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

INSPIRE   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
2022D
 ATLS ${{\mathit Z}}+{{\mathit H}}$ with ${{\mathit H}}$ $\rightarrow$ DM
2
AAD
2022P
 ATLS ${{\mathit H}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit \chi}}$ search via VBF
3
AGUILAR-AR..
2022A
 CCM ${{\mathit p}}$ dump search for MeV-scale DM
4
TUMASYAN
2022AA
 CMS ${{\mathit Z}^{\,'}}$ $\rightarrow$ DM search
5
TUMASYAN
2022AG
 CMS strongly interacting DM search
6
TUMASYAN
2022G
 CMS DM search via VBF to Higgs
7
AAD
2021AZ
 ATLS DM search in ${{\mathit H}}$ $\not E_T$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ $\not E_T$
8
AAD
2021BB
 ATLS DM search in ${{\mathit H}}$ $\not E_T$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ $\not E_T$
9
AAD
2021D
 ATLS Dark Higgs
10
AAD
2021F
 ATLS jet + missing momentum
11
AAD
2021K
 ATLS photon + DM
12
AAD
2021O
 ATLS ${{\mathit \ell}}$ + jets + $\not E_T$ to search for ${{\mathit t}}$-pairs + DM
13
AAD
2021P
 ATLS ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ + jets + $\not E_T$
14
AAD
2021S
 ATLS ${{\mathit b}}$-jets + $\not E_T$
15
SIRUNYAN
2021A
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit \chi}}{{\mathit \chi}}$ ; ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\overline{\mathit \ell}}}$
16
TUMASYAN
2021D
 CMS DM search in jets + $\not E_T$
17
SIRUNYAN
2020X
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit A}}$( ${{\mathit Z}^{\,'}}$) ${{\mathit h}}$ $\rightarrow$ ${{\mathit h}}$ + $\not E_T$
18
AABOUD
2019AA
 ATLS multi-channel BSM search
19
AABOUD
2019AI
 ATLS ${{\mathit H}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit \chi}}$
20
AABOUD
2019AL
 ATLS ${{\mathit H}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit \chi}}$
21
AABOUD
2019Q
 ATLS single ${{\mathit t}}+\not E_T$
22
AABOUD
2019V
 ATLS review mediator based DM searches
23
BANERJEE
2019
NA64 ${{\mathit e}}$ ${{\mathit N}}$ $\rightarrow$ ${{\mathit e}}{{\mathit N}}$ +$\not E$
24
SIRUNYAN
2019AN
 CMS ${{\mathit H}}$ ${{\mathit \chi}}$ ${{\mathit \chi}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ $\not E_T$
25
SIRUNYAN
2019BC
 CMS LQ LQ $\rightarrow$ ${{\mathit \mu}}{{\mathit j}}$ $\not E_T$
26
SIRUNYAN
2019BO
 CMS ${{\mathit V}}$ ${{\mathit V}}$ $\rightarrow$ ${{\mathit H}}{{\mathit q}}{{\mathit q}}$ ; ${{\mathit H}}$ $\rightarrow$ DM
27
SIRUNYAN
2019C
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit t}}}{{\mathit \chi}}{{\mathit \chi}}$
28
SIRUNYAN
2019O
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \gamma}}$ $\not E_T$
29
SIRUNYAN
2019X
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit t}}}$ + $\not\!\!p_T$; ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}$( ${{\overline{\mathit t}}}$) + $\not\!\!p_T$
30
AABOUD
2018
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit \chi}}{{\mathit \chi}}$ ; ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}$
31
AABOUD
2018A
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit t}}}$ $\not E_T$; ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ $\not E_T$
32
AABOUD
2018CA
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit V}}{{\mathit \chi}}{{\mathit \chi}}$ ; ${{\mathit V}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$
33
AABOUD
2018I
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ jet(s) + $\not E_T$
34
AGUILAR-AR..
2018B
 MBNE ${{\mathit p}}$ ${{\mathit N}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit X}}$ , ${{\mathit \chi}}$ = ${{\mathit e}}$, ${{\mathit \pi}}$, or ${{\mathit N}}$
35
KHACHATRYA..
2018
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}$ ( ${{\mathit \ell}}{{\mathit \ell}}$ ) + $\not E_T$
36
SIRUNYAN
2018BF
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}$ $\not E_T$
37
SIRUNYAN
2018BO
 CMS dijet resonance search
38
SIRUNYAN
2018BV
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}$ $\not E_T$
39
SIRUNYAN
2018C
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit t}}}$ $\not E_T$
40
SIRUNYAN
2018CU
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}$ $\not E_T$
41
SIRUNYAN
2018DH
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit \chi}}{{\mathit h}}$ ; ${{\mathit h}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ or ${{\mathit \tau}}{{\overline{\mathit \tau}}}$
42
SIRUNYAN
2018S
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ jets $\not E_T$
43
AABOUD
2017A
 ATLS ${{\mathit p}}{{\mathit p}}$ ( ${{\mathit H}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ + WIMP pair)
44
AABOUD
2017AM
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit A}}{{\mathit h}}$ $\rightarrow$ ${{\mathit h}}$( ${{\mathit b}}{{\overline{\mathit b}}}$) + $\not E_T$
45
AABOUD
2017AQ
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit h}}$( ${{\mathit \gamma}}{{\mathit \gamma}}$) + $\not E_T$
46
AABOUD
2017BD
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ jet(s) + $\not E_T$
47
AABOUD
2017R
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \gamma}}$ $\not E_T$
48
AGUILAR-AR..
2017A
 MBNE ${{\mathit p}}$ ${{\mathit N}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit \chi}}{{\mathit X}}$ ; ${{\mathit \chi}}$ ${{\mathit N}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit N}}$
49
BANERJEE
2017
NA64 ${{\mathit e}}$ ${{\mathit N}}$ $\rightarrow$ ${{\mathit e}}{{\mathit N}}{{\mathit \gamma}^{\,'}}$
50
KHACHATRYA..
2017A
 CMS forward jets + $\not E_T$
51
KHACHATRYA..
2017F
 CMS ${{\mathit H}}$ $\rightarrow$ invisibles
52
SIRUNYAN
2017
CMS ${{\mathit Z}}$ + $\not E_T$
53
SIRUNYAN
2017AP
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit A}}{{\mathit h}}$ $\rightarrow$ ${{\mathit h}}$ + $\not E_T$
54
SIRUNYAN
2017AQ
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \gamma}}$ + $\not E_T$
55
SIRUNYAN
2017BB
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit t}}}$ +$\not E_T$; ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ +$\not E_T$
56
SIRUNYAN
2017G
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}$ + $\not E_T$
57
SIRUNYAN
2017U
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit \chi}}{{\mathit \chi}}$ ; ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\overline{\mathit \ell}}}$
58
AABOUD
2016AD
 ATLS (${{\mathit W}}$ or ${{\mathit Z}}$ $\rightarrow$ jets) + $\not E_T$
59
AAD
2016AF
 ATLS ${{\mathit V}}$ ${{\mathit V}}$ $\rightarrow$ forward jets +$\not E_T$
60
AAD
2016AG
 ATLS ${{\mathit \ell}}$ + jets
61
AAD
2016M
 ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}}$ + $\not E_T$, ${{\mathit H}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$
62
KHACHATRYA..
2016BZ
 CMS jet(s) + $\not E_T$
63
KHACHATRYA..
2016CA
 CMS jets + $\not E_T$
64
KHACHATRYA..
2016N
 CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \gamma}}$ + $\not E_T$
65
AAD
2015AS
 ATLS ${{\mathit b}}$ (${{\overline{\mathit b}}}$) + $\not E_T$, ${{\mathit t}}{{\overline{\mathit t}}}$ + $\not E_T$
66
AAD
2015BH
 ATLS jet + $\not E_T$
67
AAD
2015CF
 ATLS ${{\mathit H}^{0}}$ + $\not E_T$
68
AAD
2015CS
 ATLS ${{\mathit \gamma}}$ + $\not E_T$
69
KHACHATRYA..
2015AG
 CMS ${{\mathit t}}{{\overline{\mathit t}}}$ + $\not E_T$
70
KHACHATRYA..
2015AL
 CMS jet + $\not E_T$
71
KHACHATRYA..
2015T
 CMS ${{\mathit \ell}}$ + $\not E_T$
72
AAD
2014AI
 ATLS ${{\mathit W}}$ + $\not E_T$
73
AAD
2014BK
 ATLS ${{\mathit W}}$, ${{\mathit Z}}$ + $\not E_T$
74
AAD
2014K
 ATLS ${{\mathit Z}}$ + $\not E_T$
75
AAD
2014O
 ATLS ${{\mathit Z}}$ + $\not E_T$
76
AAD
2013AD
 ATLS jet + $\not E_T$
77
AAD
2013C
 ATLS ${{\mathit \gamma}}$ + $\not E_T$
78
AALTONEN
2012K
 CDF ${{\mathit t}}$ + $\not E_T$
79
AALTONEN
2012M
 CDF jet + $\not E_T$
80
CHATRCHYAN
2012AP
 CMS jet + $\not E_T$
81
CHATRCHYAN
2012T
 CMS ${{\mathit \gamma}}$ + $\not E_T$
1  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.
2  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.
3  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.
4  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.
5  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.
6  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.
7  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.
8  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.
9  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 ${{\mathit W}^{\pm}}{{\mathit W}^{\mp}}$ , ${{\mathit Z}}{{\mathit Z}}$ .
10  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.
11  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.
12  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.
13  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.
14  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.
15  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.
16  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.
17  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.
18  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.
19  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).
20  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).
21  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.
22  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 .
23  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.
24  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.
25  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.
26  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.
27  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.
28  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.
29  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.
30  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.
31  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.
32  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; limits set in m(DM) vs m(mediator) simplified model plane .
33  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.
34  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.
35  KHACHATRYAN 2018 search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}$ ( ${{\mathit \ell}}{{\mathit \ell}}$ ) + $\not E_T$ ; no signal ; limits set on effective dark matter interactions and other exotic physics models .
36  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.
37  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.
38  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.
39  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.
40  SIRUNYAN 2018CU search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}$ $\not E_T$ at 13 TeV and 2.3 fb${}^{-1}$; no signal: limits placed for various exotic models including DM .
41  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.
42  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.
43  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.
44  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 $\not E_T$.
45  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 .
46  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.
47  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.
48  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.
49  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.
50  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.
51  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.
52  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.
53  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.
54  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.
55  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.
56  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.
57  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.
58  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.
59  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 .
60  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 $10^{-6} - E-2$.
61  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).
62  KHACHATRYAN 2016BZ search for jet(s) + $\not E_T$ in 19.7 fb${}^{-1}$ at 8 TeV; limits set for variety of simplified models.
63  KHACHATRYAN 2016CA search for WIMPs via jet(s) + $\not E_T$ using razor variable; require mediator scale $>$ 1 TeV for various effective theories.
64  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.
65  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.
66  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.
67  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.
68  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.
69  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.
70  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.
71  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.
72  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.
73  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.
74  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.
75  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.
76  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.
77  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.
78  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.
79  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.
80  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.
81  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:
AAD 2022D
PL B829 137066 Search for associated production of a $Z$ boson with an invisibly decaying Higgs boson or dark matter candidates at $\sqrt s$ =13 TeV with the ATLAS detector
AAD 2022P
JHEP 2208 104 Search for invisible Higgs-boson decays in events with vector-boson fusion signatures using 139 fb$^{-1}$ of proton-proton data recorded by the ATLAS experiment
AGUILAR-AREVALO 2022A
PR D106 012001 First dark matter search results from Coherent CAPTAIN-Mills
TUMASYAN 2022AA
JHEP 2206 156 Search for resonant production of strongly coupled dark matter in proton-proton collisions at 13 TeV
TUMASYAN 2022G
PR D105 092007 Search for invisible decays of the Higgs boson produced via vector boson fusion in proton-proton collisions at $\sqrt{s} =$ 13 TeV
TUMASYAN 2022AG
EPJ C82 213 Search for strongly interacting massive particles generating trackless jets in proton?proton collisions at $\sqrt{s} = 13\,\text {TeV} $
AAD 2021S
JHEP 2105 093 Search for new phenomena in final states with $b$-jets and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector
AAD 2021F
PR D103 112006 Search for new phenomena in events with an energetic jet and missing transverse momentum in $pp$ collisions at $\sqrt {s}$ =13 TeV with the ATLAS detector
AAD 2021K
JHEP 2102 226 Search for dark matter in association with an energetic photon in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector
AAD 2021O
JHEP 2104 174 Search for new phenomena with top quark pairs in final states with one lepton, jets, and missing transverse momentum in $pp$ collisions at $ \sqrt{s} $ = 13 TeV with the ATLAS detector
AAD 2021P
JHEP 2104 165 Search for new phenomena in events with two opposite-charge leptons, jets and missing transverse momentum in pp collisions at $ \sqrt{\mathrm{s}} $ = 13 TeV with the ATLAS detector
AAD 2021AZ
JHEP 2110 013 Search for dark matter in events with missing transverse momentum and a Higgs boson decaying into two photons in pp collisions at $ \sqrt{s} $ = 13 TeV with the ATLAS detector
AAD 2021BB
JHEP 2111 209 Search for dark matter produced in association with a Standard Model Higgs boson decaying into b-quarks using the full Run 2 dataset from the ATLAS detector
AAD 2021D
PRL 126 121802 Search for Dark Matter Produced in Association with a Dark Higgs Boson Decaying into $W^\pm W^\mp$ or $ZZ$ in Fully Hadronic Final States from $\sqrt{s}=13$ TeV pp Collisions Recorded with the ATLAS Detector
SIRUNYAN 2021A
EPJ C81 13 Search for dark matter produced in association with a leptonically decaying Z boson in proton-proton collisions at $\sqrt{s} =$ 13 TeV
Also
EPJ C81 333 (errat.) Search for dark matter produced in association with a leptonically decaying Z boson in proton-proton collisions at $\sqrt{s} =$ 13 TeV
TUMASYAN 2021D
JHEP 2111 153 Search for new particles in events with energetic jets and large missing transverse momentum in proton-proton collisions at $ \sqrt{s} $ = 13 TeV
SIRUNYAN 2020X
JHEP 2003 025 Search for dark matter particles produced in association with a Higgs boson in proton-proton collisions at $ \sqrt{\mathrm{s}} $ = 13 TeV
AABOUD 2019AA
EPJ C79 120 A strategy for a general search for new phenomena using data-derived signal regions and its application within the ATLAS experiment
AABOUD 2019V
JHEP 1905 142 Constraints on mediator-based dark matter and scalar dark energy models using $\sqrt s = 13$ TeV $pp$ collision data collected by the ATLAS detector
AABOUD 2019AI
PL B793 499 Search for invisible Higgs boson decays in vector boson fusion at $\sqrt{s} = 13$ TeV with the ATLAS detector
AABOUD 2019AL
PRL 122 231801 Combination of searches for invisible Higgs boson decays with the ATLAS experiment
AABOUD 2019Q
JHEP 1905 041 Search for large missing transverse momentum in association with one top-quark in proton-proton collisions at $ \sqrt{s} $ = 13 TeV with the ATLAS detector
BANERJEE 2019
PRL 123 121801 Dark matter search in missing energy events with NA64
SIRUNYAN 2019O
JHEP 1902 074 Search for new physics in final states with a single photon and missing transverse momentum in proton-proton collisions at $\sqrt{s} =$ 13 TeV
SIRUNYAN 2019C
PRL 122 011803 Search for dark matter particles produced in association with a top quark pair at $\sqrt{s} =$ 13 TeV
SIRUNYAN 2019BO
PL B793 520 Search for invisible decays of a Higgs boson produced through vector boson fusion in proton-proton collisions at $\sqrt{s} =$ 13 TeV
SIRUNYAN 2019X
JHEP 1903 141 Search for dark matter produced in association with a single top quark or a top quark pair in proton-proton collisions at $ \sqrt{s}=13 $ TeV
SIRUNYAN 2019AN
EPJ C79 280 Search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks in proton?proton collisions at $\sqrt{s}=13\,\text {Te}\text {V} $
SIRUNYAN 2019BC
PL B795 76 Search for dark matter in events with a leptoquark and missing transverse momentum in proton-proton collisions at 13 TeV
AABOUD 2018
PL B776 318 Search for an Invisibly Decaying Higgs Boson or Dark Matter Candidates Produced in Association with a ${{\mathit Z}}$ Boson in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV with the ATLAS Detector
AABOUD 2018I
JHEP 1801 126 Search for Dark Matter and other New Phenomena in Events with an Energetic Jet and Large Missing Transverse Momentum using the ATLAS Detector
AABOUD 2018A
EPJ C78 18 Search for Dark Matter Produced in Association with Bottom or Top Quarks in $\sqrt {s }$ = 13 TeV ${{\mathit p}}{{\mathit p}}$ Collisions with the ATLAS Detector
AABOUD 2018CA
JHEP 1810 180 Search for dark matter in events with a hadronically decaying vector boson and missing transverse momentum in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
AGUILAR-AREVALO 2018B
PR D98 112004 Dark Matter Search in Nucleon, Pion, and Electron Channels from a Proton Beam Dump with MiniBooNE
KHACHATRYAN 2018
PR D97 099903 Search for dark matter and unparticles produced in association with a Z boson in proton-proton collisions at $\sqrt s=$ 8??TeV
SIRUNYAN 2018DH
JHEP 1809 046 Search for dark matter produced in association with a Higgs boson decaying to $\gamma\gamma$ or $\tau^+\tau^-$ at $\sqrt{s} =$ 13 TeV
SIRUNYAN 2018C
PR D97 032009 Search for Top Squarks and Dark Matter Particles in Opposite-Charge Dilepton Final States at $\sqrt {s }$ = 13 TeV
SIRUNYAN 2018BF
JHEP 1806 027 Search for dark matter in events with energetic, hadronically decaying top quarks and missing transverse momentum at $ \sqrt{s}=13 $ TeV
SIRUNYAN 2018BO
JHEP 1808 130 Search for narrow and broad dijet resonances in proton-proton collisions at $ \sqrt{s}=13 $ TeV and constraints on dark matter mediators and other new particles
SIRUNYAN 2018BV
EPJ C78 291 Search for new physics in events with a leptonically decaying Z boson and a large transverse momentum imbalance in proton?proton collisions at $\sqrt{s} $ = 13 $\,\text {TeV}$
SIRUNYAN 2018CU
JHEP 1801 056 Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at $ \sqrt{s}=13 $ TeV
SIRUNYAN 2018S
PR D97 092005 Search for new physics in final states with an energetic jet or a hadronically decaying $W$ or $Z$ boson and transverse momentum imbalance at $\sqrt{s}=13\text{ }\text{ }\mathrm{TeV}$
AABOUD 2017R
EPJ C77 393 Search for Dark Matter at $\sqrt {s }$ = 13 TeV in Final States Containing an Energetic Photon and Large Missing Transverse Momentum with the ATLAS Detector
AABOUD 2017BD
EPJ C77 765 Measurement of Detector-Corrected Observables Sensitive to the Anomalous Production of Events with Jets and Large Missing Transverse Momentum in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV using the ATLAS Detector
AABOUD 2017A
PL B765 11 Search for Dark Matter in Association with a Higgs Boson Decaying to ${\mathit {\mathit b}}$-Quarks in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV with the ATLAS Detector
AABOUD 2017AM
PRL 119 181804 Search for Dark Matter Produced in Association with a Higgs Boson Decaying to ${\mathit {\mathit b}}{\mathit {\overline{\mathit b}}}$ using 36 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$=13 TeV with the ATLAS Detector
AABOUD 2017AQ
PR D96 112004 Search for Dark Matter in Association with a Higgs Boson Decaying to Two Photons at $\sqrt {s }$ = 13 TeV with the ATLAS Detector
AGUILAR-AREVALO 2017A
PRL 118 221803 Dark Matter Search in a Proton Beam Dump with MiniBooNE
BANERJEE 2017
PRL 118 011802 Search for Invisible Decays of sub-GeV Dark Photons in Missing-Energy Events at the CERN SPS
KHACHATRYAN 2017A
PRL 118 021802 Search for Dark Matter and Supersymmetry with a Compressed Mass Spectrum in the Vector Boson Fusion Topology in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
KHACHATRYAN 2017F
JHEP 1702 135 Searches for Invisible Decays of the Higgs Boson in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7, 8, and 13 TeV
SIRUNYAN 2017AQ
JHEP 1710 073 Search for New Physics in the Monophoton Final State in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV
SIRUNYAN 2017G
JHEP 1707 014 Search for Dark Matter Produced with an Energetic Jet or a Hadronically Decaying ${{\mathit W}}$ or ${{\mathit Z}}$ Boson at $\sqrt {s }$ = 13 TeV
SIRUNYAN 2017
JHEP 1703 061 Search for Dark Matter and Unparticles in Events with a ${{\mathit Z}}$ Boson and Missing Transverse Momentum in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV
SIRUNYAN 2017AP
JHEP 1710 180 Search for Associated Production of Dark Matter with a Higgs Boson Decaying to ${\mathit {\mathit b}}{\mathit {\overline{\mathit b}}}$ or ${{\mathit \gamma}}{{\mathit \gamma}}$ at $\sqrt {s }$ = 13 TeV
SIRUNYAN 2017BB
EPJ C77 845 Search for Dark Matter Produced in Association with Heavy-Flavor Quark Pairs in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV
SIRUNYAN 2017U
JHEP 1709 106 Search for Dark Matter and Unparticles in Events with a ${{\mathit Z}}$ Boson and Missing Transverse Momentum in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV
AABOUD 2016AD
PL B763 251 Search for Dark Matter Produced in Association with a Hadronically Decaying Vector Boson in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV with the ATLAS Detector
AAD 2016AF
JHEP 1601 172 Search for Invisible Decays of a Higgs Boson using Vector-Boson Fusion in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
AAD 2016M
PR D93 072007 Search for Dark Matter Produced in Association with a Higgs Boson Decaying to Two Bottom Quarks in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
AAD 2016AG
JHEP 1602 062 A Search for Prompt Lepton-Jets in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
KHACHATRYAN 2016BZ
JHEP 1612 083 Search for Dark Matter in Proton-Proton Collisions at 8 TeV with Missing Transverse Momentum and Vector Boson Tagged Jets
Also
JHEP 1708 035 (errat.) Erratum to KHACHATRYAN 2016BZ: Search for Dark Matter in Proton-Proton Collisions at 8 TeV with Missing Transverse Momentum and Vector Boson Tagged Jets
KHACHATRYAN 2016N
PL B755 102 Search for New Phenomena in Monophoton Final States in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
KHACHATRYAN 2016CA
JHEP 1612 088 Search for Dark Matter Particles in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV using the Razor Variables
AAD 2015AS
EPJ C75 92 Search for Dark Matter in Events with Heavy Quarks and Missing Transverse Momentum in ${{\mathit p}}{{\mathit p}}$ Collisions with the ATLAS Detector
AAD 2015CS
PR D91 012008 Search for New Phenomena in Events with a Photon and Missing Transverse Momentum in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
Also
PR D92 059903 (errat.) Erratum to AAD 2015CS: Search for New Phenomena in Events with a Photon and Missing Transverse Momentum in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
AAD 2015BH
EPJ C75 299 Search for New Phenomena in Final States with an Energetic Jet and Large Missing Transverse Momentum in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
Also
EPJ C75 408 (errat.) Erratum to AAD 2015BH. Search for New Phenomena in Final States with an Energetic Jet and Large Missing Transverse Momentum in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
AAD 2015CF
PRL 115 131801 Search for Dark Matter in Events with Missing Transverse Momentum and a Higgs Boson Decaying to Two Photons in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
KHACHATRYAN 2015AG
JHEP 1506 121 Search for the Production of Dark Matter in Association with Top-Quark Pairs in the Single-Lepton Final State in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
KHACHATRYAN 2015AL
EPJ C75 235 Search for Dark Matter, Extra Dimensions, and Unparticles in Monojet Events in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
KHACHATRYAN 2015T
PR D91 092005 Search for Physics Beyond the Standard Model in Final States with a Lepton and Missing Transverse Energy in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
AAD 2014BK
PRL 112 041802 Search for Dark Matter in Events with a Hadronically Decaying ${{\mathit W}}$ or ${{\mathit Z}}$ Boson and Missing Transverse Momentum in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
AAD 2014O
PRL 112 201802 Search for Invisible Decays of a Higgs Boson Produced in Association with a ${{\mathit Z}}$ Boson in ATLAS
AAD 2014AI
JHEP 1409 037 Search for New Particles in Events with one Lepton and Missing Transverse Momentum in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS detector
AAD 2014K
PR D90 012004 Search for Dark Matter in Events with a ${{\mathit Z}}$ Boson and Missing Transverse Momentum in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
AAD 2013C
PRL 110 011802 Search for Dark Matter Candidates and Large Extra Dimensions in Events with a Photon and Missing Transverse Momentum in ${{\mathit p}}{{\mathit p}}$ Collision Data at $\sqrt {s }$ = 7 TeV with the ATLAS Detector
AAD 2013AD
JHEP 1304 075 Search for Dark Matter Candidates and Large Extra Dimensions in Events with a Jet and Missing Transverse Momentum with the ATLAS Detector
AALTONEN 2012K
PRL 108 201802 Search for a Dark Matter Candidate Produced in Association with a Single Top Quark in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV
AALTONEN 2012M
PRL 108 211804 Search for Dark Matter in Events with One Jet and Missing Transverse Energy in ${{\mathit p}}{{\overline{\mathit p}}}$ Collisions at $\sqrt {s }$ = 1.96 TeV
CHATRCHYAN 2012AP
JHEP 1209 094 Search for Dark Matter and Large Extra Dimensions in Monojet Events in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV
CHATRCHYAN 2012T
PRL 108 261803 Search for Dark Matter and Large Extra Dimensions in ${{\mathit p}}{{\mathit p}}$ Collisions Yielding a Photon and Missing Transverse Energy