Transcript Indirect Dark Matter Search with Antideuterons: Progress

Antideuterons as an Indirect Dark Matter
Signature: Design and Preparation
for a Balloon-born GAPS Experiment
Jason Koglin
Columbia Astrophysics Laboratory
For the GAPS Collaboration
The General Antiparticle Spectrometer (GAPS) exploits low energy antideuterons
produced in neutralino-neutralino annihilations as an indirect dark matter (DM)
signature that is effectively free from background. When an antiparticle is captured
by a target material, it forms an exotic atom in an excited state which quickly
decays by emitting X-rays of precisely defined energy and a correlated pion
signature from nuclear annihilation. We have successfully demonstrated the GAPS
method in an accelerator environment and are currently planning a prototype flight
from Japan for 2009. This will lead to a long duration balloon (LDB) mission that
will complement existing and planned direct DM searches as well as other indirect
techniques, probing a different, and often unique, region of parameter space in a
variety of proposed DM models. Planes of coarsely pixilated Si(Li) detectors form
the heart of GAPS flight detector, providing both high X-ray resolution and good
particle tracking. We will describe the proto-flight mission that will verify the
performance of our Si(Li) detectors and cooling system in a flight-like configuration.
We also will outline the LDB science payload design.
Funding provided through NASA APRA grants NAG5-5393 & NNG06WC06G
Jason Koglin – TAUP – September 11, 2007
1
Antideuterons as an Indirect Dark Matter
Signature: Design and Preparation
for a Balloon-born GAPS Experiment
T. Aramaki, C.J. Hailey, J.E. Koglin, N. Madden, K. Mori,
H.T. Yu – Columbia University
S.E. Boggs – University of California, Berkeley
W.W. Craig – Lawrence Livermore National Laboratory
H. Fuke, T. Yoshida – Institute of Space & Astronautical
Science, Japan Aerospace Exploration Agency
F. Gahbauer – University of Latvia
R.A. Ong – University of California, Los Angeles
ORNL K.P. Ziock – Oak Ridge National Laboratory
Jason Koglin – TAUP – September 11, 2007
2
Low energy, neutralino-neutralino produced
antideuterons are near background free
Significant antideuteron flux at the
earth (with propagation & solar
modulation) first pointed out by
Donato et al. 2000
• Primary component:
 neutralino annihilation
10-3
• Secondary component:
 spallation
__
p+H → p+H+D+…
__
p+He → p+He+D+…
Antideuteron Flux [m2 s-1 sr-1 GeV-1]
BESS limit
10-4
10-5
GAPS
LDB
LZP (m = 40 GeV)
LSP (m = 100 GeV)
LKP (m = 500 GeV)
Secondary/Tertiary
ULDB
• GAPS represents a major
improvement over the state
of the art
10-8
10-9
10-10
0.1
Signal: Baer & Profumo ’05
Back: Duperray et al. ‘05
1
10
Kinetic Energy per Nucleon [GeV/n]
Jason Koglin – TAUP – September 11, 2007
X+X → D + …
• GAPS is essentially a
background free experiment
10-6
10-7
__
100
• GAPS has outstanding
discovery potential for a
variety of DM models
3
SUSY discovery potential for an antideuteron
experiment is similar to direct detection methods
There are over 20 current or planned direct
detection experiments to probe SUSY DM
A balloon GAPS antideuteron search offers
SUSY parameter space complementarity to
direct detection, underground searches
LDB
ULDB
Exploratory
Discovery
From Baer & Profumo 2005
100

SI
P
/ CDMS-II (Dev. Z BG) sensitivity
Direct
10
Both
1
0.1
0.01
0.001
GAPS
0.0001
0.001
0.01
0.1
1
10
100
Antideuteron flux / GAPS (ULD balloon) sensitivity
Jason Koglin – TAUP – September 11, 2007
1000
Note: DM theory has an
approximate symmetry:
N(experiments) ≈ N(theories)
ANAIS
ArDM
CDMSII
CUORICINO
COSME
CRESST
DAMA
DMRC
DRIFT
ELEGANT V
EDELWEISS
EURECA
GEDEON
GENIUS
Genino
GERDA
HDMS
IGEX
LIBRA
NAIAD
PICASSO
SIMPLE
SuperCDMS
SuperK
WARP
XENON
ZEPLIN
4th generation heavy neutrino
Axinos
Axions
Bino
Brane world DM
CHAMPS
Cryptons
D-matter
Gravitinos
Kaluza-Klein
Higgsino
Light scalars
Minimal DM
Mirror particles
Neutralinos
New symmetry little Higgs
Q-balls
Photino
Self-interacting DM
Simpzillas
SM neutrinos
Sneutrinos
Sterile neutrinos
SWIMPS
Theory space little Higgs
Wimpzillas
Wino
4
p*
_
D
GAPS is based on radiative emission of
antiparticles captured into exotic atoms
Atomic Transitions
Plastic Scintillator TOF
Si(Li) Target/Detector
Auger e-
no,lo
Refilling e-
p*
n=nK~15
44 keV
n=6
g
n=5
g
n=4
g
n=3
n=2
30 keV
p*
p*
A time of flight (TOF) system tags
candidate events and records velocity
The antiparticle slows down & stops in
a target material, forming an excited
exotic atom with near unity probability
Deexcitation X-rays provide signature
Pions from annihilation provide added
background suppression
Jason Koglin – TAUP – September 11, 2007
p+
 1
1 
2
Eg  zZ M*RH  2 - 2 
ni 
 nf
n=1
p+
p-
po
Ladder
Deexcitations
Dn=1, Dl=1
p-
Nuclear
Annihilation
Antiprotonic yields
measured at KEK
in 2004 & 2005
in various targets.
5
Si(Li) Wafers will be hexagonally packed into detector
planes & surrounded by segmented Plastic TOF
~200 kg Si(Li) mass – Similar to direct detection target mass
Jason Koglin – TAUP – September 11, 2007
6
GAPS employs three techniques to uniquely identify
antideuterons with enormous background suppression
1. Atomic X-rays
2. TOF and Depth Sensing
3. Charged Pion Multiplicity
Expected Background
for a 300 Day Flight
Exploratory
Type of
Background
Expected
Events
Temporally
incoherent X-rays
< 0.003
Temporally
coherent X-rays
Elastic neutrons
Secondarytertiaryatmospheric
antideuterons
Nuclear g-rays, po
shower photons,
internal
bremastrahlung
Scaling from γray telescopes
0.001
Measured at
GAPS-KEK
experiment
0.002
Monte-Carlo of
evaporative &
cascade model,
KEK limits
0.006
Propagate
calculated spectra
through
atmosphere to
instrument
Data on energy &
branching ratio of
negligible all possible lines;
analytic calc.;
GEANT4 sim.
Exploration trigger 0.2 (total)
Jason Koglin – TAUP – September 11, 2007
Basis for
estimate
Analytic & MonteCarlo Simulations
7
Si(Li) Serves a Target for Stopping Antideuterons
as well as an X-ray Detector & Particle Tracker
• Relatively low Z provides:
• Modular approach for ease
 good compromise between
of in-field assembly
X-ray escape and detection
 Low internal background.
• Excellent timing (50 ns) & energy
resolution (2 keV – much better
than NaI, but modest for Si)
 2 X-ray coincidence sufficient
(previous designs used 3 X-rays)
• Relatively course pixels (8 cm2)
 Keeps channel count low but
still provides for low pileup.
• Dual channel electronics
(5-200 keV & 0.1-200 MeV)
 Good charged particle tracking
for depth sensing & annihilation
product tracking
• Proven technology dating to 60’s
Jason Koglin – TAUP – September 11, 2007
8
A Prototype Flight will Provide a Crucial
Science & Engineering Demonstration
Balloon Prototype Goals:
•
•
•
Demonstrate stable, low noise
operation of the Si(Li) with its
polymer coating at float
altitude & ambient pressure.
Demonstrate the Si(Li) cooling
approach & deployable sun
shades. Verify thermal model.
Measure incoherent
background level in a flightlike configuration.
2009 Flight planned from Japan
with ISIS/JAXA participation
Jason Koglin – TAUP – September 11, 2007
9
GAPS Development Plan Culminates in a
Long-Duration Balloon (LDB) Experiment
2003
2004
KEK04
2005
KEK05
2006
2007
2008
Flight Instrument Design
Si(Li) Proto
Measurements
Data Analysis &
Background Studies
2009
Facility Design
pGAPS
Construction
• Flight of GAPS prototype from Japan
in 2009
• Long Duration Balloon (LDB) GAPS
flight from Antarctica in 2013
• Experiment design will be Ultra Long
Duration (ULDB) capable to exploit
such a launch if it becomes
available; flight duration >100 days
Jason Koglin – TAUP – September 11, 2007
2010
2011
Facility
Construction
Japan
Proto-Flight
2012
2013
bGAPS
Construction
Antarctic Science
Flight
NASA/ULDB
10
Primary GAPS Science Goals
Antideuteron Dark
Matter Signature
Primordial Black Holes
Low-Energy Antiproton
Spectroscopy
From Barrau et al. 2003
From Baer & Profumo 2005
•
•
Execute deep searches
for SUSY & UED DM
Complementary with
direct and other
indirect measurements
Jason Koglin – TAUP – September 11, 2007
•
•
Measure antideuterons
from evaporating PBH’s
Potentially constrain
inflation temperature
•
•
Measure 104-105
antiprotons <0.3 GeV
(BESS-polar measured
26 @ <0.3 GeV)
Perform both DM and
cosmic-ray physics
11
Jason Koglin – TAUP – September 11, 2007
12
We have tested a prototype detector that exceeds our
requirements – fabrication scale-up challenge remains
4” wafer
8 cm2
pixel
~400 wafers/layer
13 layers
Heat Dissipation & Power Load
Heat Dissipation per Si(Li) channel
130
Total Heat Dissipation
400
Jason Koglin – TAUP – September 11, 2007
1622
Power for Plastic Detector System
186
Other power requirements
200
Total Power
Mass Breakdown
Design based on tested 4” prototype
Si(Li) detector. We are studying 5”6” detectors to ease implementation.
0.005
Solar and other heat
Power for Si(Li) Detector System
126 cm
[W]
2008
[kg]
Si(Li) Detectors
204
Si(Li) Electronics, Cables, Support &
Cooling
315
Plastic Scintillator
151
PMT, Light-guide, Cables, Electronics,
Wrapping Support
190
Gondola, Computers, Telemetry Power,
Radiator,
376
Total
1237
13