Dark Matter Particle (${{\mathit X}^{0}}$) Production in Hadron Collisions

INSPIRE   JSON  (beta) PDGID:
S030DMP
Searches for ${{\mathit X}^{0}}$ production in asociation with observable particles (${{\mathit \gamma}}$, jets, $\ldots$) in high energy hadron collisions. If a specific form of effective interaction Lagrangian is assumed, the limits may be translated into limits on ${{\mathit X}^{0}}$-nucleon scattering cross section.

VALUE DOCUMENT ID TECN  COMMENT
• • We do not use the following data for averages, fits, limits, etc. • •
1
AAD
2024AC
 ATLS ${{\mathit t}}{{\overline{\mathit t}}}$ + mediator
2
AAD
2024AC
 ATLS ${{\mathit t}}{{\overline{\mathit t}}}$ + mediator
3
AAD
2024AH
 ATLS SUSY pMSSM search
4
AAD
2024AK
 ATLS ${\mathit {\mathit t}}$ + MET search
5
AAD
2024CD
 ATLS hadronic ${{\mathit W}}$ $/$ ${{\mathit Z}}$ + MET search
6
HAYRAPETYAN
2024B
 CMS inelastic DM search
7
HAYRAPETYAN
2024W
 CMS dark matter/dark Higgs
8
AAD
2023A
 ATLS ${{\mathit H}}$ $\rightarrow$ invisible search
9
AAD
2023AF
 ATLS ${{\overline{\mathit t}}}$ ${{\mathit t}}$ ${+}$ ${{\mathit H}}$ $\rightarrow$ invisible search
10
AAD
2023AJ
 ATLS extended 2HDM search
11
AAD
2023BX
 ATLS ${{\mathit H}}$ ${{\mathit a}}$ , ${{\mathit a}}$ $\rightarrow$ DM search
12
AAD
2023W
 ATLS dark Higgs model
13
AKIMOV
2023
COHR LDM search at SNS
14
LIN
2023C
 KOTO ${{\mathit \chi}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ from ${{\mathit K}_L^0}$ decay
15
AAD
2022D
 ATLS ${{\mathit Z}}+{{\mathit H}}$ with ${{\mathit H}}$ $\rightarrow$ DM
16
AAD
2022P
 ATLS ${{\mathit H}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit \chi}}$ search via VBF
17
AGUILAR-AREVA..
2022A
 CCM ${{\mathit p}}$ dump search for MeV-scale DM
18
TUMASYAN
2022AA
 CMS ${{\mathit Z}^{\,'}}$ $\rightarrow$ DM search
19
TUMASYAN
2022AG
 CMS strongly interacting DM search
20
TUMASYAN
2022G
 CMS DM search via VBF to Higgs
21
AAD
2021AZ
 ATLS DM search in ${{\mathit H}}$ $\not E_T$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ $\not E_T$
22
AAD
2021BB
 ATLS DM search in ${{\mathit H}}$ $\not E_T$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ $\not E_T$
23
AAD
2021D
 ATLS Dark Higgs
24
AAD
2021F
 ATLS jet + missing momentum
25
AAD
2021K
 ATLS photon + DM
26
AAD
2021O
 ATLS ${{\mathit \ell}}$ + jets + $\not E_T$ to search for ${{\mathit t}}$-pairs + DM
27
AAD
2021P
 ATLS ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ + jets + $\not E_T$
28
AAD
2021S
 ATLS ${{\mathit b}}$-jets + $\not E_T$
29
SIRUNYAN
2021A
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit \chi}}{{\mathit \chi}}$; ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\overline{\mathit \ell}}}$
30
TUMASYAN
2021D
 CMS DM search in jets + $\not E_T$
31
SIRUNYAN
2020X
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit A}}$( ${{\mathit Z}^{\,'}}$) ${{\mathit h}}$ $\rightarrow$ ${{\mathit h}}$ + $\not E_T$
32
AABOUD
2019AA
 ATLS multi-channel BSM search
33
AABOUD
2019AI
 ATLS ${{\mathit H}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit \chi}}$
34
AABOUD
2019AL
 ATLS ${{\mathit H}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit \chi}}$
35
AABOUD
2019Q
 ATLS single ${{\mathit t}}+\not E_T$
36
AABOUD
2019V
 ATLS review mediator based DM searches
37
BANERJEE
2019
NA64 ${{\mathit e}}$ ${{\mathit N}}$ $\rightarrow$ ${{\mathit e}}{{\mathit N}}+\not E$
38
SIRUNYAN
2019AN
 CMS ${{\mathit H}}$ ${{\mathit \chi}}$ ${{\mathit \chi}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ $\not E_T$
39
SIRUNYAN
2019BC
 CMS LQ LQ $\rightarrow$ ${{\mathit \mu}}{{\mathit j}}$ $\not E_T$
40
SIRUNYAN
2019BO
 CMS ${{\mathit V}}$ ${{\mathit V}}$ $\rightarrow$ ${{\mathit H}}{{\mathit q}}{{\mathit q}}$; ${{\mathit H}}$ $\rightarrow$ DM
41
SIRUNYAN
2019C
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit \chi}}{{\mathit \chi}}$
42
SIRUNYAN
2019O
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \gamma}}$ $\not E_T$
43
SIRUNYAN
2019X
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit t}}}$ + $\not\!\!p_T$; ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}$( ${{\overline{\mathit t}}}$) + $\not\!\!p_T$
44
AABOUD
2018
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit \chi}}{{\mathit \chi}}$; ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}$
45
AABOUD
2018A
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit t}}}$ $\not E_T$; ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ $\not E_T$
46
AABOUD
2018CA
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit V}}{{\mathit \chi}}{{\mathit \chi}}$; ${{\mathit V}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$
47
AABOUD
2018I
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ jet(s) + $\not E_T$
48
AGUILAR-AREVA..
2018B
 MBNE ${{\mathit p}}$ ${{\mathit N}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit X}}$, ${{\mathit \chi}}$ = ${{\mathit e}}$, ${{\mathit \pi}}$, or ${{\mathit N}}$
49
KHACHATRYAN
2018
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}({{\mathit \ell}}{{\mathit \ell}}$) + $\not E_T$
50
SIRUNYAN
2018BF
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}$ $\not E_T$
51
SIRUNYAN
2018BO
 CMS dijet resonance search
52
SIRUNYAN
2018BV
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}$ $\not E_T$
53
SIRUNYAN
2018C
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit t}}}$ $\not E_T$
54
SIRUNYAN
2018CU
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}$ $\not E_T$
55
SIRUNYAN
2018DH
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit \chi}}{{\mathit h}}$; ${{\mathit h}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ or ${{\mathit \tau}}{{\overline{\mathit \tau}}}$
56
SIRUNYAN
2018S
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ jets $\not E_T$
57
AABOUD
2017A
 ATLS ${{\mathit p}}{{\mathit p}}$ (${{\mathit H}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ + WIMP pair)
58
AABOUD
2017AM
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit A}}{{\mathit h}}$ $\rightarrow$ ${{\mathit h}}$( ${{\mathit b}}{{\overline{\mathit b}}}$) + $\not E_T$
59
AABOUD
2017AQ
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit h}}$( ${{\mathit \gamma}}{{\mathit \gamma}}$) + $\not E_T$
60
AABOUD
2017BD
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$jet(s) + $\not E_T$
61
AABOUD
2017R
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \gamma}}\not E_T$
62
AGUILAR-AREVA..
2017A
 MBNE ${{\mathit p}}$ ${{\mathit N}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit \chi}}{{\mathit X}}$; ${{\mathit \chi}}$ ${{\mathit N}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit N}}$
63
BANERJEE
2017
NA64 ${{\mathit e}}$ ${{\mathit N}}$ $\rightarrow$ ${{\mathit e}}{{\mathit N}}{{\mathit \gamma}^{\,'}}$
64
KHACHATRYAN
2017A
 CMS forward jets + $\not E_T$
65
KHACHATRYAN
2017F
 CMS ${{\mathit H}}$ $\rightarrow$ invisibles
66
SIRUNYAN
2017
CMS ${{\mathit Z}}$ + $\not E_T$
67
SIRUNYAN
2017AP
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit A}}{{\mathit h}}$ $\rightarrow$ ${{\mathit h}}$ + $\not E_T$
68
SIRUNYAN
2017AQ
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \gamma}}$ + $\not E_T$
69
SIRUNYAN
2017BB
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit t}}}+\not E_T$; ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}+\not E_T$
70
SIRUNYAN
2017G
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}$ + $\not E_T$
71
SIRUNYAN
2017U
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit \chi}}{{\mathit \chi}}$ ; ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\overline{\mathit \ell}}}$
72
AABOUD
2016AD
 ATLS (${{\mathit W}}$ or ${{\mathit Z}}$ $\rightarrow$ jets) + $\not E_T$
73
AAD
2016AF
 ATLS ${{\mathit V}}$ ${{\mathit V}}$ $\rightarrow$ forward jets +$\not E_T$
74
AAD
2016AG
 ATLS ${{\mathit \ell}}$ + jets
75
AAD
2016M
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}}$ + $\not E_T$, ${{\mathit H}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$
76
KHACHATRYAN
2016BZ
 CMS jet(s) + $\not E_T$
77
KHACHATRYAN
2016CA
 CMS jets + $\not E_T$
78
KHACHATRYAN
2016N
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \gamma}}$+ $\not E_T$
79
AAD
2015AS
 ATLS ${{\mathit b}}$ (${{\overline{\mathit b}}}$) + $\not E_T$, ${{\mathit t}}{{\overline{\mathit t}}}$ + $\not E_T$
80
AAD
2015BH
 ATLS jet + $\not E_T$
81
AAD
2015CF
 ATLS ${{\mathit H}^{0}}$ + $\not E_T$
82
AAD
2015CS
 ATLS ${{\mathit \gamma}}$ + $\not E_T$
83
KHACHATRYAN
2015AG
 CMS ${{\mathit t}}{{\overline{\mathit t}}}$ + $\not E_T$
84
KHACHATRYAN
2015AL
 CMS jet + $\not E_T$
85
KHACHATRYAN
2015T
 CMS ${{\mathit \ell}}$ + $\not E_T$
86
AAD
2014AI
 ATLS ${{\mathit W}}$ + $\not E_T$
87
AAD
2014BK
 ATLS ${{\mathit W}}$, ${{\mathit Z}}$ + $\not E_T$
88
AAD
2014K
 ATLS ${{\mathit Z}}$ + $\not E_T$
89
AAD
2014O
 ATLS ${{\mathit Z}}$ + $\not E_T$
90
AAD
2013AD
 ATLS jet + $\not E_T$
91
AAD
2013C
 ATLS ${{\mathit \gamma}}$ + $\not E_T$
92
AALTONEN
2012K
 CDF ${{\mathit t}}$ + $\not E_T$
93
AALTONEN
2012M
 CDF jet + $\not E_T$
94
CHATRCHYAN
2012AP
 CMS jet + $\not E_T$
95
CHATRCHYAN
2012T
 CMS ${{\mathit \gamma}}$ + $\not E_T$
1  AAD 2024AC search for ${{\mathit t}}{{\overline{\mathit t}}}$ + mediator, where mediator decays to dark matter, within 140 fb${}^{-1}$ of data. No signal observed. Limits placed in ${{\mathit \sigma}}$ vs m(mediator) plane.
2  AAD 2024AC search for ${{\mathit t}}{{\overline{\mathit t}}}$+MET signal at $\sqrt {s }$=13 TeV and 139 fb${}^{-1}$. No signal observed. Assume DM mediator model coupling to ${{\mathit t}}{{\overline{\mathit t}}}$ and limits placed in various m(DM), m(mediator), coupling planes.
3  AAD 2024AH search for SUSY in pMSSM model. No signal observed. Several regions of DM-allowed parameters space now ruled out.
4  AAD 2024AK search for top + MET in various simplified models including mediator decaying to DM. No signal observed. Limits placed in various parameter space planes.
5  AAD 2024CD search for hadronically-decaying ${{\mathit W}}$ $/$ ${{\mathit Z}}$ plus MET events in 140 fb${}^{-1}$ at 13 TeV. No signal observed. Limits placed in m(${{\mathit \chi}}$) vs. mediator mass plane for simplified dark matter model.
6  HAYRAPETYAN 2024B search for inelastic DM production where heavier state decays to displaced muons. No signal observed. Limits placed in signal strength vs mass plane for various choices of mass gap.
7  HAYRAPETYAN 2024W search for dark matter via dark Higgs decay in ${{\mathit W}}{{\mathit W}}$ + MET events. No signal observed. Limits placed in m(${{\mathit \chi}}$) vs m(mediator) or m(${{\mathit s}}$) plane where ${{\mathit s}}$ is dark Higgs.
8  AAD 2023A search for ${{\mathit H}}$ $\rightarrow$ invisible. No signal observed. Results interpreted in terms of several DM Higgs portal simplified models.
9  AAD 2023AF search for ${{\overline{\mathit t}}}$ ${{\mathit t}}$ ${+}$ ${{\mathit H}}$ $\rightarrow$ invisible with 139 fb${}^{-1}$ of data. No signal observed. Limits placed on branching fractions of ${{\mathit H}}$ decays etc. for various DM mediator models. Result also included in AAD 2023A.
10  AAD 2023AJ search for ${{\mathit t}}{{\mathit W}}{{\mathit \chi}}{{\mathit \chi}}$ production in mediator-extended 2HDM with 139 fb${}^{-1}$ of data. No signal observed. Limits placed in m(H) vs. m(mediator) and tan$(\beta )$ vs. m(H) planes.
11  AAD 2023BX search for ${{\mathit A}}$ $\rightarrow$ ${{\mathit H}}{{\mathit a}}$ production where ${{\mathit H}}$ $\rightarrow$ ${{\mathit \tau}}{{\overline{\mathit \tau}}}$ and ${{\mathit a}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit \chi}}$. No signal observed. Limits placed on 2HDM+a model.
12  AAD 2023W search for DM in dark Higgs model via ${{\mathit W}}{{\mathit W}}{{\mathit \chi}}{{\mathit \chi}}$ final state with 139 fb${}^{-1}$ of data. No signal detected. Limits set in m(dark Higgs) vs. m(${{\mathit Z}^{\,'}}$) plane.
13  AKIMOV 2023 search for light DM via COHERENT ${}^{}\mathrm {CsI}$ detector at SNS. No signal observed. For scalar DM model, limits set for m(${{\mathit \chi}}$) = $1 - 300$ MeV. Limit of ${\mathit \sigma (}{{\mathit \chi}}{{\mathit N}}{)}$ $<$ $1 \times 10^{1}$ pb set at peak sensitivity m(${{\mathit \chi}}$) = 25 MeV.
14  LIN 2023C search for ${{\mathit \chi}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ decay where ${{\mathit p}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit \chi}}$ at KOTO. No signal observed. Limits placed on ${{\mathit K}_L^0}$ branching fraction.
15  AAD 2022D search for ${{\mathit Z}}+{{\mathit H}}$ production with ${{\mathit Z}}$ $\rightarrow$ ${{\mathit l}}{{\overline{\mathit l}}}$ and ${{\mathit H}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit \chi}}$ with 139 fb${}^{-1}$ at 13 TeV; no signal found; limits placed in various simplified models depending on Higgs portal and DM mediator.
16  AAD 2022P search for ${{\mathit H}}$ production via VBF with ${{\mathit H}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit \chi}}$ with 139 fb${}^{-1}$ at 13 TeV; no signal found; limits placed for various Higgs DM portal simplified models.
17  AGUILAR-AREVALO 2022A report search for MeV vector portal and leptophobic DM via scatter on liquid ${}^{}\mathrm {Ar}$ at the Lujan stopped pion source at LANL; no signal detected; limits placed on vector portal and leptophobic DM vs. m(${{\mathit \chi}}$): $1 - 40$ MeV.
18  TUMASYAN 2022AA search for ${{\mathit Z}^{\,'}}$ decay to dark quarks with 138 fb${}^{-1}$ at 13 TeV; no signal observed; limits exclude a wide range of strongly coupled hidden sector models.
19  TUMASYAN 2022AG search for strongly interacting dark matter production via scalar mediator, with SIMP decay to trackless jets with 16.1 fb${}^{-1}$ at 13 TeV; no signal detected; limits placed in mass vs. cross section plane for simplified models.
20  TUMASYAN 2022G search for VBF production of Higgs with ${{\mathit H}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit \chi}}$ with 101 fb${}^{-1}$ at 13 TeV, combined with earlier searches, in total 19.7 fb${}^{-1}$ at 8 TeV and 140 fb${}^{-1}$ at 13 TeV are used; no signal detected; limits placed in mass vs. cross section plane for various Higgs portal simplified models.
21  AAD 2021AZ search for DM in ${{\mathit H}}$ $\not E_T$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ $\not E_T$ events with 139 fb${}^{-1}$ at 13 TeV. No signal observed. Limits placed for several simplified models.
22  AAD 2021BB search for DM in ${{\mathit H}}$ $\not E_T$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ $\not E_T$ events with 139 fb${}^{-1}$ at 13 TeV. No signal observed. Limits placed for several simplified models.
23  AAD 2021D search for ${{\mathit V}}{{\mathit V}}{+}$ ${{\mathit \chi}}{{\mathit \chi}}$, ${{\mathit V}}$ $\rightarrow$ ${{\mathit q}}{{\overline{\mathit q}}}$ with 139 fb${}^{-1}$ at 13 TeV LHC. No signal detected. Limits placed in dark Higgs boson mass vs. m(${{\mathit Z}^{\,'}}$) plane. Here ${{\mathit V}}{{\mathit V}}$ stand for ${{\mathit W}^{\pm}}{{\mathit W}^{\mp}}$, ${{\mathit Z}}{{\mathit Z}}$.
24  AAD 2021F search for monojet recoiling against invisibles with 139 fb${}^{-1}$ at 13 TeV LHC. No signal detected. Limits placed in various simplified dark matter models.
25  AAD 2021K search for a photon recoiling against dark matter with 139 fb${}^{-1}$ at 13 TeV LHC. No signal detected. Limits placed on parameter space of various simplified models.
26  AAD 2021O search for ${{\mathit \ell}}$ + jets + $\not E_T$ to search for ${{\mathit t}}$-pairs + DM particles with 139 fb${}^{-1}$ at LHC 13 TeV LHC. No signal detected. Limits placed in the cross-section vs. mediator mass plane, assuming light DM states.
27  AAD 2021P search for ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ + jets + $\not E_T$ in context of various BSM models with 139 fb${}^{-1}$ at 13 TeV LHC. No signal observed. Limits placed in parameter space of dark matter models and SUSY.
28  AAD 2021S search for ${{\mathit b}}$-jets + $\not E_T$ signal from BSM/DM models with 139 fb${}^{-1}$ at 13 TeV LHC. No signal observed. Limits placed on parameter space of DM models.
29  SIRUNYAN 2021A search for DM production in association with leptonically decaying ${{\mathit Z}}$ boson in 137 fb${}^{-1}$ at 13 TeV; no signal; limits set in large variety of simplified DM models.
30  TUMASYAN 2021D search for DM and other exotica at CMS in jets + $\not E_T$ events with 137 fb${}^{-1}$ at 13 TeV. No signal observed. Limits placed for a variety of simplified models.
31  SIRUNYAN 2020X search for DM in ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit A}}$( ${{\mathit Z}^{\,'}}$) ${{\mathit h}}$ $\rightarrow$ ${{\mathit h}}$ + $\not E_T$ in CMS at 13 TeV with 35.9 fb${}^{-1}$; no signal; limits placed in ${{\mathit \sigma}^{SI}}$ vs. m(${{\mathit \chi}}$), and ${{\mathit \sigma}}$, m(A) and tan${{\mathit \beta}}$ vs m(Z') for considered DM models.
32  AABOUD 2019AA searches for BSM physics in more than 700 event classes with more than $10^{5}$ regions at 13 TeV with 3.2 fb${}^{-1}$; no significant signal.
33  AABOUD 2019AI searches for vector boson fusion ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}}{{\mathit q}}{{\mathit q}}$ , ${{\mathit H}}$ $\rightarrow$ invisible at 13 TeV with 36.1 fb${}^{-1}$; no signal: require B(${{\mathit H}}$ $\rightarrow$ invisible) $<$ 0.37 (0.28 expected).
34  AABOUD 2019AL perform search in three different channels for ${{\mathit H}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit \chi}}$ at 7, 8 and 13 TeV; combined result BF(${{\mathit H}}$ $\rightarrow$ invisible) $<$ 0.26 (0.17 expected).
35  AABOUD 2019Q search for single ${{\mathit t}}$ + $\not E_T$ at 13 TeV with 36.1 fb${}^{-1}$ of data; no signal; limits set in ${{\mathit \sigma}}$ or coupling vs. mass plane for simplified models.
36  AABOUD 2019V review ATLAS results from 7, 8 and 13 TeV searches for mediator-based DM and DE scalar which couples to gravity; no signal: limits set for large variety of simplified models.
37  BANERJEE 2019 search for dark photon via ${{\mathit e}}$ ${{\mathit N}}$ $\rightarrow$ ${{\mathit e}}{{\mathit N}}+\not E$ in NA64; no signal, limits placed in kinetic mixing ${{\mathit \epsilon}}$ vs. m(DM) plane for m(DM) $\sim{}$ $0.001 - 1$ GeV.
38  SIRUNYAN 2019AN search at 13 TeV with 35.9 fb${}^{-1}$ for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}}{{\mathit \chi}}{{\mathit \chi}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ $\not E_T$; no signal: limits set in the context of a 2HDM + pseudoscalar (${{\mathit a}}$) model and a baryonic ${{\mathit Z}^{\,'}}$ model.
39  SIRUNYAN 2019BC search for DM via LeptoQuark pair annihilation LQ LQ $\rightarrow$ ${{\mathit \mu}}{{\mathit j}}{{\mathit \chi}}{{\mathit \chi}}$ $\rightarrow$ ${{\mathit \mu}}{{\mathit j}}$ $\not E_T$ with 77.4 fb${}^{-1}$, 13 TeV; no signal: limits placed in m(${{\mathit \chi}}$) vs. m(LQ) plane. Model dependent limits on DM mass up to 600 GeV depending on m(LQ) placed.
40  SIRUNYAN 2019BO search for vector boson fusion ${{\mathit V}}$ ${{\mathit V}}$ $\rightarrow$ ${{\mathit q}}{{\mathit q}}{{\mathit H}}$ with ${{\mathit H}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit \chi}}$ at 13 TeV with 38.2 fb${}^{-1}$; no signal: limits placed for several models. Also search for ${{\mathit H}}$ $\rightarrow$ invisible at 7, 8, and 13 TeV; no signal: limit placed on BF $<$ 0.19.
41  SIRUNYAN 2019C search for DM via ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit \chi}}{{\mathit \chi}}$ at 13 TeV, 35.9 fb${}^{-1}$; no signal; limits placed on coupling vs. mediator mass for various simplified models.
42  SIRUNYAN 2019O search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \gamma}}$ at 13 TeV with 35.9 fb${}^{-1}$; no signal: limits placed on parameters of various models.
43  SIRUNYAN 2019X search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit t}}}$ $\not E_T$ and ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}$ $\not E_T$ + ... at 13 TeV with 35.9 fb${}^{-1}$; no signal: limits placed on ${{\mathit \chi}}$ production ${{\mathit \sigma}}$ for various simplified models with m(${{\mathit \chi}}$) = 1 GeV.
44  AABOUD 2018 search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}$ + $\not E_T$ with ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}$ at 13 TeV with 36.1 fb${}^{-1}$ of data. Limits set for simplified models.
45  AABOUD 2018A search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit t}}}$ $\not E_T$ or ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ $\not E_T$ at 13 TeV, 36.1 fb${}^{-1}$ of data. Limits set for simplified models.
46  AABOUD 2018CA search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit V}}{{\mathit \chi}}{{\mathit \chi}}$ with ${{\mathit V}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$ at 13 TeV, 36.1 fb${}^{-1}$. No signal observed. Limits set in m(DM) vs m(mediator) simplified model plane.
47  AABOUD 2018I search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}$ + $\not E_T$ at 13 TeV with 36.1 fb${}^{-1}$ of data. Limits set for simplified models with pair-produced weakly interacting dark-matter candidates.
48  AGUILAR-AREVALO 2018B search for WIMP production in MiniBooNE ${{\mathit p}}$ beam dump; no signal; limits set for m(${{\mathit \chi}}$) $\sim{}$ $5 - 50$ MeV in vector portal DM model.
49  KHACHATRYAN 2018 search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}({{\mathit \ell}}{{\mathit \ell}}$) + $\not E_T$. No signal observed. Llimits set on effective dark matter interactions and other exotic physics models.
50  SIRUNYAN 2018BF search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}$ $\not E_T$ at 13 TeV and 36 fb${}^{-1}$; no signal; limits placed on DM models involving a flavor changing neutral current, scalar resonance decaying to top quark and DM.
51  SIRUNYAN 2018BO search for high mass dijet resonances at 13 TeV and 36 fb${}^{-1}$; no signal: limits placed on various models, including simplified DM models involving a spin = 1 ${{\mathit Z}^{\,'}}$ mediator.
52  SIRUNYAN 2018BV search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}$ $\not E_T$ at 13 TeV; no signal, limits placed for various exotic physics models including DM.
53  SIRUNYAN 2018C search for new physics in ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ final states with two oppositely charged leptons at 13 TeV with 35.9 fb${}^{-1}$. Limits placed on m(mediator) and top squark for various simplified models.
54  SIRUNYAN 2018CU search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}$ $\not E_T$ at 13 TeV and 2.3 fb${}^{-1}$. No signal observed. Limits placed for various exotic models including DM.
55  SIRUNYAN 2018DH search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit \chi}}{{\mathit h}}$; ${{\mathit h}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ or ${{\mathit \tau}}{{\overline{\mathit \tau}}}$ at 13 TeV, 35.9 fb${}^{-1}$; no signal; limits placed on massive boson mediator ${{\mathit Z}^{\,'}}$ in the context of ${{\mathit Z}^{\,'}}$+2HDM and baryonic ${{\mathit Z}^{\,'}}$ models. Limits also cast in terms of spin-independent WIMP-nucleon cross section for masses $1 - 200$ GeV.
56  SIRUNYAN 2018S search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ jets $\not E_T$ at 13 TeV; no signal: limits placed on simplified dark matter models, on the branching ratio of the Higgs boson to invisible particles, and on several other exotic physics models including fermion portal DM.
57  AABOUD 2017A search for ${{\mathit H}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ + $\not E_T$. See Fig. 4b for limits set on VB mediator vs WIMP mass.
58  AABOUD 2017AM search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit A}}{{\mathit h}}$ $\rightarrow$ ${{\mathit h}}$( ${{\mathit b}}{{\overline{\mathit b}}}$) + $\not E_T$ at 13 TeV. Limits set in m(${{\mathit Z}^{\,'}}$) vs. m(${{\mathit A}}$) plane and on the visible cross section of ${{\mathit h}}$( ${{\mathit b}}{{\overline{\mathit b}}}$) + $\not E_T$ events in bins of $\not E_T$.
59  AABOUD 2017AQ search for WIMP in ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit h}}$( ${{\mathit \gamma}}{{\mathit \gamma}}$) + $\not E_T$ in 36.1 fb${}^{-1}$ of data. Limits on the visible cross section are also provided. Model dependent limits on spin independent DM - Nucleon cross-section are also presented, which are more stringent than those from direct searches for DM mass smaller than 2.5 GeV.
60  AABOUD 2017BD search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$jet(s) + $\not E_T$ at 13 TeV with 3.2 fb${}^{-1}$ of data. Limits set for simplified models. Observables corrected for detector effects can be used to constrain other models.
61  AABOUD 2017R, for an axial vector mediator in the s-channel, excludes $\mathit m$(mediator) $<$ $750 - 1200$ GeV for $\mathit m$(DM) $<$ $230 - 480$ GeV, depending on the couplings.
62  AGUILAR-AREVALO 2017A search for DM produced in 8 GeV proton collisions with steel beam dump followed by DM-nucleon scattering in MiniBooNE detector. Limit placed on DM cross section parameter ${{\mathit Y}}$ $<$ $2 \times 10^{-8}$ for ${{\mathit \alpha}_{{{D}}}}$ = 0.5 and for 0.01 $<$ $\mathit m$(DM) $<$ 0.3 GeV.
63  BANERJEE 2017 search for dark photon invisible decay via ${{\mathit e}}{{\mathit N}}$ scattering; exclude m(${{\mathit \gamma}^{\,'}}$) $<$ 100 MeV as an explanation of (${{\mathit g}_{{{\mu}}}}−$2) muon anomaly.
64  KHACHATRYAN 2017A search for WIMPs in forward jets + $\not E_T$ channel with 18.5 fb${}^{-1}$ at 8 TeV; limits set in effective theory model, Fig. 3.
65  KHACHATRYAN 2017F search for ${{\mathit H}}$ $\rightarrow$invisibles in ${{\mathit p}}{{\mathit p}}$ collisions at 7, 8, and 13 TeV; place limits on Higgs portal DM.
66  SIRUNYAN 2017 search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}$ + $\not E_T$ with 2.3 fb${}^{-1}$ at 13 TeV; no signal seen; limits placed on WIMPs and unparticles.
67  SIRUNYAN 2017AP search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit A}}{{\mathit h}}$ $\rightarrow$ ${{\mathit h}}$ + $\not E_T$ with ${{\mathit h}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ or ${{\mathit \gamma}}{{\mathit \gamma}}$ and ${{\mathit A}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit \chi}}$ with 2.3 fb${}^{-1}$ at 13 TeV. Limits set in m(${{\mathit Z}^{\,'}}$) vs. m(${{\mathit A}}$) plane.
68  SIRUNYAN 2017AQ search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \gamma}}$ + $\not E_T$ at 13 TeV with 12.9 fb${}^{-1}$. Limits derived for simplified DM models, effective electroweak-DM interaction and Extra Dimensions models.
69  SIRUNYAN 2017BB search for WIMPs via ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit t}}}+\not E_T$, ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}+\not E_T$ at 13 TeV with 2.2 fb${}^{-1}$. Limits derived for various simplified models.
70  SIRUNYAN 2017G search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}$ + $\not E_T$ with 12.9 fb${}^{-1}$ at 13 TeV; limits placed on WIMP mass/mediators in DM simplified models.
71  SIRUNYAN 2017U search for WIMPs/unparticles via ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit \chi}}{{\mathit \chi}}$, ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\overline{\mathit \ell}}}$ at 13 TeV with 2.3 fb${}^{-1}$. Limits derived for various simplified models.
72  AABOUD 2016AD place limits on ${{\mathit V}}{{\mathit V}}{{\mathit X}}{{\mathit X}}$ effective theory via search for hadronic ${{\mathit W}}$ or ${{\mathit Z}}$ plus WIMP pair production. See Fig. 5.
73  AAD 2016AF search for ${{\mathit V}}$ ${{\mathit V}}$ $\rightarrow$ (${{\mathit H}}$ $\rightarrow$ WIMP pair) + forward jets with 20.3 ${\mathrm {fb}}{}^{-1}$ at 8 TeV; set limits in Higgs portal model, Fig. 8.
74  AAD 2016AG search for lepton jets with 20.3 fb${}^{-1}$ of data at 8 TeV; Fig. 13 excludes dark photons around $0.1 - 1$ GeV for kinetic mixing $10^{-6} - 10^{-2}$.
75  AAD 2016M search with 20.3 fb${}^{-1}$ of data at 8 TeV ${{\mathit p}}{{\mathit p}}$ collisions; limits placed on EFT model (Fig. 7) and simplified ${{\mathit Z}^{\,'}}$ model (Fig. 6).
76  KHACHATRYAN 2016BZ search for jet(s) + $\not E_T$ in 19.7 fb${}^{-1}$ at 8 TeV; limits set for variety of simplified models.
77  KHACHATRYAN 2016CA search for WIMPs via jet(s) + $\not E_T$ using razor variable; require mediator scale $>$ 1 TeV for various effective theories.
78  KHACHATRYAN 2016N search for ${{\mathit \gamma}}$ + WIMPs in 19.6 fb${}^{-1}$ at 8 TeV; limits set on SI and SD WIMP-${{\mathit p}}$ scattering in Fig. 3.
79  AAD 2015AS search for events with one or more bottom quark and missing $\mathit E_{T}$, and also events with a top quark pair and missing $\mathit E_{T}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV with $\mathit L$ = 20.3 fb${}^{-1}$. See their Figs. 5 and 6 for translated limits on ${{\mathit X}^{0}}$-nucleon cross section for $\mathit m$ = $1 - 700$ GeV.
80  AAD 2015BH search for events with a jet and missing $\mathit E_{T}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV with $\mathit L$ = 20.3 fb${}^{-1}$. See their Fig. 12 for translated limits on ${{\mathit X}^{0}}$-nucleon cross section for $\mathit m$ = $1 - 1200$ GeV.
81  AAD 2015CF search for events with a ${{\mathit H}^{0}}$ ($\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$) and missing $\mathit E_{T}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV with $\mathit L$ = 20.3 fb${}^{-1}$. See paper for limits on the strength of some contact interactions containing ${{\mathit X}^{0}}$ and the Higgs fields.
82  AAD 2015CS search for events with a photon and missing $\mathit E_{T}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV with $\mathit L$ = 20.3 fb${}^{-1}$. See their Fig. 13 (see also erratum) for translated limits on ${{\mathit X}^{0}}$-nucleon cross section for $\mathit m$ = $1 - 1000$ GeV.
83  KHACHATRYAN 2015AG search for events with a top quark pair and missing $\mathit E_{T}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV with $\mathit L$ = 19.7 fb${}^{-1}$. See their Fig. 8 for translated limits on ${{\mathit X}^{0}}$-nucleon cross section for $\mathit m$ = $1 - 200$ GeV.
84  KHACHATRYAN 2015AL search for events with a jet and missing $\mathit E_{T}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV with $\mathit L$ = 19.7 fb${}^{-1}$. See their Fig. 5 and Tables $4 - 6$ for translated limits on ${{\mathit X}^{0}}$-nucleon cross section for $\mathit m$ = $1 - 1000$ GeV.
85  KHACHATRYAN 2015T search for events with a lepton and missing $\mathit E_{T}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV with $\mathit L$ = 19.7 fb${}^{-1}$. See their Fig. 17 for translated limits on ${{\mathit X}^{0}}$-proton cross section for $\mathit m$ = $1 - 1000$ GeV.
86  AAD 2014AI search for events with a ${{\mathit W}}$ and missing $\mathit E_{T}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV with $\mathit L$ = 20.3 fb${}^{-1}$. See their Fig. 4 for translated limits on ${{\mathit X}^{0}}$--nucleon cross section for $\mathit m$ = $1 - 1500$ GeV.
87  AAD 2014BK search for hadronically decaying ${{\mathit W}}$, ${{\mathit Z}}$ in association with $\not E_T$ in 20.3 fb${}^{-1}$ at 8 TeV ${{\mathit p}}{{\mathit p}}$ collisions. Fig. 5 presents exclusion results for SI and SD scattering cross section. In addition, cross section limits on the anomalous production of ${{\mathit W}}$ or ${{\mathit Z}}$ bosons with large missing transverse momentum are also set in two fiducial regions.
88  AAD 2014K search for events with a ${{\mathit Z}}$ and missing $\mathit E_{T}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 8 TeV with $\mathit L$ = 20.3 fb${}^{-1}$. See their Fig. 5 and 6 for translated limits on ${{\mathit X}^{0}}$--nucleon cross section for $\mathit m$ = $1 - 10^{3}$ GeV.
89  AAD 2014O search for ${{\mathit Z}}{{\mathit H}^{0}}$ production with ${{\mathit H}^{0}}$ decaying to invisible final states. See their Fig. 4 for translated limits on ${{\mathit X}^{0}}$--nucleon cross section for $\mathit m$ = $1 - 60$ GeV in Higgs-portal ${{\mathit X}^{0}}$ scenario.
90  AAD 2013AD search for events with a jet and missing $\mathit E_{T}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV with $\mathit L$ = 4.7 fb${}^{-1}$. See their Figs. 5 and 6 for translated limits on ${{\mathit X}^{0}}$-nucleon cross section for $\mathit m$ = $1 - 1300$ GeV.
91  AAD 2013C search for events with a photon and missing $\mathit E_{T}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV with $\mathit L$ = 4.6 fb${}^{-1}$. See their Fig. 3 for translated limits on ${{\mathit X}^{0}}$-nucleon cross section for $\mathit m$ = $1 - 1000$ GeV.
92  AALTONEN 2012K search for events with a top quark and missing $\mathit E_{T}$ in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV with $\mathit L$ = 7.7 fb${}^{-1}$. Upper limits on ${\mathit \sigma (}{{\mathit t}}{{\mathit X}^{0}}{)}$ in the range $0.4 - 2$ pb (95$\%$ CL) is given for ${\mathit m}_{{{\mathit X}^{0}}}$ = $0 - 150$ GeV.
93  AALTONEN 2012M search for events with a jet and missing $\mathit E_{T}$ in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 1.96 TeV with $\mathit L$ = 6.7 fb${}^{-1}$. Upper limits on the cross section in the range $2 - 10~$pb (90$\%$ CL) is given for ${\mathit m}_{{{\mathit X}^{0}}}$ = $1 - 300$ GeV. See their Fig. 2 for translated limits on ${{\mathit X}^{0}}$-nucleon cross section.
94  CHATRCHYAN 2012AP search for events with a jet and missing $\mathit E_{T}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV with $\mathit L$ = 5.0 fb${}^{-1}$. See their Fig. 4 for translated limits on ${{\mathit X}^{0}}$-nucleon cross section for ${\mathit m}_{{{\mathit X}^{0}}}$ = $0.1 - 1000$ GeV.
95  CHATRCHYAN 2012T search for events with a photon and missing $\mathit E_{T}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\mathit E_{{\mathrm {cm}}}$ = 7 TeV with $\mathit L$ = 5.0 fb${}^{-1}$. Upper limits on the cross section in the range $13 - 15~$fb (90$\%$ CL) is given for ${\mathit m}_{{{\mathit X}^{0}}}$ = $1 - 1000$ GeV. See their Fig. 2 for translated limits on ${{\mathit X}^{0}}$-nucleon cross section.
References