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

For ${\mathit m}_{{{\mathit X}^{0}}}$ in GeV range

INSPIRE   JSON  (beta) PDGID:
S030DI5
We provide here limits fo ${\mathit m}_{{{\mathit X}^{0}}}$ $<$ 5 GeV
S030DI5
VALUE (pb) CL% DOCUMENT ID TECN  COMMENT
• • We do not use the following data for averages, fits, limits, etc. • •
$<5000$ 90 1
AALBERS
2025A
 
LZ cosmic ray boosted DM
2
ADAMS
2025
 
PICO fermionic DM absorption
$<2.5 \times 10^{-9}$ 90 3
APRILE
2025
 
XENT light DM search
$<2 \times 10^{-3}$ 90 4
APRILE
2025A
 
XENT light DM search
$<4 \times 10^{4}$ 90 5
BUI
2025
 
TESS light DM search
$<1.1 \times 10^{-7}$ 90 6
ZHANG
2025B
 
PNDX wimp search
$<3 \times 10^{3}$ 90 7
ANGLOHER
2024
 
CRES light WIMP via diamond
$<1 \times 10^{4}$ 90 8
ANGLOHER
2024B
 
CRES low mass DM search
$<3 \times 10^{-3}$ 90 9
AALBERS
2023A
 
LZ SI scatter on ${}^{}\mathrm {Xe}$
$<4 \times 10^{-7}$ 90 10
AGNES
2023
 
DS50 LDM search via Migdal
$<6 \times 10^{-7}$ 90 11
AGNES
2023B
 
DS50 LDM scatter on nucleons
$<0.5$ 90 12
ALBAKRY
2023
 
SCDM LDM via Migdal
$<1$ 95 13
AMBROSONE
2023
 
DM distortion of CR spectra
$<70$ 90 14
ANGLOHER
2023
 
CRES LDM search
$<8 \times 10^{-8}$ 90 15
LI
2023F
 
PNDX SI light DM limits
$<5 \times 10^{-10}$ 90 16
MA
2023A
 
PNDX LDM search
$<10$ 90 17
ADHIKARI
2022B
 
C100 sub-GeV WIMP via SI coupling/Migdal effect
$<1.4 \times 10^{4}$ 90 18
ARMENGAUD
2022
 
EDEL GeV-scale DM on ${}^{}\mathrm {Ge}$ via Migdal effect
$<5 \times 10^{5}$ 90 19
CUI
2022
 
PNDX sub-GeV boosted DM
$<6.5 \times 10^{6}$ 90 20
XU
2022
 
CDEX sub-GeV DM
$<2 \times 10^{-7}$ 95 21
AKERIB
2021A
 
LUX low mass WIMPs
$<5 \times 10^{6}$ 90 22
ALKHATIB
2021
 
SCDM light DM
$<1 \times 10^{8}$ 95 23
ANDRIAMIRADO
2021A
 
sub-GeV DM on nucleon
$<1 \times 10^{-8}$ 90 24
APRILE
2021
 
XE1T GeV scale DM
$<8 \times 10^{-4}$ 90 25
AGUILAR-AREVA..
2020C
 
DMIC WIMP SI scatter on ${}^{}\mathrm {Si}$
$<8 \times 10^{-4}$ 90 26
AKERIB
2020A
 
LUX GeV-scale WIMP search
$<0.01$ 90 27
ABDELHAMEED
2019A
 
CRES ${}^{}\mathrm {CaWO}_{4}$
$<5.4 \times 10^{-6}$ 90 28
AGNESE
2019A
 
SCDM GeV-scale WIMPs on ${}^{}\mathrm {Ge}$
$<1$ 90 29
AKERIB
2019
 
LUX light DM on ${}^{}\mathrm {Xe}$ via Migdal/brem effect
$<1 \times 10^{-6}$ 90 30
AMOLE
2019
 
PICO ${}^{}\mathrm {C}_{3}{}^{}\mathrm {F}_{8}$
$<1.6 \times 10^{-3}$ 90 31
APRILE
2019C
 
XE1T DM on ${}^{}\mathrm {Xe}$
$<1 \times 10^{-7}$ 90 32
APRILE
2019D
 
XE1T DM on ${}^{}\mathrm {Xe}$
$<0.1$ 90 33
ARMENGAUD
2019
 
EDEL GeV-scale WIMPs on ${}^{}\mathrm {Ge}$
$<1.6 \times 10^{3}$ 90 34
KOBAYASHI
2019
 
XMAS annual modulation ${}^{}\mathrm {Xe}$
$<700$ 90 35
LIU
2019B
 
CDEX ${}^{}\mathrm {Ge}$; sub-GeV DM via Migdal
$<7 \times 10^{-7}$ 90 36
AGNES
2018
 
DS50 GeV-scale WIMPs on ${}^{}\mathrm {Ar}$
$<1.5 \times 10^{-5}$ 95 37
AGNESE
2018
 
SCDM GeV-scale WIMPs on ${}^{}\mathrm {Ge}$
$<2 \times 10^{-8}$ 90 38
APRILE
2018
 
XE1T ${}^{}\mathrm {Xe}$, SI
$<4.5 \times 10^{-3}$ 90 39
ARNAUD
2018
 
NEWS low mass WIMP, ${}^{}\mathrm {Ne}$
$<8 \times 10^{-6}$ 90 40
JIANG
2018
 
CDEX GeV-scale WIMPs on ${}^{}\mathrm {Ge}$
$<3 \times 10^{-5}$ 90 41
YANG
2018
 
CDEX WIMPs on ${}^{}\mathrm {Ge}$
$<1 \times 10^{-6}$ 90 42
AKERIB
2017
 
LUX ${}^{}\mathrm {Xe}$
$<100$ 90 43
ANGLOHER
2017A
 
CRES GeV-scale WIMPs
$<7 \times 10^{-5}$ 90 44
ANGLOHER
2016
 
CRES ${}^{}\mathrm {CaWO}_{4}$
$<3 \times 10^{-5}$ 90 45
APRILE
2016
 
X100 ${}^{}\mathrm {Xe}$
$<4.3 \times 10^{-4}$ 90 46
ARMENGAUD
2016
 
EDE3 GeV-scale WIMPs on ${}^{}\mathrm {Ge}$
$<7 \times 10^{-5}$ 90 47
HEHN
2016
 
EDE3 SI WIMP on ${}^{}\mathrm {Ge}$
$<6 \times 10^{-5}$ 90 48
ZHAO
2016
 
CDEX GeV-scale WIMPs on ${}^{}\mathrm {Ge}$
$<1 \times 10^{-4}$ 90 49
AMOLE
2015
 
PICO ${}^{}\mathrm {C}_{3}{}^{}\mathrm {F}_{8}$
$<8 \times 10^{-5}$ 90 50
XIAO
2015
 
PNDX WIMPs on ${}^{}\mathrm {Xe}$
$<3 \times 10^{-5}$ 90 51
AGNESE
2014
 
SCDM GeV-scale WIMPs
$<1 \times 10^{-3}$ 90 52
AKERIB
2014
 
LUX WIMP on ${}^{}\mathrm {Xe}$
$<9 \times 10^{-4}$ 90 53
LI
2013B
 
TEXO WIMPs on ${}^{}\mathrm {Ge}$
$<3 \times 10^{-4}$ 90 54
ARCHAMBAULT
2012
 
PICA ${}^{}\mathrm {C}_{4}{}^{}\mathrm {F}_{10}$
$<2 \times 10^{-4}$ 90 55
AALSETH
2011
 
CGNT GeV WIMPs on ${}^{}\mathrm {Ge}$
$<5 \times 10^{-4}$ 90 56
AHMED
2011B
 
CDM2 GeV-scale WIMPs on ${}^{}\mathrm {Ge}$
$<8 \times 10^{-5}$ 90 57
ANGLE
2011
 
XE10 ${}^{}\mathrm {Xe}$
$<5 \times 10^{-4}$ 90 58
AKERIB
2010
 
CDM2 WIMPs on ${}^{}\mathrm {Ge}/{}^{}\mathrm {Si}$
1  AALBERS 2025A search for sub-GeV cosmic-ray boosted wimps at LZ. No signal observed. Limits placed in m(DM): $1 \times 10^{-4} - 1$ GeV range vs. ${{\mathit \sigma}^{SI}}$ plane. Quoted limit for m(DM) = 1 MeV.
2  ADAMS 2025 report on fermionic DM in MeV range search via DM absorption at PICO-60. No signal observed. Limits placed on absorption cross section for EFT operator O$_{4}$ vs. m(DM) .
3  APRILE 2025 report light DM search near edge of neutrino fog using XENONnT. No signal observed. Require ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) $<$ $2.5 \times 10^{-9}$ pb for m(${{\mathit \chi}}$) = 6 GeV.
4  APRILE 2025A search for light MeV-scale DM using XENONnT. No signal observed. Limits placed in various planes. Quoted limit for Halo light DM with heavy mediator Fig. 5b with m(${{\mathit \chi}}$) = 1 GeV.
5  BUI 2025 report search for light DM via phonons in TESSERACT detector. No signal observed. Limits placed in m(${{\mathit \chi}}$) vs. ${{\mathit \sigma}^{SI}}$ plane for MeV-scale DM. Quoted limit is for m(${{\mathit \chi}}$) = 87 MeV.
6  ZHANG 2025B search for light GeV-scale wimps using run 0 and run 1 PandaX-4T data. No signal observed. Quoted limit is for m(${{\mathit \chi}}$) = 3 GeV.
7  ANGLOHER 2024 search for spin-independent light WIMP (mass between 0.16 and 6 GeV) scatter on diamond target. No signal observed. Limits placed in ${{\mathit \sigma}^{SI}}$ vs mass plane for sub-GeV WIMPs. Quoted limit is for m(WIMP) = 0.2 GeV.
8  ANGLOHER 2024B search for low mass m(wimp) $\sim{}$100 MeV. No signal observed. Limits placed in cross section vs. mass plane. Quoted limit for m(wimp) = 100 MeV.
9  AALBERS 2023A search for ${{\mathit e}}$ recoil events from GeV scale WIMP scatter on ${}^{}\mathrm {Xe}$. No signal observed. Limits placed on 6 different models including ${{\mathit \sigma}^{SI}}$ $<$ $3 \times 10^{-3}$ for m(${{\mathit \chi}}$) $\sim{}$ 1 GeV via Migdal scattering.
10  AGNES 2023 for for light DM via ${{\mathit e}}$ recoil/Migdal effect. No signal observed. ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) $<$ $4 \times 10^{-7}$ pb for m(${{\mathit \chi}}$) = 3 GeV.
11  AGNES 2023B search for GeV-scale DM scatter on nucleons in ${}^{}\mathrm {Ar}$. No signal observed. Limit ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) $<$ $6 \times 10^{-7}$ pb for m(${{\mathit \chi}}$) = 3 GeV.
12  ALBAKRY 2023 search for light DM via Migdal effect. No signal observed. Allow ${{\mathit \sigma}^{SI}}$ $<$ $0.5$ pb for m(${{\mathit \chi}}$)=1 GeV (see e.g. Fig. 7).
13  AMBROSONE 2023 derive limits on ${{\mathit \sigma}}({{\mathit \chi}}{{\mathit p}}$) due to possible DM distortion of cosmic ray spectra in starburst galaxies. Limits placed in ${{\mathit \sigma}}$ vs. mass ($10^{-3} - 10$ MeV) plane, the most stringent given above being at 1 keV.
14  ANGLOHER 2023 search for light DM using ${}^{}\mathrm {Si}$ target. No signal observed. Require ${{\mathit \sigma}^{SI}}$ $<$ $70$ pb for m(${{\mathit \chi}}$) = 0.3 GeV (see e.g. Fig. 5).
15  LI 2023F searches for SI light DM scatter from ${}^{}\mathrm {Xe}$. No signal observed. The quoted limit for m(${{\mathit \chi}}$) = 4 GeV.
16  MA 2023A search for GeV-scale DM using PandaX-4T. No signal observed. ${{\mathit \sigma}}({{\mathit \chi}}{{\mathit p}}$) $<$ $5 \times 10^{-10}$ pb for m(${{\mathit \chi}}$) = 10 GeV.
17  ADHIKARI 2022B search for sub-GeV WIMPs via SI and SD detection; no signal detected; limits placed in m(${{\mathit \chi}}$) vs. ${{\mathit \sigma}}$ plane for m(${{\mathit \chi}}$): $0.2 - 3$ GeV; quoted limit is for m(${{\mathit \chi}}$) = 1 GeV.
18  ARMENGAUD 2022 search for GeV-scale DM scatter on ${}^{}\mathrm {Ge}$ at EDELWEISS via Migdal effect; no signal observed; limits placed in ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) vs. m(DM) plane; quoted limit is for m(DM) = 100 MeV.
19  CUI 2022 search for sub-GeV boosted DM at PandaX-II at CJPL; no signal detected; limits set in ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit p}}$) vs. m(${{\mathit \chi}}$) plane; quoted limit for m(${{\mathit \chi}}$) = 0.1 GeV.
20  XU 2022 search for sub-GeV boosted DM in CDEX; no signal observed; limits placed in ${\mathit \sigma (}{{\mathit \chi}}{{\mathit N}}{)}$ vs. m(DM) plane; quoted limit is for m(DM) = 0.1 GeV.
21  AKERIB 2021A present new technique for low mass WIMP detection. Require ${{\mathit \sigma}^{SI}}({{\mathit p}}{{\mathit \chi}}$) $<$ $2 \times 10^{-7}$ pb for m(WIMP) 10 GeV.
22  ALKHATIB 2021 search for light DM using SuperCDMS; require ${{\mathit \sigma}^{SI}}({{\mathit p}}{{\mathit \chi}}$) $<$ $5 \times 10^{6}$ for m(DM) = 0.1 GeV.
23  ANDRIAMIRADO 2021A search for upscattered (boosted) sub-GeV DM interacting with proton in PROSPECT detector. No signal observed. Limits placed in ${{\mathit \sigma}}({{\mathit \chi}}{{\mathit N}}$) vs. m(DM) plane for m(DM) $\sim{}$ 1 keV $−$ 0.5 GeV. The listed limit is for m(DM) = 1 keV.
24  APRILE 2021 search for low recoil energy GeV-scale DM in XENON1T with 1.6 keV threshold. No signal in 0.6 t y exposure. Limits placed in ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) vs. m(DM) plane for m(DM) between $3 - 12$ GeV. The listed limit is for m(DM) = 5 GeV.
25  AGUILAR-AREVALO 2020C search for WIMP SI scatter on ${}^{}\mathrm {Si}$ using DAMIC at SNOLab; some excess; limits placed in ${{\mathit \sigma}}$ vs m(DM) for m(DM) in $1.2 - 10$ GeV; quoted limit for m(WIMP) = 2 GeV.
26  AKERIB 2020A search for GeV-scale WIMPs via WIMP-nucleon scatter with single photon emission; no signal; limits placed in m(WIMP) vs ${{\mathit \sigma}^{SI}}$ plane: for example ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit n}}$) $<$ $8 \times 10^{-4}$ pb for m(WIMP) = 2.5 GeV.
27  ABDELHAMEED 2019A search for GeV scale dark matter SI scatter on ${}^{}\mathrm {CaWO}_{4}$; no signal, limits placed in ${{\mathit \sigma}}$ vs. mass plane for m(DM) $\sim{}$ $0.1 - 10$ GeV. The listed limit is for m(DM) = 1 GeV.
28  AGNESE 2019A search for $1.5 - 10$ GeV WIMP scatter on ${}^{}\mathrm {Ge}$ in CDMSlite dataset. Limits set in a likelihood analysis. No signal was observed. Limit reported for m(${{\mathit \chi}}$) = 5 GeV.
29  AKERIB 2019 search for $0.4 - 5$ GeV DM using bremsstrahlung photons and "Migdal" electrons; $1.4 \times 10^{4}$ kg d exposure of liquid ${}^{}\mathrm {Xe}$; constraint ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) $<$ 1 pb for m(${{\mathit \chi}}$) = 5 GeV in light scalar mediator model.
30  AMOLE 2019 search for SI WIMP scatter on ${}^{}\mathrm {C}_{3}{}^{}\mathrm {F}_{8}$ in PICO-60 bubble chamber; no signal: set limit for spin independent coupling ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) $<$ $1 \times 10^{-6}$ pb for m(${{\mathit \chi}}$) = 5 GeV.
31  APRILE 2019C search for light DM scatter on ${}^{}\mathrm {Xe}$ via atomic excitation, ionization (Migdal effect) or bremsstrahlung; no signal, limits placed in ${{\mathit \sigma}}$ vs. m(DM) plane for m(DM) $\sim{}$ $0.085 - 2$ GeV. The listed limit is for m(DM) = 1 GeV.
32  APRILE 2019D search for light DM scatter on ${}^{}\mathrm {Xe}$ via ionization to probe SI, SD, and ${{\mathit \chi}}{{\mathit e}}$ cross sections; with 22 t d exposure, limits placed in various ${{\mathit \sigma}}$ vs. m(DM) planes. Quoted limit is for m(DM) = 5 GeV.
33  ARMENGAUD 2019search for GeV scale WIMP scatter on ${}^{}\mathrm {Ge}$; limits placed in ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) vs. m(${{\mathit \chi}}$) plane for m(${{\mathit \chi}}$) $\sim{}$ $0.045 - 10$ GeV; quoted limit is for m(${{\mathit \chi}}$) = 5 GeV.
34  KOBAYASHI 2019 search for sub-GeV WIMP annual modulation in ${}^{}\mathrm {Xe}$ via brems; no signal; limits placed in ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) vs. m(${{\mathit \chi}}$) plane for m $\sim{}$ $0.3 - 1$ GeV; quoted limit is for m(${{\mathit \chi}}$) = 0.5 GeV.
35  LIU 2019B seach for sub-GeV DM using Migdal effect on ${}^{}\mathrm {Ge}$ at CDEX-IB; no signal, require ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) $<$ $7 \times 10^{2}$ pb for m(${{\mathit \chi}}$) = 0.1 GeV.
36  AGNES 2018 search for $1.8 - 20$ GeV WIMP SI scatter on ${}^{}\mathrm {Ar}$; quoted limit is for m(${{\mathit \chi}}$) = 5 GeV.
37  AGNESE 2018 search for GeV scale WIMPs using CDMSlite; limits placed in ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) vs. m(${{\mathit \chi}}$) plane for m $\sim{}$ $1.5 - 20$ GeV; quoted limit is for m(${{\mathit \chi}}$) = 5 GeV.
38  APRILE 2018 search for WIMP scatter on 1 t yr ${}^{}\mathrm {Xe}$; no signal, limits set in ${{\mathit \sigma}}({{\mathit \chi}}{{\mathit N}}$) vs. m(${{\mathit \chi}}$) plane for m(${{\mathit \chi}}$) $\sim{}$ $6 - 1000$ GeV; quoted limit is for m = 6 GeV.
39  ARNAUD 2018 search for low mass WIMP scatter on ${}^{}\mathrm {Ne}$ via SPC at NEWS-G; limits set in ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) vs. m(${{\mathit \chi}}$) plane for m $\sim{}$ $0.5 - 20$ GeV; quoted limit is for m = 5 GeV.
40  JIANG 2018 search for GeV scale WIMP scatter on ${}^{}\mathrm {Ge}$; limits placed in ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) vs. m(${{\mathit \chi}}$) plane for m(${{\mathit \chi}}$) $\sim{}$ $3 - 10$ GeV; quoted limit is for m(${{\mathit \chi}}$) = 5 GeV.
41  YANG 2018 search for WIMP scatter on ${}^{}\mathrm {Ge}$; limits placed in ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) vs. m(${{\mathit \chi}}$) plane for m(${{\mathit \chi}}$) $\sim{}$ $2 - 10$ GeV; quoted limit is for m(${{\mathit \chi}}$) = 5 GeV.
42  AKERIB 2017 search for WIMP scatter on ${}^{}\mathrm {Xe}$; limits placed in ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) vs. m(${{\mathit \chi}}$) plane for m(${{\mathit \chi}}$) $\sim{}$ $5 - 1 \times 10^{5}$ GeV; quoted limit is for m(${{\mathit \chi}}$) = 5 GeV.
43  ANGLOHER 2017A search for GeV scale WIMP scatter on ${}^{}\mathrm {Al}_{2}{}^{}\mathrm {O}_{3}$ crystal; limits placed in ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) vs. m(${{\mathit \chi}}$) plane for m(${{\mathit \chi}}$) $\sim{}$ $0.15 - 10$ GeV; quoted limit is for m(${{\mathit \chi}}$) = 5 GeV.
44  ANGLOHER 2016 search for GeV scale WIMP scatter on ${}^{}\mathrm {CaWO}_{4}$; limits placed in ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) vs. m(${{\mathit \chi}}$) plane for m(${{\mathit \chi}}$) $\sim{}$ $0.5 - 30$ GeV; quoted limit is for m(${{\mathit \chi}}$) = 5 GeV.
45  APRILE 2016 search for low mass WIMPs via ionization at XENON100; limits placed in ${{\mathit \sigma}}{}^{SI}({{\mathit \chi}}{{\mathit N}}$) vs m(${{\mathit \chi}}$) plane for m $\sim{}$ $3.5 - 20$ GeV; quoted limit is for m(${{\mathit \chi}}$) = 5 GeV.
46  ARMENGAUD 2016 search for GeV scale WIMP scatter on ${}^{}\mathrm {Ge}$; limits placed in ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) vs. m(${{\mathit \chi}}$) plane for m(${{\mathit \chi}}$) $\sim{}$ $4 - 30$ GeV; quoted limit is for m(${{\mathit \chi}}$) = 5 GeV.
47  HEHN 2016 search for low mass WIMPs via SI scatter on ${}^{}\mathrm {Ge}$ target using profile likelihood analysis; limits placed in ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) vs. m(${{\mathit \chi}}$) plane for m(${{\mathit \chi}}$) $\sim{}$ $4 - 30$ GeV; quoted limit is for m(${{\mathit \chi}}$) = 5 GeV.
48  ZHAO 2016 search for GeV-scale WIMP scatter on ${}^{}\mathrm {Ge}$; limits placed in ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) vs. m(${{\mathit \chi}}$) plane for m(${{\mathit \chi}}$) $\sim{}$ $4 - 30$ GeV; quoted limit is for m(${{\mathit \chi}}$) = 5 GeV.
49  AMOLE 2015 search for WIMP scatter on ${}^{}\mathrm {C}_{3}{}^{}\mathrm {F}_{8}$ in PICO-2L; limits placed in ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) vs. m(${{\mathit \chi}}$) plane for m(${{\mathit \chi}}$) $\sim{}$ $4 - 25$ GeV; quoted limit is for m(${{\mathit \chi}}$) = 5 GeV.
50  XIAO 2015 search for WIMP scatter on ${}^{}\mathrm {Xe}$ with PandaX-I; limits placed in ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) vs. m(${{\mathit \chi}}$) plane for m(${{\mathit \chi}}$) $\sim{}$ $5 - 100$ GeV; quoted limit is for m(${{\mathit \chi}}$) = 5 GeV.
51  AGNESE 2014 search for GeV scale WIMPs SI scatter at SuperCDMS; no signal, limits placed in ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) vs. m(${{\mathit \chi}}$) plane for m(${{\mathit \chi}}$) $\sim{}$ $3.5 - 30$ GeV; quoted limit is for m(${{\mathit \chi}}$) = 5 GeV.
52  AKERIB 2014 search for WIMP scatter on ${}^{}\mathrm {Xe}$; limits placed in ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) vs. m(${{\mathit \chi}}$) plane for m(${{\mathit \chi}}$) $\sim{}$ $5 - 5000$ GeV. Limit given for m(${{\mathit \chi}}$) = 5 GeV.
53  LI 2013B search for WIMP scatter on ${}^{}\mathrm {Ge}$; limits placed in ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) vs. m(${{\mathit \chi}}$) plane for m(${{\mathit \chi}}$) $\sim{}$ $4 - 100$ GeV; quoted limit is for m(${{\mathit \chi}}$) = 5 GeV.
54  ARCHAMBAULT 2012 search for low mass WIMP scatter on ${}^{}\mathrm {C}_{4}{}^{}\mathrm {F}_{10}$; limits set in ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) vs. m(${{\mathit \chi}}$) plane for m $\sim{}$ $4 - 12$ GeV; quoted limit is for m = 5 GeV.
55  AALSETH 2011 search for GeV-scale SI WIMP scatter on ${}^{}\mathrm {Ge}$; limits placed on ${{\mathit \sigma}}{}^{SI}({{\mathit \chi}}{{\mathit N}}$) for m(${{\mathit \chi}}$) $\sim{}$ $3.5 - 100$ GeV; quoted limit is for m(${{\mathit \chi}}$) = 5 GeV.
56  AHMED 2011B search for GeV scale WIMP scatter on ${}^{}\mathrm {Ge}$ in CDMS II; limits placed in ${{\mathit \sigma}^{SD}}({{\mathit \chi}}{{\mathit n}}$) vs. m(${{\mathit \chi}}$) plane for m $\sim{}$ $4 - 12$ GeV.
57  ANGLE 2011 search for GeV scale WIMPs in Xenon-10; limits placed in ${{\mathit \sigma}^{SI}}({{\mathit \chi}}{{\mathit N}}$) vs. m(${{\mathit \chi}}$) plane for m(${{\mathit \chi}}$) $\sim{}$ $4 - 20$ GeV; quoted limit is for m(${{\mathit \chi}}$) = 5 GeV.
58  AKERIB 2010 search for WIMP scatter on ${}^{}\mathrm {Ge}/{}^{}\mathrm {Si}$ in CDMS II; limits place in ${{\mathit \sigma}_{{{SI}}}}({{\mathit \chi}}{{\mathit N}}$) vs. m(${{\mathit \chi}}$) plane for m $\sim{}$ $3 - 100$ GeV. Limit given for m(DM) = 5 GeV.
References