Physics Letters B 767 (2017) 209–213
Contents lists available at ScienceDirect
Physics Letters B
www.elsevier.com/locate/physletb
Dirac neutrinos and dark matter stability from lepton quarticity
Salvador Centelles Chuliá
a
, Ernest Ma
b
, Rahul Srivastava
a,c,∗
, José W.F. Valle
a
a
AHEP Group, Instituto de Física Corpuscular – C.S.I.C./Universitat de València, Edificio de Institutos de Paterna, C/Catedratico José Beltrán, 2 E-46980 Paterna
(València) -Spain
b
Physics Department, University of California, Riverside, CA 92521, USA
c
Physical Research Laboratory, Navrangpura, Ahmedabad - 380 009, India
a r t i c l e i n f o a b s t r a c t
Article history:
Received
14 November 2016
Received
in revised form 13 January 2017
Accepted
30 January 2017
Available
online 2 February 2017
Editor: A.
Ringwald
We propose to relate dark matter stability to the possible Dirac nature of neutrinos. The idea is illustrated
in a simple scheme where small Dirac neutrino masses arise from a type-I seesaw mechanism as a result
of a Z
4
discrete lepton number symmetry. The latter implies the existence of a viable WIMP dark matter
candidate, whose stability arises from the same symmetry which ensures the Diracness of neutrinos.
© 2017 The Authors. 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
.
Amongst the major shortcomings of the Standard Model are the
neutrino mass and the dark matter problems. Underpinning the
origin of neutrino mass and elucidating the nature of dark mat-
ter
would constitute a gigantic step forward in particle physics.
Here we focus on the possibility that the neutrino mass and dark
matter problems may be closely interconnected [1,2]. Concerning
neutrino mass a major unknown is whether neutrinos are their
own anti-particles, an issue which has remained an open challenge
ever since Ettore Majorana’s pioneer idea on the quantum mechan-
ics
of spin. On the other hand, since many years physicists have
pondered about what is the dark matter made of, and what makes
it stable, a property usually assumed in an ad-hoc fashion.
1
Indeed,
although the existence of non-baryonic dark matter is well estab-
lished
by using cosmological and astrophysical probes, its nature
has otherwise remained elusive [5].
The
detection of neutrinoless double beta decay would be a
major step in particle physics since, according to the black-box the-
orem [6,7] it
would not only demonstrate that lepton number is
violated in nature, but also imply that neutrinos are of Majorana
type. On the other hand, the fact that the weak interaction is V-A
turns this quest into a major challenge [8,9]. As of now the nature
of neutrinos remains as mysterious as the mechanism responsible
for generating their small masses. Little is known regarding the
nature of its associated messenger particles, the underlying mass
*
Corresponding author.
E-mail
addresses: salcen@alumni.uv.es (S. Centelles Chuliá), ma@phyun8.ucr.edu
(E. Ma),
rahulsri@ific.uv.es (R. Srivastava), valle@ific.uv.es (J.W.F. Valle).
1
Attempts at stabilizing dark matter by using the Z
2
and Z
3
symmetries have
already been considered in the literature [3,4].
scale or its flavor structure [10], currently probed only in neutrino
oscillation experiments [11]. Here we assume that neutrinos are
Dirac particles. Realizing this possibility requires extra assumptions
beyond the standard SU(3)
c
⊗SU(2)
L
⊗U(1)
Y
electroweak gauge
invariance. One approach is to extend the gauge group itself, for
example, by using the SU(3)
c
⊗SU(3)
L
⊗U(1)
X
gauge structure due
to its special features [12]. In this framework it has recently been
shown how to obtain a type-II seesaw mechanism for Dirac neutri-
nos [13,14].
Using unconventional lepton charges for right handed
neutrinos [15] and gauging B − L can also lead to Dirac neutrinos
within the type-I seesaw mechanism [4,16,17]. Alternatively, one
may stick to the SU(3)
c
⊗ SU(2)
L
⊗ U(1)
Y
gauge structure but use
extra flavor symmetries implying a conserved lepton number, so as
to obtain Dirac neutrinos, as suggested in [18].
In
this letter we focus on having neutrinos as Dirac particles as
a result of the cyclic symmetry Z
4
, which plays the role of a dis-
crete
version of lepton number, we call quarticity.
2
We show that
a WIMP dark matter candidate can naturally emerge, stabilized by
quarticity, the same symmetry associated to the Diracness of neu-
trinos.
Our
model is based on the discrete symmetry Z
4
⊗Z
2
where Z
4
is the cyclic group of order four and Z
2
is the cyclic group of or-
der
two. As we show here, Z
4
symmetry not only forbids Majorana
terms but also forbids couplings of potential dark matter candi-
date
ensuring stability. Thus, the same symmetry which implies
the
Dirac nature of neutrinos also ensures the stability of dark
matter. The Z
2
symmetry is required here to ensure the seesaw
2
It is not inconceivable that such symmetry could arise from anomaly-free dis-
crete
gauge symmetries [19].
http://dx.doi.org/10.1016/j.physletb.2017.01.070
0370-2693/
© 2017 The Authors. 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
.