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1
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.
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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).
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3
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).
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4
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.
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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 .
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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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 .
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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.
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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.
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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 .
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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.
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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.
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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.
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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.
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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 .
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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.
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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.
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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.
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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 $\not E_T$.
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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 .
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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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 .
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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 .
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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).
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KHACHATRYAN 2016BZ search for jet(s) + $\not E_T$ in 19.7 fb${}^{-1}$ at 8 TeV; limits set for variety of simplified models.
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KHACHATRYAN 2016CA search for WIMPs via jet(s) + $\not E_T$ using razor variable; require mediator scale $>$ 1 TeV for various effective theories.
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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.
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48
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.
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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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.
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