Limits for Spin-Independent Cross Section of Dark Matter Particle (${{\boldsymbol X}^{0}}$) on Nucleon

Isoscalar coupling is assumed to extract the limits from those on ${{\mathit X}^{0}}$--nuclei cross section.

For ${\boldsymbol m}_{{{\boldsymbol X}^{0}}}$ = 20 GeV INSPIRE search

For limits from ${{\mathit X}^{0}}$ annihilation in the Sun, the assumed annihilation final state is shown in parenthesis in the comment.
VALUE (pb) CL% DOCUMENT ID TECN  COMMENT
• • • We do not use the following data for averages, fits, limits, etc. • • •
$<5 \times 10^{-6}$ 95 1
AGNESE
2018
CDMS ${}^{}\mathrm {Ge}$
$<2 \times 10^{-6}$ 90 2
AARTSEN
2017
ICCB ${{\mathit \nu}}$, earth
$<1 \times 10^{4}$ 90 3
ANGLOHER
2017A
CRES ${{\mathit \chi}}{{\mathit p}}$
$<1 \times 10^{-3}$ 90 4
BARBOSA-DE-SO..
2017
ICCB ${}^{}\mathrm {Na}{}^{}\mathrm {I}$
$<7.3 \times 10^{-7}$ 90
AGNES
2016
DS50 ${}^{}\mathrm {Ar}$
$<1 \times 10^{-5}$ 90 5
AGNESE
2016
CDMS ${}^{}\mathrm {Ge}$
$<2 \times 10^{-4}$ 90 6
AGUILAR-AREVA..
2016
DMIC ${}^{}\mathrm {Si}$ CCDs
$<4 \times 10^{-5}$ 90 7
ANGLOHER
2016
CRES ${}^{}\mathrm {Ca}{}^{}\mathrm {W}{}^{}\mathrm {O}_{4}$
$<2 \times 10^{-6}$ 90 8
APRILE
2016
X100 ${}^{}\mathrm {Xe}$
$<9.4 \times 10^{-8}$ 90 9
ARMENGAUD
2016
EDE3 ${}^{}\mathrm {Ge}$
$<1.0 \times 10^{-7}$ 90 10
HEHN
2016
EDE3 ${}^{}\mathrm {Ge}$
$<4 \times 10^{-6}$ 90 11
ZHAO
2016
CDEX ${}^{}\mathrm {Ge}$
$<1 \times 10^{-5}$ 90
AGNES
2015
DS50 ${}^{}\mathrm {Ar}$
$<1.5 \times 10^{-6}$ 90 12
AGNESE
2015A
CDM2 ${}^{}\mathrm {Ge}$
$<1.5 \times 10^{-7}$ 90 13
AGNESE
2015B
CDM2 ${}^{}\mathrm {Ge}$
$<2 \times 10^{-6}$ 90 14
AMOLE
2015
PICO ${}^{}\mathrm {C}_{3}{}^{}\mathrm {F}_{8}$
$<1.2 \times 10^{-5}$ 90
CHOI
2015
SKAM ${}^{}\mathrm {H}$, solar ${{\mathit \nu}}$ ( ${{\mathit b}}{{\overline{\mathit b}}}$ )
$<1.19 \times 10^{-6}$ 90
CHOI
2015
SKAM ${}^{}\mathrm {H}$, solar ${{\mathit \nu}}$ ( ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ )
$<2 \times 10^{-8}$ 90 15
XIAO
2015
PNDX ${}^{}\mathrm {Xe}$
$<2.0 \times 10^{-7}$ 90 16
AGNESE
2014
SCDM ${}^{}\mathrm {Ge}$
$<3.7 \times 10^{-5}$ 90 17
AGNESE
2014A
SCDM ${}^{}\mathrm {Ge}$
$<1 \times 10^{-9}$ 90 18
AKERIB
2014
LUX ${}^{}\mathrm {Xe}$
$<2 \times 10^{-6}$ 90 19
ANGLOHER
2014
CRES CaWO$_{4}$
$<5 \times 10^{-6}$ 90
FELIZARDO
2014
SMPL C$_{2}$ClF$_{5}$
$<8 \times 10^{-6}$ 90 20
LEE
2014A
KIMS CsI
$<2 \times 10^{-4}$ 90 21
LIU
2014A
CDEX ${}^{}\mathrm {Ge}$
$<1 \times 10^{-5}$ 90 22
YUE
2014
CDEX ${}^{}\mathrm {Ge}$
$<1.08 \times 10^{-4}$ 90 23
AARTSEN
2013
ICCB ${}^{}\mathrm {H}$, solar ${{\mathit \nu}}$ ( ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ )
$<1.5 \times 10^{-5}$ 90 24
ABE
2013B
XMAS ${}^{}\mathrm {Xe}$
$<3.1 \times 10^{-6}$ 90 25
AGNESE
2013
CDM2 ${}^{}\mathrm {Si}$
$<3.4 \times 10^{-6}$ 90 26
AGNESE
2013A
CDM2 ${}^{}\mathrm {Si}$
$<2.2 \times 10^{-6}$ 90 27
AGNESE
2013A
CDM2 ${}^{}\mathrm {Si}$
28
BERNABEI
2013A
DAMA ${}^{}\mathrm {Na}{}^{}\mathrm {I}$ modulation
$<5 \times 10^{-5}$ 90 29
LI
2013B
TEXO ${}^{}\mathrm {Ge}$
30
ZHAO
2013
CDEX ${}^{}\mathrm {Ge}$
$<1.2 \times 10^{-7}$ 90
AKIMOV
2012
ZEP3 ${}^{}\mathrm {Xe}$
31
ANGLOHER
2012
CRES CaWO$_{4}$
$<8 \times 10^{-6}$ 90 32
ANGLOHER
2012
CRES CaWO$_{4}$
$<7 \times 10^{-9}$ 90 33
APRILE
2012
X100 ${}^{}\mathrm {Xe}$
34
ARCHAMBAULT
2012
PICA ${}^{}\mathrm {F}$ (C$_{4}F_{10}$)
$<7 \times 10^{-7}$ 90 35
ARMENGAUD
2012
EDE2 ${}^{}\mathrm {Ge}$
36
BARRETO
2012
DMIC CCD
$<2 \times 10^{-6}$ 90
BEHNKE
2012
COUP CF$_{3}$I
$<7 \times 10^{-6}$ 37
FELIZARDO
2012
SMPL C$_{2}$ClF$_{5}$
$<1.5 \times 10^{-6}$ 90
KIM
2012
KIMS CsI
$<5 \times 10^{-5}$ 90 38
AALSETH
2011
CGNT ${}^{}\mathrm {Ge}$
39
AALSETH
2011A
CGNT ${}^{}\mathrm {Ge}$
$<5 \times 10^{-7}$ 90 40
AHMED
2011
CDM2 ${}^{}\mathrm {Ge}$, inelastic
$<2.7 \times 10^{-7}$ 90 41
AHMED
2011A
RVUE ${}^{}\mathrm {Ge}$
42
AHMED
2011B
CDM2 ${}^{}\mathrm {Ge}$, low threshold
$<3 \times 10^{-6}$ 90 43
ANGLE
2011
XE10 ${}^{}\mathrm {Xe}$
$<7 \times 10^{-8}$ 90 44
APRILE
2011
X100 ${}^{}\mathrm {Xe}$
45
APRILE
2011A
X100 ${}^{}\mathrm {Xe}$, inelastic
$<2 \times 10^{-8}$ 90 33
APRILE
2011B
X100 ${}^{}\mathrm {Xe}$
46
HORN
2011
ZEP3 ${}^{}\mathrm {Xe}$
$<2 \times 10^{-7}$ 90
AHMED
2010
CDM2 ${}^{}\mathrm {Ge}$
$<1 \times 10^{-5}$ 90 47
AKERIB
2010
CDM2 ${}^{}\mathrm {Si}$, ${}^{}\mathrm {Ge}$, low threshold
$<1 \times 10^{-7}$ 90
APRILE
2010
X100 ${}^{}\mathrm {Xe}$
$<2 \times 10^{-6}$ 90
ARMENGAUD
2010
EDE2 ${}^{}\mathrm {Ge}$
$<4 \times 10^{-5}$ 90
FELIZARDO
2010
SMPL C$_{2}$ClF$_{3}$
$<1.5 \times 10^{-7}$ 90 48
AHMED
2009
CDM2 ${}^{}\mathrm {Ge}$
$<2 \times 10^{-4}$ 90 49
LIN
2009
TEXO ${}^{}\mathrm {Ge}$
50
AALSETH
2008
CGNT ${}^{}\mathrm {Ge}$
1  AGNESE 2018 give limits for ${{\mathit \sigma}}{}^{SI}$( ${{\mathit p}}{{\mathit \chi}}$ ) for m(WIMP) between 1.5 and 20 GeV using CDMSlite mode data.
2  AARTSEN 2017 obtain ${\mathit \sigma (}SI{)}$ $<$ $6 \times 10^{-6}$ pb for m(wimp) = 20 GeV from ${{\mathit \nu}}$ from earth.
3  ANGLOHER 2017A find $\sigma {}^{SI}$( ${{\mathit \chi}}{{\mathit p}}$ ) $<$ $10^{4}$ pb for m(WIMP) = 0.2 GeV.
4  BARBOSA-DE-SOUZA 2017 search for annual modulation of WIMP scatter on ${}^{}\mathrm {Na}{}^{}\mathrm {I}$ using an exposure of 61 kg yr of DM-Ice17 for recoil energy in the $4 - 20$ keV range (DAMA found modulation for recoil energy $<$ 5 keV). No modulation seen. Sensitivity insufficient to distinguish DAMA signal from null.
5  AGNESE 2016 CDMSlite excludes low mass WIMPs $1.6 - 5.5$ GeV and SI scattering cross section depending on $\mathit m$(WIMP); see Fig. 4.
6  AGUILAR-AREVALO 2016 search low mass $1 - 10$ GeV WIMP scatter on ${}^{}\mathrm {Si}$ CCDs; set limits Fig. 11.
7  ANGLOHER 2016 requires SI WIMP-nucleon cross section $<$ $9 \times 10^{-3}$ pb for $\mathit m$(WIMP) = 1 GeV on ${}^{}\mathrm {Ca}{}^{}\mathrm {W}{}^{}\mathrm {O}_{4}$ target.
8  APRILE 2016 search low mass WIMP SI scatter on ${}^{}\mathrm {Xe}$; exclude ${{\mathit \sigma}}$ $>$ $1.4 \times 10^{-5}$ pb for m(WIMP) = 6 GeV.
9  ARMENGAUD 2016 require SI WIMP-${{\mathit p}}$ cross section $<$ $4.3 \times 10^{-4}$ pb for $\mathit m$(WIMP) = 5 GeV on ${}^{}\mathrm {Ge}$ target.
10  HEHN 2016 search for low mass WIMPs via SI scatter on ${}^{}\mathrm {Ge}$ target; ${{\mathit \sigma}}$(SI) $<$ $5.8 \times 10^{-4}~$pb for m(WIMP) = 5 GeV, Fig. 6.
11  ZHAO 2016 require SI scatter $<$ $4 \times 10^{-6}$ pb for $\mathit m$(WIMP) = 20 GeV using ${}^{}\mathrm {Ge}$ target; limits also on SD scatter, see Fig. 19.
12  AGNESE 2015A reanalyse AHMED 2011B low threshold data. See their Fig. 12 (left) for improved limits extending down to 5 GeV.
13  AGNESE 2015B reanalyse AHMED 2010 data.
14  See their Fig. 7 for limits extending down to 4 GeV.
15  See their Fig. 13 for limits extending down to 5 GeV.
16  This limit value is provided by the authors. See their Fig. 4 for limits extending down to ${\mathit m}_{{{\mathit X}^{0}}}$ = 3.5 GeV.
17  This limit value is provided by the authors. AGNESE 2014A result is from CDMSlite mode operation with enhanced sensitivity to low mass ${\mathit m}_{{{\mathit X}^{0}}}$. See their Fig. 3 for limits extending down to ${\mathit m}_{{{\mathit X}^{0}}}$ = 3.5 GeV (see also Fig. 4 in AGNESE 2014 ).
18  See their Fig. 5 for limits extending down to ${\mathit m}_{{{\mathit X}^{0}}}$ = 5.5 GeV.
19  See their Fig. 5 for limits extending down to ${\mathit m}_{{{\mathit X}^{0}}}$ = 1 GeV.
20  See their Fig. 5 for limits extending down to ${\mathit m}_{{{\mathit X}^{0}}}$ = 5 GeV.
21  LIU 2014A result is based on prototype CDEX-0 detector. See their Fig. 13 for limits extending down to ${\mathit m}_{{{\mathit X}^{0}}}$ = 2 GeV.
22  See their Fig. 4 for limits extending down to ${\mathit m}_{{{\mathit X}^{0}}}$ = 4.5 GeV.
23  AARTSEN 2013 search for neutrinos from the Sun arising from the pair annihilation of ${{\mathit X}^{0}}$ trapped by the sun in data taken between June 2010 and May 2011.
24  See their Fig. 8 for limits extending down to ${\mathit m}_{{{\mathit X}^{0}}}$ = 7 GeV.
25  This limit value is provided by the authors. AGNESE 2013 use data taken between Oct. 2006 and July 2007. See their Fig. 4 for limits extending down to ${\mathit m}_{{{\mathit X}^{0}}}$ = 7 GeV.
26  This limit value is provided by the authors. AGNESE 2013A use data taken between July 2007 and Sep. 2008. Three candidate events are seen. Assuming these events are real, the best fit parameters are ${\mathit m}_{{{\mathit X}^{0}}}$ = 8.6 GeV and $\sigma $ = $1.9 \times 10^{-5}$ pb.
27  This limit value is provided by the authors. Limit from combined data of AGNESE 2013 and AGNESE 2013A. See their Fig. 4 for limits extending down to ${\mathit m}_{{{\mathit X}^{0}}}$ = 5.5 GeV.
28  BERNABEI 2013A search for annual modulation of counting rate in the $2 - 6$ keV recoil energy interval, in a 14 yr live time exposure of 1.33 t yr. Find a modulation of $0.0112$ $\pm0.0012$ counts/(day kg keV) with 9.3 sigma C.L. Find period and phase in agreement with expectations from DM particles.
29  See their Fig. 4 for limits extending down to ${\mathit m}_{{{\mathit X}^{0}}}$ = 4 GeV.
30  See their Fig. 5 for limits for ${\mathit m}_{{{\mathit X}^{0}}}$ = $4 - 12$ GeV.
31  ANGLOHER 2012 observe excess events above the expected background which are consistent with ${{\mathit X}^{0}}$ with mass $\sim{}$ 25 GeV (or 12 GeV) and spin-independent ${{\mathit X}^{0}}$-nucleon cross section of $2 \times 10^{-6}$ pb (or $4 \times 10^{-5}$ pb).
32  Reanalysis of ANGLOHER 2009 data with all three nuclides. See also BROWN 2012 .
33  See also APRILE 2014A.
34  See their Fig. 7 for cross section limits for ${\mathit m}_{{{\mathit X}^{0}}}$ between 4 and 12 GeV.
35  See their Fig. 4 for limits extending down to ${\mathit m}_{{{\mathit X}^{0}}}$ = 7 GeV.
36  See their Fig. 13 for cross section limits for ${\mathit m}_{{{\mathit X}^{0}}}$ between 1.2 and 10 GeV.
37  See also DAHL 2012 for a criticism.
38  See their Fig. 4 for limits extending to ${\mathit m}_{{{\mathit X}^{0}}}$ = 3.5 GeV.
39  AALSETH 2011A find indications of annual modulation of the data, the energy spectrum being compatible with ${{\mathit X}^{0}}$ mass around 8 GeV. See also AALSETH 2013 .
40  AHMED 2011 search for ${{\mathit X}^{0}}$ inelastic scattering. See their Fig. $8 - 10$ for limits. The inelastic cross section reduces to the elastic cross section at the limit of zero mass splitting (Fig. 8, left).
41  AHMED 2011A combine CDMS II and EDELWEISS data.
42  AHMED 2011B give limits on spin-independent ${{\mathit X}^{0}}$-nucleon cross section for ${\mathit m}_{{{\mathit X}^{0}}}$ = $4 - 12$ GeV in the range $10^{-3} - 10^{-5}$ pb. See their Fig. 3.
43  See their Fig. 3 for limits down to ${\mathit m}_{{{\mathit X}^{0}}}$ = 4 GeV.
44  APRILE 2011 reanalyze APRILE 2010 data.
45  APRILE 2011A search for ${{\mathit X}^{0}}$ inelastic scattering. See their Fig. 2 and 3 for limits. See also APRILE 2014A.
46  HORN 2011 perform detector calibration by neutrons. Earlier results are only marginally affected.
47  See their Fig. 10 and 12 for limits extending to ${{\mathit X}^{0}}$ mass of 1 GeV.
48  Superseded by AHMED 2010 .
49  See their Fig. 6(a) for cross section limits for ${\mathit m}_{{{\mathit X}^{0}}}$ extending down to 2 GeV.
50  See their Fig. 2 for cross section limits for ${\mathit m}_{{{\mathit X}^{0}}}$ between 4 and 10 GeV.
  References:
AGNESE 2018
PR D97 022002 Low-Mass Dark Matter Search with CDMSlite
AARTSEN 2017
EPJ C77 82 First Search for Dark Matter Annihilations in the Earth with the IceCube Detector
ANGLOHER 2017A
EPJ C77 637 Results on MeV-scale Dark Matter from a Gram-Scale Cryogenic Calorimeter Operated above Ground
BARBOSA-DE-SOUZA 2017
PR D95 032006 First Search for a Dark Matter Annual Modulation Signal with NaI(Tl) in the Southern Hemisphere by DM-Ice17
AGNES 2016
PR D93 081101 Results from the First use of Low Radioactivity Argon in a Dark Matter Search
AGNESE 2016
PRL 116 071301 New Results from the Search for Low-Mass Weakly Interacting Massive Particles with the CDMS Low Ionization Threshold Experiment
AGUILAR-AREVALO 2016
PR D94 082006 Search for Low-Mass WIMPs in a 0.6 kg Day Exposure of the DAMIC Experiment at SNOLAB
ANGLOHER 2016
EPJ C76 25 Results on Light Dark Matter Particles with a Low-Threshold CRESST-II Detector
APRILE 2016
PR D94 092001 Low-Mass Dark Matter Search using Ionization Signals in XENON100
ARMENGAUD 2016
JCAP 1605 019 Constraints on Low-Mass WIMPs from the EDELWEISS-III Dark Matter Search
HEHN 2016
EPJ C76 548 Improved EDELWEISS-III Sensitivity for Low-Mass WIMPs using a Profile Likelihood Approach
ZHAO 2016
PR D93 092003 Search of Low-Mass WIMPs with a $\mathit p$-Type Point Contact Germanium Detector in the CDEX-1 Experiment
AGNES 2015
PL B743 456 First Results from the DarkSide-50 Dark Matter Experiment at Laboratori Nazionali del Gran Sasso
AGNESE 2015A
PR D91 052021 Maximum Likelihood Analysis of Low Energy CDMS II Germanium Data
AGNESE 2015B
PR D92 072003 Improved WIMP-Search Reach of the CDMS II Germanium Data
AMOLE 2015
PRL 114 231302 Dark Matter Search Results from the PICO-2L C$_{3}F_{8}$ Bubble Chamber
CHOI 2015
PRL 114 141301 Search for Neutrinos from Annihilation of Captured Low-Mass Dark Matter Particles in the Sun by Super-Kamiokande
XIAO 2015
PR D92 052004 Low-Mass Dark Matter Search Results from full Exposure of the PandaX-I Experiment
AGNESE 2014
PRL 112 241302 Search for Low-Mass Weakly Interacting Massive Particles with SuperCDMS
AGNESE 2014A
PRL 112 041302 CDMSlite: A Search for Low-Mass WIMPs using Voltage-Assisted Calorimetric Ionization Detection in the SuperCDMS Experiment
AKERIB 2014
PRL 112 091303 First Results from the LUX Dark Matter Experiment at the Sanford Underground Research Facility
ANGLOHER 2014
EPJ C74 3184 Results on Low Mass WIMPs using an Upgraded CRESST-II Detector
FELIZARDO 2014
PR D89 072013 The SIMPLE Phase II Dark Matter Search
LEE 2014A
PR D90 052006 Search for Low-Mass Dark Matter with CsI(Tl) Crystal Detectors
LIU 2014A
PR D90 032003 Limits on Light WIMPs with a Germanium Detector at 177 eVee (electron equivalent) Threshold at the China Jinping Underground Laboratory
YUE 2014
PR D90 091701 Limits on Light WIMPs from the CDEX-1 Experiment with a $\mathit p$-Type Point-Contact Germanium Detector at the China Jingping Underground Laboratory
AARTSEN 2013
PRL 110 131302 Search for Dark Matter Annihilations in the Sun with the 79-String IceCube Detector
ABE 2013B
PL B719 78 Light WIMP Search in XMASS
AGNESE 2013A
PRL 111 251301 Silicon Detector Dark Matter Results from the Final Exposure of CDMS II
AGNESE 2013
PR D88 031104 Silicon Detector Results from the First Five-Tower Run of CDMS II
BERNABEI 2013A
EPJ C73 2648 Final Model Independent Result of DAMA/LIBRA-Phase1
LI 2013B
PRL 110 261301 Limits on Spin-Independent Couplings of WIMP Dark Matter with a p-Type Point-Contact Germanium Detector
ZHAO 2013
PR D88 052004 First Results on Low-Mass WIMP from the CDEX-1 Experiment at the China Jinping Underground Laboratory
AKIMOV 2012
PL B709 14 WIMP-Nucleon Cross-Section Results from the Second Science Run of ZEPLIN-II
ANGLOHER 2012
EPJ C72 1971 Results from 730 kg days of the CRESST-II Dark Matter Search
APRILE 2012
PRL 109 181301 Dark Matter Results from 225 Live Days of XENON100 Data
ARCHAMBAULT 2012
PL B711 153 Constraints on Low-Mass WIMP Interactions on ${}^{19}\mathrm {F}$ from PICASSO
ARMENGAUD 2012
PR D86 051701 Search for Low-Mass WIMPs with EDELWEISS-II Heat-and-Ionization Detectors
BARRETO 2012
PL B711 264 Direct Search for Low Mass Dark Matter Particles with CCDs
BEHNKE 2012
PR D86 052001 First Dark Matter Search Results from a 4-kg CF$_{3}$I Bubble Chamber Operated in a Deep Underground Site
FELIZARDO 2012
PRL 108 201302 Final Analysis and Results of the Phase II SIMPLE Dark Matter Search
KIM 2012
PRL 108 181301 New Limits on Interactions between Weakly Interacting Massive Particles and Nucleons Obtained with CsI(Tl) Crystal Detectors
AALSETH 2011A
PRL 107 141301 Search for an Annual Modulation in a $\mathit p$-Type Point Contact Germanium Dark Matter Detector
AALSETH 2011
PRL 106 131301 Results from a Search for Light-Mass Dark Matter with a $\mathit p$-Type Point Contact Germanium Detector
AHMED 2011A
PR D84 011102 Combined Limits on WIMPs from the CDMS and EDELWEISS Experiments
AHMED 2011
PR D83 112002 Search for Inelastic Dark Matter with the CDMS II Experiment
AHMED 2011B
PRL 106 131302 Results from a Low-Energy Analysis of the CDMS II Germanium Data
ANGLE 2011
PRL 107 051301 Search for Light Dark Matter in XENON10 Data
APRILE 2011B
PRL 107 131302 Dark Matter Results from 100 Live Days of XENON100 Data
APRILE 2011
PR D84 052003 Likelihood Approach to the First Dark Matter Results from XENON100
APRILE 2011A
PR D84 061101 Implications on Inelastic Dark Matter from 100 Live Days of XENON100 Data
HORN 2011
PL B705 471 Nuclear Recoil Scintillation and Ionisation Yields in Liquid Xenon from ZEPLIN-III Data
AHMED 2010
SCI 327 1619 Dark Matter Search Results from the CDMS II Experiment
AKERIB 2010
PR D82 122004 Low-Threshold Analysis of CDMS Shallow-Site Data
APRILE 2010
PRL 105 131302 First Dark Matter Results from the XENON100 Experiment
ARMENGAUD 2010
PL B687 294 First Results of the EDELWEISS-II WIMP Search using ${}^{}\mathrm {Ge}$ Cryogenic Detectors with Interleaved Electrodes
FELIZARDO 2010
PRL 105 211301 First Results of the Phase II SIMPLE Dark Matter Search
AHMED 2009
PRL 102 011301 Search for Weakly Interacting Massive Particles with the First Five-Tower Data from the Cryogenic Dark Matter Search at the Soudan Underground Laboratory
LIN 2009
PR D79 061101 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
AALSETH 2008
PRL 101 251301 Experimental Constraints on a Dark Matter Origin for the DAMA Annual Modulation Effect
DAHL 2012
PRL 108 259001 Comments on FELIZARDO 2010 ''First Results of the Phase II SIMPLE Dark Matter Search''
ANGLOHER 2009
ASP 31 270 Commissioning Run of the CRESST-II Dark Matter Search
BROWN 2012
PR D85 021301 Extending the CRESST-II Commissioning Run Limits to Lower Masses
APRILE 2014A
ASP 54 11 Analysis of the XENON100 Dark Matter Search Data
AALSETH 2013
PR D88 012002 CoGeNT: A Search for Low-Mass Dark Matter using $\mathit p$-type Point Contact Germanium Detectors