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Introduction to dark matter experiments
Cosmology and Nongalactic Astrophysics · Submitted 27 Jan 2011
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Experiments are already probing SUSY models, with best limits on the spin-independent coupling below 10^-7 pb.
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The abstract, sentence by sentence
This is a set of four lectures presented at the Theoretical Advanced Study Institute (TASI-09) in June 2009. I provide an introduction to experiments designed to detect WIMP dark matter directly, focusing on building intuitive understanding of the characteristics of potential WIMP signals and the experimental techniques. After deriving the characteristics of potential signals in direct-detection experiments for standard WIMP models, I summarize the general experimental methods shared by most direct-detection experiments and review the advantages, challenges, and status of such searches (as of late 2009). Experiments are already probing SUSY models, with best limits on the spin-independent coupling below 10^-7 pb.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | This is a set of four lectures presented at the Theoretical Advanced Study Institute (TASI-09) in June 2009. | background 0.89 | 0.35 | 0.01 | asserted 1.00 |
| s1 | I provide an introduction to experiments designed to detect WIMP dark matter directly, focusing on building intuitive understanding of the characteristics of potential WIMP signals and the experimental techniques. | contribution 0.99 | 0.45 | 0.06 | asserted 0.88 |
| s2 | After deriving the characteristics of potential signals in direct-detection experiments for standard WIMP models, I summarize the general experimental methods shared by most direct-detection experiments and review the advantages, challenges, and status of such searches (as of late 2009). | contribution 0.87 | 0.57 | 0.14 | asserted 0.92 |
| s3 | Experiments are already probing SUSY models, with best limits on the spin-independent coupling below 10^-7 pb. | background 0.60 | 0.10 | 0.18 | asserted 1.00 |
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The paper
Original abstract
This is a set of four lectures presented at the Theoretical Advanced Study Institute (TASI-09) in June 2009. I provide an introduction to experiments designed to detect WIMP dark matter directly, focusing on building intuitive understanding of the characteristics of potential WIMP signals and the experimental techniques. After deriving the characteristics of potential signals in direct-detection experiments for standard WIMP models, I summarize the general experimental methods shared by most direct-detection experiments and review the advantages, challenges, and status of such searches (as of late 2009). Experiments are already probing SUSY models, with best limits on the spin-independent coupling below 10^-7 pb.
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References
How the literature uses it
28 arXiv papers cite this in 42 sentences
Papers citing it · 21 sentences without a confident label
Uses its method or tool 2 papers
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We broadly follow the description in Refs. [ref] in order to compute the expected event rate for dark matter scattering in our detectors as well as the recoil energy spectrum.
Passive low-energy nuclear recoil detection with color centers · Dark matter detection · 1.00
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Our first approach involves considering a canonical WIMP and astrophysical scenario, and applying a standard analysis based on time-independent rates [ref] : i) assuming that all of the background is time-independent and caused by electron recoils, ii) estimating how much of the background leaks into the nuclear recoil region of our detectors and iii) determining how the leakage would limit the sensitivity of these detectors to nuclear recoils from a WIMP.
Sensitivity of alkali halide scintillating calorimeters with particle identification to investigate the DAMA dark matter detection claim · Time-independent sensitivity limited by background leakage into signal region · 0.86
Uses its data or values 1 paper
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To evaluate the spin-dependent cross section we use for $^19$F the proton-coupling $⟨S_p⟩=0.477$ [ref] , for $^7$Li we use $⟨S_p⟩=0.497$ [ref] and we set $⟨S_n ⟩≃0$ for both isotopes.
Passive low-energy nuclear recoil detection with color centers · Dark matter detection · 0.90
Cites it as background 13 papers
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A scintillating calorimeter is a particle detector consisting of a scintillating crystal held at cryogenic temperatures ($≲$ 50 mK) as the target medium, read-out by a light detector and thermal sensors, such that, for a given particle interaction, both scintillation and phonon signals can be observed [ref] .
Sensitivity of alkali halide scintillating calorimeters with particle identification to investigate the DAMA dark matter detection claim · Introduction · 0.80
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Assuming that the DM consists of composite T-baryons (mostly, T-neutrons with probably a small fraction of anti-T-neutrons), let us discuss extra possible constraints on the vector-like TC parameter space coming from astrophysical observations and cosmological evolution of the DM (for a review on the current (in)direct DM detection measurements and constraints, see e.g. Refs. [ref] ).
Vector-like technineutron Dark Matter: is a QCD-type Technicolor ruled out by XENON100? · Annihilation of T-baryons in cosmological plasma · 1.00
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Liquid noble elements (LNE) have been established as an attractive detection medium in experiments searching for dark matter or neutrino-less double-beta decay: a large number of existing or planned experiments employ liquid xenon, argon, or neon [ref] .
NEST: A Comprehensive Model for Scintillation Yield in Liquid Xenon · Introduction and Motivations · 0.96
What it cites · 53 sentences without a confident label
Uses data or values from 11 papers
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The TEXONO collaboration has achieved an energy threshold of 220 eVee in four 5 g detectors [ref] , while the CoGeNT collaboration achieved nearly as low a threshold for a run of 8.4 kg days exposure [ref] .
New limits on spin-independent and spin-dependent couplings of low-mass WIMP dark matter with a germanium detector at a threshold of 220 eV · Cryogenic Detectors · 0.85
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As shown in Figure [ref], the DEAP-1 experiment has already demonstrated better than $10^7$:1 rejection of backgrounds [ref] , and an analytic model predicts better than billion-to-one rejection with 90% efficiency for WIMPs.
Measurement of the scintillation time spectra and pulse-shape discrimination of low-energy beta and nuclear recoils in liquid argon with DEAP-1 · Noble Liquid Detectors · 0.87
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In the blindly chosen energy region, 2–12 keVee (corresponding to 4.5–27 keV$_R$ for the assumed nuclear quenching factor, but to a higher energy range for more recent measurements [ref] ), 10 presumed background events passed cuts (see Fig. [ref]), with studies after unblinding suggesting that most were multiple-scatter events with one interaction below the cathode.
Scintillation efficiency and ionization yield of liquid xenon for mono-energetic nuclear recoils down to 4 keV · Noble Liquid Detectors · 0.86
Cites as support 2 papers
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No suggested background process appears likely to yield modulation as large as the observed signal [ref] .
Dark Matter search · DAMA · 0.97
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If the LHC determines the WIMP mass, direct detection can determine WIMP-nucleon cross section much better than LHC alone [ref] .
Determination of Dark Matter Properties at High-Energy Colliders · Implications of a detection · 0.96
Cites as background 6 papers
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Whatever physics solves the hierarchy problem associated with this symmetry breaking – be it supersymmetry [ref] , extra dimensions [ref] , or something else – gives rise to additional particles.
Kaluza-Klein Dark Matter: Direct Detection vis-a-vis LHC · Introduction · 0.86
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Whatever physics solves the hierarchy problem associated with this symmetry breaking – be it supersymmetry [ref] , extra dimensions [ref] , or something else – gives rise to additional particles.
Is the Lightest Kaluza-Klein Particle a Viable Dark Matter Candidate? · Introduction · 0.86
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Whatever physics solves the hierarchy problem associated with this symmetry breaking – be it supersymmetry [ref] , extra dimensions [ref] , or something else – gives rise to additional particles.
Kaluza-Klein Dark Matter · Introduction · 0.86
Discussion
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