Physics Letters B 732 (2014) 373–379
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Physics Letters B
www.elsevier.com/locate/physletb
Light dark matter for Fermi-LAT and CDMS observations
Bumseok Kyae
a
,Jong-ChulPark
b,∗
a
Department of Physics, Pusan National University, Busan 609-735, Republic of Korea
b
Department of Physics, Sungkyunkwan University, Suwon 440-746, Republic of Korea
article info abstract
Article history:
Received 15 October 2013
Received in revised form 27 March 2014
Accepted 1 April 2014
Available online 4 April 2014
Editor: G.F. Giudice
Keywords:
Light dark matter
Fermi-LAT
Gamma-ray
CDMS
CoGeNT
Light fermionic/scalar dark matter (DM) (m
DM
≈ 8 GeV) neutral under the standard model can be
responsible for the CDMS and CoGeNT signals, and the Fermi-LAT gamma-ray excesses. In order to
explain them in a relatively simple framework, we have explored various DM annihilation and scattering
processes, discussing important phenomenological constraints coming from particle physics. Assuming
that the two independent observations have a common DM origin and the processes arise through a
common mediator, DM should annihilate into tau/anti-tau lepton pairs through an s-channel, and scatter
with nuclei through a t-channel process. To avoid the p-wave suppression, a new Higgs-like scalar field
with a mass of
O(1) TeV is necessary as a common mediator of both the processes. We propose a
supersymmetric model realizing the scenario.
© 2014 The Authors. Published by Elsevier B.V. This is an open access article under the CC BY license
(http://creativecommons.org/licenses/by/3.0/). Funded by SCOAP
3
.
1. Introduction
Dark matter (DM) is one of the most important building blocks
constituting the universe [1]. According to the recent precise ob-
servation from the Planck satellite experiment, it is believed that
DM occupies 27 percent of the present energy density of the uni-
verse [2]. In particular, weakly interacting massive particle (WIMP),
which is the most promising DM candidate, is essential for under-
standing the physics law at the electroweak (EW) scale as well as
the structure formation in the universe. Thus, various experiments
to explore DM are being carried out on the earth and also outside
the atmosphere.
Recently, DM direct detection experiments such as CoGeNT [3],
CDMS-Ge [4] and
CDMS-Si [5] have reported the observations of
some WIMP-candidate events at (2–3)
σ confidence level. They are
claimed to be interpreted as DM signals with a relatively light
mass of m
DM
≈ 7–10 GeV and a spin-independent (SI) elastic scat-
tering cross section per nucleon of
σ
SI
≈ 10
−41
–10
−40
cm
2
.The
best fit point for these three measurements is around m
DM
≈
8 GeV and σ
SI
≈ 3 ×10
−41
cm
2
. DAMA/LIBRA [6] and CRESST-II [7]
results also support similar parameter regions. However, all such
signals are not exactly compatible with the constraints from
XENON10 [8] and XENON100 [9]. Recently, the authors of Ref. [10]
have pointed out that XENON10’s constraint should be weakened,
*
Corresponding author.
E-mail addresses: bky
ae@pusan.ac.kr (B. Kyae), log1079@gmail.com (J.-C. Park).
and the XENON10 Collaboration has corrected the old result in
the erratum to Ref. [8]. In addition, the author of Ref. [11] has
studied various uncertainties and assumptions, which could af-
fect XENON100’s constraint on light DM. Very recently, CoGeNT
released the updated data, confirming their previous light DM sig-
nals [12]. Under such a tension among the observations, we will
particularly focus on the positive results of CDMS and CoGeNT in
this paper.
1
If DM annihilates into the standard model (SM) chiral fermions,
it should also emit gamma-rays. Fermi Large Area Telescope
(Fermi-LAT) [17] is a satellite based experiment measuring cos-
mic gamma-rays. The recent analyses [18] based on the data
from Fermi-LAT show peaks at energies around 1–10 GeV in the
gamma-ray spectrum coming from around the galactic center. It
could be interpreted as an evidence of DM annihilation into the
leptons l
¯
l with m
DM
≈ 7–12 GeV or the bottom quarks bb with
m
DM
≈ 25–45 GeV. In this case, the required annihilation cross
section is
σ v ∼ 10
−26
cm
3
/s.
2
1
Right after completion of this work, LUX [13] reported more stringent limit,
constraining all the positive signal regions. In light of LUX, light DM possibilities
have been examined in various ways in Refs. [14–16].
2
The current limits on the annihilation of light DM into leptons coming from the
cosmic microwave background (CMB) are
σ v
e
e
≈ 0.5–1 ×10
−26
cm
3
/s, σ v
μμ
≈
1–2 × 10
−26
cm
3
/s, and σ v
τ τ
≈ 2–3 × 10
−26
cm
3
/s [19].Thus,thecaseofDM
annihilations into e
−
e
+
, μ
−
μ
+
, τ
−
τ
+
with the same ratio is slightly constrained
by the CMB bound. However, if DM mainly annihilates only into
τ
−
τ
+
,theCMB
constraint could be easily avoidable.
http://dx.doi.org/10.1016/j.physletb.2014.04.003
0370-2693/
© 2014 The Authors. Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/3.0/). Funded by
SCOAP
3
.