# Dark Matter Particle (${{\boldsymbol X}^{0}}$) Production in Hadron Collisions INSPIRE search

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
 2018
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit \chi}}{{\mathit \chi}}$ ; ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \ell}}$
2
 2018 A
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit t}}}$ $\not E_T$; ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ $\not E_T$
3
 2018 I
ATLS jet(s) + $\not E_T$
4
 2018 C
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit t}}}$ $\not E_T$
5
 2017 A
ATLS ${{\mathit p}}{{\mathit p}}$ ( ${{\mathit H}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ + WIMP pair)
6
 2017 AM
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit A}}{{\mathit h}}$ $\rightarrow$ ${{\mathit h}}$( ${{\mathit b}}{{\overline{\mathit b}}}$) + $\not E_T$
7
 2017 AQ
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit h}}$( ${{\mathit \gamma}}{{\mathit \gamma}}$) + $\not E_T$
8
 2017 BD
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ jet(s) + $\not E_T$
9
 2017 R
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \gamma}}$ $\not E_T$
10
 2017 A
MBNE ${{\mathit p}}$ ${{\mathit N}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit \chi}}{{\mathit X}}$ ; ${{\mathit \chi}}$ ${{\mathit N}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit N}}$
11
 2017
NA64 ${{\mathit e}}$ ${{\mathit N}}$ $\rightarrow$ ${{\mathit e}}{{\mathit N}}{{\mathit \gamma}^{\,'}}$
12
 2017 A
CMS forward jets + $\not E_T$
13
 2017 F
CMS ${{\mathit H}}$ $\rightarrow$ invisibles
14
 2017
CMS ${{\mathit Z}}$ + $\not E_T$
15
 2017 AP
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit A}}{{\mathit h}}$ $\rightarrow$ ${{\mathit h}}$ +MET
16
 2017 AQ
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \gamma}}$ +MET
17
 2017 BB
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit t}}{{\overline{\mathit t}}}$ +$\not E_T$; ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ +$\not E_T$
18
 2017 G
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}$ + $\not E_T$
19
 2017 U
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}}{{\mathit \chi}}{{\mathit \chi}}$ ; ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \ell}}{{\overline{\mathit \ell}}}$
20
ATLS (${{\mathit W}}$ or ${{\mathit Z}}$ $\rightarrow$ jets) + $\not E_T$
21
 2016 AF
ATLS ${{\mathit V}}$ ${{\mathit V}}$ $\rightarrow$ forward jets +$\not E_T$
22
 2016 AG
ATLS ${{\mathit \ell}}$ + jets
23
 2016 M
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit H}}$ + $\not E_T$, ${{\mathit H}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$
24
 2016 BZ
CMS jet(s) + $\not E_T$
25
 2016 CA
CMS jets + $\not E_T$
26
 2016 N
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \gamma}}$ + $\not E_T$
27
 2015 AS
ATLS ${{\mathit b}}$ (${{\overline{\mathit b}}}$) + $\not E_T$, ${{\mathit t}}{{\overline{\mathit t}}}$ + $\not E_T$
28
 2015 BH
ATLS jet + $\not E_T$
29
 2015 CF
ATLS ${{\mathit H}^{0}}$ + $\not E_T$
30
 2015 CS
ATLS ${{\mathit \gamma}}$ + $\not E_T$
31
 2015 AG
CMS ${{\mathit t}}{{\overline{\mathit t}}}$ + $\not E_T$
32
 2015 AL
CMS jet + $\not E_T$
33
 2015 T
CMS ${{\mathit \ell}}$ + $\not E_T$
34
 2014 AI
ATLS ${{\mathit W}}$ + $\not E_T$
35
 2014 BK
ATLS ${{\mathit W}}$, ${{\mathit Z}}$ + $\not E_T$
36
 2014 K
ATLS ${{\mathit Z}}$ + $\not E_T$
37
 2014 O
ATLS ${{\mathit Z}}$ + $\not E_T$
38
ATLS jet + $\not E_T$
39
 2013 C
ATLS ${{\mathit \gamma}}$ + $\not E_T$
40
 2012 K
CDF ${{\mathit t}}$ + $\not E_T$
41
 2012 M
CDF jet + $\not E_T$
42
 2012 AP
CMS jet + $\not E_T$
43
 2012 T
CMS ${{\mathit \gamma}}$ + $\not E_T$
1  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.
2  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.
3  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.
4  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.
5  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.
6  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 $\not E_T$.
7  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 .
8  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.
9  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.
10  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.
11  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.
12  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.
13  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.
14  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.
15  SIRUNYAN 2017AP search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit A}}{{\mathit h}}$ $\rightarrow$ ${{\mathit h}}$ +MET 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.
16  SIRUNYAN 2017AQ search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \gamma}}$ +MET at 13 TeV with 12.9 fb${}^{-1}$. Limits derived for simplified DM models, effective electroweak-DM interaction and Extra Dimensions models.
17  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.
18  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.
19  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.
20  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.
21  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 .
22  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 .
23  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).
24  KHACHATRYAN 2016BZ search for jet(s) + $\not E_T$ in 19.7 fb${}^{-1}$ at 8 TeV; limits set for variety of simplified models.
25  KHACHATRYAN 2016CA search for WIMPs via jet(s) + $\not E_T$ using razor variable; require mediator scale $>$ 1 TeV for various effective theories.
26  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.
27  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.
28  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.
29  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.
30  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.
31  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.
32  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.
33  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.
34  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.
35  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.
36  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.
37  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.
38  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.
39  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.
40  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.
41  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.
42  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.
43  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:
 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 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 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
 SIRUNYAN 2018C
PR D97 032009 Search for Top Squarks and Dark Matter Particles in Opposite-Charge Dilepton Final States at $\sqrt {s }$ = 13 TeV
 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 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
 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 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 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
 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 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
 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
 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
 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 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
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
JHEP 1602 062 A Search for Prompt Lepton-Jets in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
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
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
 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
 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
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
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
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
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
 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 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 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
PRL 112 201802 Search for Invisible Decays of a Higgs Boson Produced in Association with a ${{\mathit Z}}$ Boson in ATLAS
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
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
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
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
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
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
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
PRL 108 261803 Search for Dark Matter and Large Extra Dimensions in ${{\mathit p}}{{\mathit p}}$ Collisions Yielding a Photon and Missing Transverse Energy
PR D96 112003 Measurement of Charged Pion, Kaon, and Proton Production in Proton-Proton Collisions at $\sqrt {s }$ = 13 TeV