Search for the lepton-flavor-violating decays
Bs0→τ±μ∓
and
B0→τ±μ∓
Bs0→τ±μ∓
and
B0→τ±μ∓
File(s)PhysRevLett.123.211801 (1).pdf (310.82 KB)
Published version
Author(s)
Type
Journal Article
Abstract
Results are reported from a search for the rare decays
B
0
s
→
τ
±
μ
∓
and
B
0
→
τ
±
μ
∓
, where the
τ
lepton is reconstructed in the channel
τ
−
→
π
−
π
+
π
−
ν
τ
. These processes are effectively forbidden in the standard model, but they can potentially occur at detectable rates in models of new physics that can induce lepton-flavor-violating decays. The search is based on a data sample corresponding to
3
fb
−
1
of proton-proton collisions recorded by the LHCb experiment in 2011 and 2012. The event yields observed in the signal regions for both processes are consistent with the expected standard model backgrounds. Because of the limited mass resolution arising from the undetected
τ
neutrino, the
B
0
s
and
B
0
signal regions are highly overlapping. Assuming no contribution from
B
0
→
τ
±
μ
∓
, the upper limit
B
(
B
0
s
→
τ
±
μ
∓
)
<
4.2
×
10
−
5
is obtained at 95% confidence level. If no contribution from
B
0
s
→
τ
±
μ
∓
is assumed, a limit of
B
(
B
0
→
τ
±
μ
∓
)
<
1.4
×
10
−
5
is obtained at 95% confidence level. These results represent the first limit on
B
(
B
0
s
→
τ
±
μ
∓
)
and the most stringent limit on
B
(
B
0
→
τ
±
μ
∓
)
.
B
0
s
→
τ
±
μ
∓
and
B
0
→
τ
±
μ
∓
, where the
τ
lepton is reconstructed in the channel
τ
−
→
π
−
π
+
π
−
ν
τ
. These processes are effectively forbidden in the standard model, but they can potentially occur at detectable rates in models of new physics that can induce lepton-flavor-violating decays. The search is based on a data sample corresponding to
3
fb
−
1
of proton-proton collisions recorded by the LHCb experiment in 2011 and 2012. The event yields observed in the signal regions for both processes are consistent with the expected standard model backgrounds. Because of the limited mass resolution arising from the undetected
τ
neutrino, the
B
0
s
and
B
0
signal regions are highly overlapping. Assuming no contribution from
B
0
→
τ
±
μ
∓
, the upper limit
B
(
B
0
s
→
τ
±
μ
∓
)
<
4.2
×
10
−
5
is obtained at 95% confidence level. If no contribution from
B
0
s
→
τ
±
μ
∓
is assumed, a limit of
B
(
B
0
→
τ
±
μ
∓
)
<
1.4
×
10
−
5
is obtained at 95% confidence level. These results represent the first limit on
B
(
B
0
s
→
τ
±
μ
∓
)
and the most stringent limit on
B
(
B
0
→
τ
±
μ
∓
)
.
Date Issued
2019-11-22
Date Acceptance
2019-11-01
Citation
Physical Review Letters, 2019, 123 (21), pp.211801-1-211801-11
ISSN
0031-9007
Publisher
American Physical Society (APS)
Start Page
211801-1
End Page
211801-11
Journal / Book Title
Physical Review Letters
Volume
123
Issue
21
Copyright Statement
© 2019 CERN, for the LHCb Collaboration. Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license (https://creativecommons.org/licenses/by/4.0/). Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI. Funded by SCOAP3.
Identifier
http://dx.doi.org/10.1103/PhysRevLett.123.211801
http://arxiv.org/abs/1905.06614v2
Subjects
hep-ex
hep-ex
General Physics
01 Mathematical Sciences
02 Physical Sciences
09 Engineering
Notes
15 pages, 5 figures. All figures and tables, along with any supplementary material and additional information, are available at https://cern.ch/lhcbproject/Publications/p/LHCb-PAPER-2019-016.html
Publication Status
Published
Article Number
211801
Date Publish Online
2019-11-22