Search for long-lived particles decaying to $$e ^\pm $$ e ± $$\mu ^\mp $$ μ ∓ $$\nu $$ ν
Name
10052_2021_Article_8994.pdf
Size
1.87 MB
Format
Adobe PDF
Checksum (MD5)
f720c28f39879bfeea5888a851e4711c
Author(s) • • • • • • • • •
Aaij, R.
Beteta, C. A
Ackernley, T.
Adeva, B.
Adinolfi, M.
Afsharnia, H.
Aidala, C. A
Aiola, S.
Ajaltouni, Z.
Akar, S.
Date Issued
March 26, 2021
Publisher
Springer Berlin Heidelberg
Citation
The European Physical Journal C. 2021 Mar 26;81(3):261
Version
Final published version
Abstract
Abstract
Long-lived particles decaying to
$${e ^\pm } {\mu ^\mp } {\nu } $$
e
±
μ
∓
ν
, with masses between 7 and
$$50 \,\text {GeV/}c^2 $$
50
GeV/
c
2
and lifetimes between 2 and
$$50 \,\text {ps} $$
50
ps
, are searched for by looking at displaced vertices containing electrons and muons of opposite charges. The search is performed using
$$5.4 \,\text {fb} ^{-1} $$
5.4
fb
-
1
of
$$p $$
p
$$p $$
p
collisions collected with the LHCb detector at a centre-of-mass energy of
$$\sqrt{s} = 13 \,\text {TeV} $$
s
=
13
TeV
. Three mechanisms of production of long-lived particles are considered: the direct pair production from quark interactions, the pair production from the decay of a Standard-Model-like Higgs boson with a mass of
$$125 \,\text {GeV/}c^2 $$
125
GeV/
c
2
, and the charged current production from an on-shell
$$W $$
W
boson with an additional lepton. No evidence of these long-lived states is obtained and upper limits on the production cross-section times branching fraction are set on the different production modes.
MIT Department
Massachusetts Institute of Technology. Department of Physics
Terms of Use
Creative Commons Attribution
Persistent DSpace Link
DOI of Published Version
https://doi.org/10.1140/epjc/s10052-021-08994-0