CYGNUS HD10
A low-mass dark matter search with directional sensitivity via charge cloud tomography
Sven Vahsen (University of Hawaii) for the U.S. and U.K. CYGNUS Collaborators
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CYGNUS HD10 A low-mass dark matter search with directional - - PowerPoint PPT Presentation
CYGNUS HD10 A low-mass dark matter search with directional sensitivity via charge cloud tomography Sven Vahsen (University of Hawaii) for the U.S. and U.K. CYGNUS Collaborators 3/23/17 U.S. Cosmic Visions: New Ideas in Dark Matter 1 The
Sven Vahsen (University of Hawaii) for the U.S. and U.K. CYGNUS Collaborators
3/23/17 U.S. Cosmic Visions: New Ideas in Dark Matter 1
directional dark matter detection formed a new international proto-collaboration: CYGNUS
Italy, Spain, China
https://indico.phys.hawaii.edu/categoryDisplay. py?categId=34
CYGNUS workshop on directional dark matter detection, held since 2007.
http://www.tir.tw/conf/cygnus2017/
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The dark matter wind is expected to come from the constellation Cygnus.
nuclear recoil detector capable
directional oscillation (ó Dipole in galactic coordinates)
and physics
directional Dark Matter detection, Physics Reports 627 (2016)
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CYGNUS but most costly and challenging
Source Absent Cf-252 Source Present
27-sigma evidence for “neutron wind” in Hawaii! Recoils point back to source, in 3D.
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Cf-252
for penetrating the neutrino floor, though advantage here is smaller
not include energy dependence of detector performance (such as angular resolution, efficiency, head/tail reconstruction).
collaboration working on a comprehensive technology
CYGNUS HD10…
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Readout strategies for directional dark matter detection beyond the neutrino background Ciaran A. J. O'Hare, Anne M. Green, Julien Billard, Enectali Figueroa-Feliciano, Louis E. Strigari
mode) operation to low pressure operation for (improved) directional confirmation of WIMP signal
µm pitch) for improved
discrimination to lower energies through Helium target
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WIMP
E E
recoil (track) ionization SF6:4He gas gas vessel neutron + gamma shielding central cathode
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better than LZ / PICO-60 projections (not shown)
threshold (see later slide)
with improved directionality in low-pressure mode (~0.1 atm)
3/23/17 U.S. Cosmic Visions: New Ideas in Dark Matter 8 1 10 100 1000 10000 WIMP Mass (GeV/c2) WIMP−proton SD cross section (pb) 10−8 10−7 10−6 10−5 10−4 10−3 10−2 10−1 1 10 102 103 104 105 106 107
DAMA Allowed NAIAD (2005) ZEPLIN−III (2009) DMTPC (2010) COUPP (2012) PICASSO (2012) KIMS (2012) DRIFT (2012) XENON100 (2013) SIMPLE (2014) DRIFT (2015) NEWAGE (2015) LUX (2016) PICO−2L (2016) PICO−60 (2016) DRIFT (2016) CYGNUS 200 Torr SF6, 3 yrs, 10 m^3, 10 keVee CYGNUS 200 Torr SF6, 3 yrs, 10 m^3, 1 keVee
Highly preliminary - likely to change
due to He target
detectors, but with electron event discrimination
with improved directionality in low-pressure mode (~0.1 atm)
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Highly preliminary - likely to change
achievable gain, readout segmentation→capacitance → noise floor, and diffusion/drift length
threshold
gain, S/N, readout dimensionality, segmentation, drift length, gas density, target nucleus)
discrimination threshold
]
2
WIMP mass [GeV/c 1 10 [pb]
SD N
σ
10
10
10 1 10
> 30 eVee, no direc.
thresF recoil - E > 1 keVee
thresF recoil - E > 5 keVee
thresF recoil - E > 10 keVee
thresF recoil - E
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]
2
WIMP mass [GeV/c 1 10 [pb]
SI N
σ
10
10
10
10
10
10
> 30 eVe, no direc. thres He recoil - E > 1 keVee thres He recoil - E > 5 keVee thres He recoil - E > 10 keVee thres He recoil - E > 30 eVe, no direc. thres F recoil - E > 1 keVee thres F recoil - E > 5 keVee thres F recoil - E > 10 keVee thres F recoil - E > 30 eVe, no direc. thres S recoil - E > 1 keVee thres S recoil - E > 5 keVee thres S recoil - E > 10 keVee thres S recoil - E10 torr of SF6 + 50 torr of He 1 event detected 1000 days exposure 1 m3 60cm drift length track length / sigma(drift distance) > 3
Highly preliminary - likely to change
Each of these thresholds is lowest with 3D charge readout --- pixels or strips.
capacitance à lower noise à lower charge threshold
efficiency at gain > 20k
events à lower discrimination threshold
à Best compromise
x/y strips (available from CERN
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𝛽 – particle neutron Charge density Charge density
density, measured w/ 2x2 cm ATLAS pixel chip readout
Raw data – no noise hits! HeC02 gas,p=1 atm
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CS2-CF4-O2 All BG removed!
Discovery of Multiple, Ionization-Created Anions in Gas Mixtures Containing CS2 and O2 Daniel P . Snowden-Ifft http://arxiv.org/abs/1308.0354
has gain, and is a good SD target (!)
profile (not width) of track, enables accurate measurement of transverse diffusion, which depends on drift length à obtain absolute position in drift direction
P.Lewis
extended by grad student to also work with recoil events (unpublished)
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10-5 around 10 keVee
via negative ion drift)
but longer recoils)
àmore than half the detector volume should have excellent electron discrimination at ~5 keVee and below.
beyond range-energy signature.
3/23/17 U.S. Cosmic Visions: New Ideas in Dark Matter 14 GEM-based TPC with CCD imaging for directional dark matter detection N.S. Phan, et. al., roparticle Physics, 84 (2016)
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( ”weak priors” corner of priorhedron – see talk by N. Weiner this morning) BEAST micro TPC – 3D neutron recoils Experimental data Each box is 50μm x 250 μm x250 μm Color = charge density
(DRIFT, DMTPC) or under construction (NEWAGE, MIMAC)
10 scale-up, but aims for drastically enhanced performance
have already been experimentally demonstrated by CYGNUS collaboration members, but individually
with the proposed gas mixture.
5 keVee energies via 3d readout and He recoils needs experimental demonstration
– prototypes exist
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dedicated cavern
(infrastructure, manpower for operations)
get the rock and cosmogenic neutron background at Boulbydown to < 0.5 events
depends on readout discrimination power and radio-purity
manpower)
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Underground at Boulby
for CYGNUS 2017 conference in June
utilized to measure coherent neutrino scattering at a neutrino source (COHERENT)
neutrino community (NOvA)
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charge readout (most powerful option) of large volumes at reasonable cost
a single detector, with improved electron rejection expected at low masses
SD or (low-mass) SI - with further improvements in sensitivity
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With source present Without source present Detector is essentially background free for high-energy neutron recoil events. From cathode mesh. Rejected by position cut
extended to nuclear recoil by student
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at < 1m3 scale:
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