-protoncollisionsat root s=8TeV
File(s)10.1007%2FJHEP04(2016)169.pdf (722.26 KB)
Published version
Author(s)
Type
Journal Article
Abstract
A search is performed for heavy Majorana neutrinos (N) decaying into a W
boson and a lepton using the CMS detector at the Large Hadron Collider. A signature of
two jets and either two same sign electrons or a same sign electron-muon pair is searched for
using 19.7 fb−1 of data collected during 2012 in proton-proton collisions at a centre-of-mass
energy of 8 TeV. The data are found to be consistent with the expected standard model
(SM) background and, in the context of a Type-1 seesaw mechanism, upper limits are set
on the cross section times branching fraction for production of heavy Majorana neutrinos
in the mass range between 40 and 500 GeV. The results are additionally interpreted as
limits on the mixing between the heavy Majorana neutrinos and the SM neutrinos. In
the mass range considered, the upper limits range between 0.00015–0.72 for |VeN|
2 and
6.6×10−5–0.47 for |VeNV
∗
µN
|
2/(|VeN|
2 +|VµN
|
2
), where V`N
is the mixing element describing
the mixing of the heavy neutrino with the SM neutrino of flavour `. These limits are the
most restrictive direct limits for heavy Majorana neutrino masses above 200 GeV.
boson and a lepton using the CMS detector at the Large Hadron Collider. A signature of
two jets and either two same sign electrons or a same sign electron-muon pair is searched for
using 19.7 fb−1 of data collected during 2012 in proton-proton collisions at a centre-of-mass
energy of 8 TeV. The data are found to be consistent with the expected standard model
(SM) background and, in the context of a Type-1 seesaw mechanism, upper limits are set
on the cross section times branching fraction for production of heavy Majorana neutrinos
in the mass range between 40 and 500 GeV. The results are additionally interpreted as
limits on the mixing between the heavy Majorana neutrinos and the SM neutrinos. In
the mass range considered, the upper limits range between 0.00015–0.72 for |VeN|
2 and
6.6×10−5–0.47 for |VeNV
∗
µN
|
2/(|VeN|
2 +|VµN
|
2
), where V`N
is the mixing element describing
the mixing of the heavy neutrino with the SM neutrino of flavour `. These limits are the
most restrictive direct limits for heavy Majorana neutrino masses above 200 GeV.
Date Issued
2016-04-27
Date Acceptance
2016-04-12
Citation
Journal of High Energy Physics, 2016, 2016 (4)
ISSN
1029-8479
Publisher
Springer Verlag (Germany)
Journal / Book Title
Journal of High Energy Physics
Volume
2016
Issue
4
Copyright Statement
Open Access, Copyright CERN,
for the benefit of the CMS Collaboration.
Article funded by SCOAP3
for the benefit of the CMS Collaboration.
Article funded by SCOAP3
License URL
Subjects
Science & Technology
Physical Sciences
Physics, Particles & Fields
Physics
Beyond Standard Model
Hadron-Hadron scattering (experiments)
LEPTON NUMBER
MASSES
VIOLATION
DECAYS
MIXINGS
MODELS
Publication Status
Published
Article Number
169