If the excess events from the CoGeNT experiment arise from elastic scatterings of a light dark matter off the nuclei, crossing symmetry implies non-vanishing annihilation cross-sections of the light dark matter into hadronic final states inside the galactic halo, which we confront with the anti-proton spectrum measured by the PAMELA collaboration. We consider two types of effective interactions between the dark matter and the quarks: 1) contact interactions from integrating out heavy particles and 2) long-range interactions due to the electromagnetic properties of the dark matter. The lack of excess in the anti-proton spectrum results in tensions for a scalar and, to a less extent, a vector dark matter interacting with the quarks through the Higgs portal.
Deep Dive into When CoGeNT met PAMELA.
If the excess events from the CoGeNT experiment arise from elastic scatterings of a light dark matter off the nuclei, crossing symmetry implies non-vanishing annihilation cross-sections of the light dark matter into hadronic final states inside the galactic halo, which we confront with the anti-proton spectrum measured by the PAMELA collaboration. We consider two types of effective interactions between the dark matter and the quarks: 1) contact interactions from integrating out heavy particles and 2) long-range interactions due to the electromagnetic properties of the dark matter. The lack of excess in the anti-proton spectrum results in tensions for a scalar and, to a less extent, a vector dark matter interacting with the quarks through the Higgs portal.
arXiv:1010.1774v2 [hep-ph] 22 Dec 2010
When CoGeNT met PAMELA
Wai-Yee Keung a, Ian Low b,c, Gabe Shaughnessy b,c
a Department of Physics, University of Illinois, Chicago, IL 60607
bHigh Energy Physics Division, Argonne National Laboratory, Argonne, IL 60439
cDepartment of Physics and Astronomy, Northwestern University, Evanston, IL 60208
Abstract
If the excess events from the CoGeNT experiment arise from elastic scatterings of a light dark
matter offthe nuclei, crossing symmetry implies non-vanishing annihilation cross-sections of the
light dark matter into hadronic final states inside the galactic halo, which we confront with the
anti-proton spectrum measured by the PAMELA collaboration. We consider two types of effective
interactions between the dark matter and the quarks: 1) contact interactions from integrating out
heavy particles and 2) long-range interactions due to the electromagnetic properties of the dark
matter. The lack of excess in the anti-proton spectrum results in tensions for a scalar and, to a
less extent, a vector dark matter interacting with the quarks through the Higgs portal.
1
I.
INTRODUCTION
In recent years we have witnessed a plethora of experimental anomalies in both direct
and indirect detection experiments in search of the dark matter (DM). For example, the
direct detection experiment DAMA [1] observed signals of annual modulations consistent
with that expected from dark matter scattering offthe nuclei, while the CDMS collaboration
announced two candidate events for detection of dark matter [2]. More recently, the CoGeNT
experiment [3] released results containing signal events suggestive of a light dark matter in
the range of 7 – 12 GeV. On the other hand, several collaborations in indirect detections
reported excessive fluxes of electrons/positrons and photons, such as the PAMELA [4], the
ATIC [5], the Fermi LAT [6], the HESS [7], and the WMAP [8], which may not be explained
away easily by conventional astrophysical sources.
In order to understand whether these experimental excesses are indeed the prelude to a
discovery of the dark matter, it is crucial to cross-check dark matter interpretations of these
empirical anomalies against one another. One possibility is to construct a unified theory
explaining all these signal events [9]. Another is to confront the events with constraints from
measurements which do not see any excess, one example of which is the anti-proton spectrum
measured also by the PAMELA [10]. While this has been generally been studied for Dirac
DM with a contact interaction [11] and specifically for 10 GeV DM [12], In this work we
propose to study the consistency of the CoGeNT signals with the anti-proton spectrum of
PAMELA within the context of generic effective interactions between DM and quarks.
If the signal events in various direct detection experiments are due to elastic scatterings of
the dark matter offthe nuclei, which arise from the dark matter interaction with the quarks,
then crossing symmetry implies the same interactions must also give rise to annihilations of
dark matter into quarks. This argument has been used to constrain the boost factor [13]
necessary to explain the electron/positron excess in the PAMELA, using the updated limits
from the CDMS [11]. Another example studied the implication of various direct detection
bounds on the anti-deuteron flux from hadronic annihilations of the dark matter [14].
Theoretically, the light ( 7 – 12 GeV) dark matter interpretation of the CoGeNT offers
a unique opportunity for a model-independent study. Since such a mass scale is far below
the electroweak scale, it seems reasonable to assume that any degrees of freedom mediating
the dark matter interactions with the standard model particles have masses much heavier
2
than that of the dark matter.1 Hence at energy scales relevant for the elastic scattering
of dark matter with the nucleons and the dark matter annihilations into quarks, these
“mediator particles” can be integrated out and the interactions could be approximated by
higher dimensional operators.
The resulting effective interactions can be either contact
interactions, when the mediator particle interacts with the quarks, or long range in nature,
when the mediator particle interacts with the photon.
By combining the PAMELA anti-proton spectrum and the putative CoGeNT signal, we
find that contact interactions of a scalar or vector dark matter, arising from a heavy mediator
particle with Yukawa-like interactions with quarks, is the most severely constrained. These
constraints apply to models with a light scalar dark matter which interacts with the standard
model through the Higgs portal [16]. Cases of fermionic dark matter with an electromagnetic
charge form factor coupling or magnetic moment coupling also exhibit tension with these
data, but to a lesser degree. Previous studies on properties of the dark matter using higher
dimensional contact interactions can be found in Refs. [17, 18].
This work is organized as f
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