Physics Letters B 760 (2016) 486–493
Contents lists available at ScienceDirect
Physics Letters B
www.elsevier.com/locate/physletb
Diphoton excess from hidden U(1) gauge symmetry with large kinetic
mixing
Fuminobu Takahashi
a,b
, Masaki Yamada
a
, Norimi Yokozaki
a,∗
a
Department of Physics, Tohoku University, Sendai, Miyagi 980-8578, Japan
b
Kavli IPMU (WPI), UTIAS, The University of Tokyo, Kashiwa, Chiba 277-8583, Japan
a r t i c l e i n f o a b s t r a c t
Article history:
Received
28 April 2016
Received
in revised form 5 July 2016
Accepted
6 July 2016
Available
online 9 July 2016
Editor:
J. Hisano
We show that the 750 GeV diphoton excess can be explained by introducing vector-like quarks and
hidden fermions charged under a hidden U(1) gauge symmetry, which has a relatively large coupling
constant as well as a significant kinetic mixing with U(1)
Y
. With the large kinetic mixing, the standard
model gauge couplings unify around 10
17
GeV, suggesting the grand unified theory without too rapid
proton decay. Our scenario predicts events with a photon and missing transverse momentum, and its
cross section is related to that for the diphoton excess through the kinetic mixing. We also discuss
other possible collider signatures and cosmology, including various ways to evade constraints on exotic
stable charged particles. In some cases where the 750 GeV diphoton excess is due to diaxion decays, our
scenario also predicts triphoton and tetraphoton signals.
© 2016 The Author(s). Published by Elsevier B.V. This is an open access article under the CC BY license
(http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP
3
.
1. Introduction
The diphoton excess with an invariant mass around 750 GeV
was
recently reported by the ATLAS [1] and CMS [2] collaborations;
for a spin-0 particle with a narrow width approximation, the local
significance is estimated to be 3.9σ and 2.9σ , respectively. While
more data is certainly needed to confirm if the signal is real or
just a statistical fluke, its high statistical significance in the clean
analysis using photons triggered enthusiasm and exuberance for
the new physics beyond the standard model (SM), followed by the
appearance of many theoretical papers.
Among
various models proposed so far, the simplest one is
to include a gauge singlet (pseudo)scalar coupled to vector-like
quarks and/or leptons (see e.g. Refs. [3–5] for the early works).
1
In this model, the (pseudo)scalar is produced via gluon fusion and
decays into a pair of photons through one-loop diagrams with the
extra quarks/leptons running in the loop. The diphoton excess can
be explained if the product of the production cross section times
branching ratio to two photons is in the range of 5–10 fb. This
gives a preference to a relatively large branching fraction to dipho-
*
Corresponding author.
E-mail
address: yokozaki@truth.phys.tohoku.ac.jp (N. Yokozaki).
1
It is still a puzzle why such a (pseudo)scalar coupled to gluons and photons
exists in nature. One possible answer is to relate it to the QCD axion (or its bosonic
partner, saxion) which solves the strong CP problem [6–9].
tons, which necessitates either multiple extra matter fields and/or
large hypercharges (Y 1) of the extra field running in the loop.
In
this paper we consider a possibility that the large hyper-
charges
are originated from unbroken hidden U(1)
H
gauge symme-
try
which has a relatively strong gauge coupling and a significant
kinetic mixing with U(1)
Y
. Then, hidden fermions acquire large
hypercharges due to the kinetic mixing, and the induced hyper-
charges
are generically irrational. We will show that the diphoton
excess can be explained by the (pseudo)scalar coupled to gluons
and photons though the extra quark/hidden fermion loop dia-
grams.
Our
scenario is based on a rather simple U(1)
H
extension of
the standard model, which enables us to make a definite predic-
tion
that can be tested soon at the LHC Run-2. Since the hidden
fermions are charged under U(1)
H
, the (pseudo)scalar responsible
for the diphoton excess can also decay into γγ
, where γ
denotes
the hidden photon. Thus, our scenario predicts events with a pho-
ton
and missing momentum,
2
and we will see that its production
cross section times branching fraction is simply related to that for
the diphoton excess through the kinetic mixing. The events with a
photon and missing momentum have been searched for at the LHC
Run-1 [11,12] and Run-2 [13], and there is an upper bound on the
2
See Ref. [10] for a related work.
http://dx.doi.org/10.1016/j.physletb.2016.07.013
0370-2693/
© 2016 The Author(s). Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/). Funded by
SCOAP
3
.