LIMITS ON NEUTRAL PARTICLE PRODUCTION

ATLS

${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \mu}}$ $/$ ${{\mathit e}}{{\mathit \tau}}$ $/$ ${{\mathit \mu}}{{\mathit \tau}}$

²⁵

LHCB

${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit A}^{\,'}}$ $\rightarrow$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$; dark photon

²⁶

NA64

${{\mathit e}}$ ${{\mathit Z}}$ $\rightarrow$ ${{\mathit e}}{{\mathit Z}}{{\mathit X}}$( ${{\mathit A}^{\,'}}$)

²⁷

NA64

${{\mathit e}}$ ${{\mathit Z}}$ $\rightarrow$ ${{\mathit e}}{{\mathit Z}}{{\mathit A}^{\,'}}$, ${{\mathit A}^{\,'}}$ $\rightarrow$ ${{\mathit \chi}}{{\mathit \chi}}$

²⁸

MARSICANO

E137

${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit A}^{\,'}}$( ${{\mathit \gamma}}$) visible decay

²⁹

CMS

${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit Z}^{\,'}}$ $\rightarrow$ ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$ at 13 TeV

³⁰

CMS

${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ Black Hole, string ball, sphaleron

³¹

CMS

${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$

³²

CMS

${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit b}}{{\mathit \mu}}{{\overline{\mathit \mu}}}$

³³

CMS

${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$

³⁴

CMS

${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit V}}$ $\rightarrow$ ${{\mathit W}}{{\mathit h}}$; ${{\mathit h}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$; ${{\mathit W}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$

³⁵

2017

ATLS

${{\mathit W}}{{\mathit H}}$, ${{\mathit Z}}{{\mathit H}}$ resonance

³⁶

2017

LHCB

${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \pi}_{{{v}}}}{{\mathit \pi}_{{{v}}}}$, ${{\mathit \pi}_{{{v}}}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$

³⁷

ATLS

${{\mathit \ell}}$ + (${{\mathit \ell}}$s or jets)

³⁸

ATLS

${{\mathit W}}{{\mathit W}}$ , ${{\mathit W}}{{\mathit Z}}$ , ${{\mathit Z}}{{\mathit Z}}$ resonance

³⁹

KRASZNAHORKAY

${{\mathit p}}$ ${}^{7}\mathrm {Li}$ $\rightarrow$ ${}^{8}\mathrm {Be}$ $\rightarrow$ ${{\mathit X}{(17)}}{{\mathit N}}$ , ${{\mathit X}{(17)}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$

⁴⁰

LEES

2015

BABR

${{\mathit e}^{+}}{{\mathit e}^{-}}$ collisions

⁴¹

ADAMS

1997

KTEV

$\mathit m$= $1.2 - 5$ GeV

$<10^{-36} - 10^{-33}$

⁴²

GALLAS

1995

TOF

$\mathit m$= $0.5 - 20$ GeV

$<(4 - 0.3){\times }\text{ 10^}{-31}$

⁴³

AKESSON

1991

CNTR

$\mathit m$ = $0 - 5$ GeV

$<2 \times 10^{-36}$

⁴⁴

BADIER

1986

BDMP

$\tau $ = (0.05$-1.){\times }10^{-8}$s

$<2.5 \times 10^{-35}$

⁴⁵

GUSTAFSON

1976

CNTR

$\tau $ $>10^{-7}$ s

¹ AFANACIEV 2025 report on search for ${}^{8}\mathrm {Be}{}^{*}$ emission of ${{\mathit X}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ at MEG-II. No signal observed. Limits placed in m(${{\mathit e}^{+}}{{\mathit e}^{-}}$) vs. branching fraction plane.

² ALRAHMAN 2025 report on search for neutral long-lived particle (${{\mathit S}}$) produced from ${{\mathit K}}$ decay but decaying ${{\mathit S}}$ $\rightarrow$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ at ICARUS experiment at Fermilab. No signal observed. Limits placed in mass vs.coupling plane for axion and Higgs portal models.

³ HAYRAPETYAN 2025O search for long-lived heavy neutral leptons at CMS with 138 fb${}^{-1}$using displaced lepton plus jet. No signal observed. Limits placed in lepton mixing angle vs mass plane for masses in the range of $1.0 - 16.5$ GeV.

⁴ AAD 2024AE search for heavy vector triplet production with decay to boson pairs. No signal was observed. Limits placed in ${{\mathit \sigma}}$ vs m plane. Limits also placed in various two-dimensional coupling planes (${{\mathit g}_{{{F}}}}$, ${{\mathit g}_{{{H}}}}$, ${{\mathit g}_{{{{{\mathit \ell}}}}}}$, ${{\mathit g}_{{{{{\mathit \ell}}}}}}$(3rd Gen), ${{\mathit g}_{{{q}}}}$, ${{\mathit g}_{{{q}}}}$(3rd Gen), ${{\mathit g}_{{{q}}}}$(1st/2nd Gen)).

⁵ AAD 2024BV search for VBF di-Higgs production with decay to boosted 4${{\mathit b}}$ state. No signal observed. Limits placed in mass vs. cross section plane for various simplified models.

⁶ AAD 2024CD search for hadronically-decaying ${{\mathit W}}$ $/$ ${{\mathit Z}}$ + MET events from new physics with 140 fb${}^{-1}$ at 13 TeV. No signal observed. Limits placed on various simplified new physics models.

⁷ AAD 2024E uses a new resonance search technique for two-body decays into any pair of ${{\mathit \ell}}$, ${{\mathit b}}$, and jet with 140 fb${}^{-1}$ of data. No signal was observed. Limits placed in ${{\mathit \sigma}}$ vs mass plane for various decay modes.

⁸ AAD 2024S search for quantum black hole (QBH) decay to lepton + jet in 140 fb${}^{-1}$ of data. No signal observed. Limits placed in ${{\mathit \sigma}}\cdot{}$BF vs mass plane for ADD and RS models.

⁹ HAYRAPETYAN 2024AB search for heavy neutral leptons ${{\mathit N}}$ at CMS with 138 fb${}^{-1}$ of data. No signal observed. Limits placed in mixing angle vs m(${{\mathit N}}$) plane.

¹⁰ HAYRAPETYAN 2024AC search for heavy long-lived neutrino ${{\mathit N}}$ produced in ${{\mathit B}}$-decays in 41.6 fb${}^{-1}$ of data. No signal observed. Limits placed in mixing angle vs m(${{\mathit N}}$) plane.

¹¹ HAYRAPETYAN 2024AZ search for various new bosons via production and decay to four muon states with 41.5 and 59.7 fb${}^{-1}$ of data at 13 TeV. No signal observed. Limits placed usually in mass vs. cross section plane for a variety of new physics simplified models.

¹² AAD 2023P search in 22 channels for exotica produced in association with ${{\mathit h}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ in 139 fb${}^{-1}$ of data. No signal observed. Limits placed on production cross section in various channels.

¹³ TUMASYAN 2023BC search for ${{\mathit \gamma}}$-jet resonance at CMS with 138 fb${}^{-1}$ of data. No signal observed. Limits placed on quantum black hole and excited quark models.

¹⁴ TUMASYAN 2023BF search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit p}}{{\mathit p}}{+}$ ${{\mathit \gamma}}$ $/$ ${{\mathit Z}}{+}$ ${{\mathit X}}$ search where ${{\mathit X}}$ is missing particle using CMS-TOTEM with 37.2 fb${}^{-1}$ of data. No signal observed. Limits placed on ${{\mathit \sigma}}$ vs. m plane.

¹⁵ TUMASYAN 2022AG search for strongly interacting neutral massive particles via trackless jets with 16.1 fb${}^{-1}$ at 13 TeV; no signal detected; limits placed in mass vs. cross section plane for various simplified models.

¹⁶ AAD 2021F search for hard monojet production at ATLAS with 139 ${}^{-1}$ of 13 TeV data. No signal observed. Limits placed on invisible production cross-section recoiling against ISR and interpreted in variety of BSM models.

¹⁷ AAIJ 2020AL search for dimuon resonance from promptly decaying ${{\mathit X}}$ particle. No signal detected. Limits placed on m(${{\mathit X}}$) up to 60 GeV depending on mixing in 2HDM.

¹⁸ SIRUNYAN 2020AY measured ${{\mathit \Upsilon}}$(1S) pair production cross section and searched for new states decaying into ${{\mathit \Upsilon}{(1S)}}{{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ at CMS with 13 TeV with 35.9 fb${}^{-1}$. No signal is found and limits are set in ${{\mathit \sigma}}\cdot{}$BF vs. mass plane for tetra-${{\mathit b}}$-quarks with masses between 17.5 and 19 GeV and for generic search for narrow resonances with mass between 16.5 and 27 GeV.

¹⁹ SIRUNYAN 2020Z search for BSM physics via multilepton production with CMS at 13 TeV with 137 fb${}^{-1}$; no signal is found and limits are set on type-III seesaw and other BSM models.

²⁰ AABOUD 2019H searches for di-photon-jet resonance at 13 TeV and 36.7 fb${}^{-1}$ of data; no signal found and limits placed on ${{\mathit \sigma}}\cdot{}$BR vs. mass plane for various simplified models.

²¹ AABOUD 2019V review ATLAS searches for mediator-based DM at 7, 8, and 13 TeV with up to 37 fb${}^{-1}$ of data; no signal found and limits set for wide variety of simplified models of dark matter.

²² SIRUNYAN 2019O search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \gamma}}$ $\not E_T$ at 13 TeV with 36.1 fb${}^{-1}$; no signal found and limits set for various simplified models.

²³ AABOUD 2018CJ make multichannel search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit V}}{{\mathit V}}$ $/$ ${{\mathit \ell}}{{\mathit \ell}}$ $/$ ${{\mathit \ell}}{{\mathit \nu}}$, ${{\mathit V}}$ = ${{\mathit W}},{{\mathit Z}},{{\mathit h}}$ at 13 TeV, 36.1 fb${}^{-1}$; no signal found; limits placed for several BSM models.

²⁴ AABOUD 2018CM search for lepton-flavor violating resonance in ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \mu}}$ $/$ ${{\mathit e}}{{\mathit \tau}}$ $/$ ${{\mathit \mu}}{{\mathit \tau}}$ at 13 TeV, 36.1 fb${}^{-1}$; no signal is found and limits placed for various BSM models.

²⁵ AAIJ 2018AJ search for prompt and delayed dark photon decay ${{\mathit A}^{\,'}}$ $\rightarrow$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ at LHCb detector using 1.6 fb${}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ collisions at 13 TeV; limits on m(${{\mathit A}^{\,'}}$) vs. kinetic mixing are set.

²⁶ BANERJEE 2018 search for dark photon ${{\mathit A}^{\,'}}$/16.7 MeV boson ${{\mathit X}}$ at NA64 via ${{\mathit e}}$ ${{\mathit Z}}$ $\rightarrow$ ${{\mathit e}}{{\mathit Z}}{{\mathit X}}$( ${{\mathit A}^{\,'}}$); no signal found and limits set on the ${{\mathit X}}-{{\mathit e}^{-}}$ coupling ${{\mathit \epsilon}_{{{e}}}}$ in the range $1.3 \times 10^{-4}{}\leq{}{{\mathit \epsilon}_{{{e}}}}{}\leq{}4.2 \times 10^{-4}$ excluding part of the allowed parameter space.

²⁷ BANERJEE 2018A search for invisibly decaying dark photons in ${{\mathit e}}$ ${{\mathit Z}}$ $\rightarrow$ ${{\mathit e}}{{\mathit Z}}{{\mathit A}^{\,'}}$, ${{\mathit A}^{\,'}}$ $\rightarrow$invisible; no signal found and limits set on mixing for m(${{\mathit A}^{\,'}}$) $<$ 1 GeV.

²⁸ MARSICANO 2018 search for dark photon ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit A}^{\,'}}$( ${{\mathit \gamma}}$) visible decay in SLAC E137 ${{\mathit e}}$ beam dump data. No signal observed and limits set in ${{\mathit \epsilon}}$ coupling vs m(${{\mathit A}^{\,'}}$) plane, see their figure 7.

²⁹ SIRUNYAN 2018BB search for high mass dilepton resonance; no signal found and exclude portions of p-space of ${{\mathit Z}^{\,'}}$, KK graviton models.

³⁰ SIRUNYAN 2018DA search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ Black Hole, string ball, sphaleron via high multiplicity events at 13 TeV, 35.9 fb${}^{-1}$; no signal, require e.g. m(BH) $>$ 10.1 TeV.

³¹ SIRUNYAN 2018DD search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$ deviations in dijet angular distribution. No signal observed. Set limits on large extra dimensions, black holes and DM mediators e.g. m(BH) $>$ $5.9 - 8.2$ TeV.

³² SIRUNYAN 2018DR search for dimuon resonance in ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit b}}{{\mathit \mu}}{{\overline{\mathit \mu}}}$ at 8 and 13 TeV. Slight excess seen at m(${{\mathit \mu}}{{\overline{\mathit \mu}}}$) $\sim{}$ 28 GeV in some channels.

³³ SIRUNYAN 2018DU search for high mass diphoton resonance in ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \gamma}}$ at 13 TeV using 35.9 fb${}^{-1}$; no signal; limits placed on RS Graviton, LED, and clockwork.

³⁴ SIRUNYAN 2018ED search for ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit V}}$ $\rightarrow$ ${{\mathit W}}{{\mathit h}}$; ${{\mathit h}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$; ${{\mathit W}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit \nu}}$ at 13 TeV with 35.9 fb${}^{-1}$; no signal; limits set on m(${{\mathit W}^{\,'}}$) $>$ 2.9 TeV.

³⁵ AABOUD 2017B exclude m(${{\mathit W}^{\,'}}$, ${{\mathit Z}^{\,'}}$) $<1.49 - 2.31$ TeV depending on the couplings and ${{\mathit W}^{\,'}}/{{\mathit Z}^{\,'}}$ degeneracy assumptions via ${{\mathit W}}{{\mathit H}}$, ${{\mathit Z}}{{\mathit H}}$ search in ${{\mathit p}}{{\mathit p}}$ collisions at 13 TeV with 3.2$~$fb${}^{-1}$ of data.

³⁶ AAIJ 2017BR search for long-lived hidden valley pions from Higgs decay. Limits are set on the signal strength as a function of the mass and lifetime of the long-lived particle in their Fig. 4 and Tab. 4.

³⁷ AAD 2016O search for high $\mathit E_{T}$ ${{\mathit \ell}}$ + (${{\mathit \ell}}$s or jets) with 3.2 fb${}^{-1}$ at 13 TeV; exclude micro black holes mass $<$ 8 TeV (Fig. 3) for models with two extra dimensions.

³⁸ AAD 2016R search for ${{\mathit W}}{{\mathit W}}$, ${{\mathit W}}{{\mathit Z}}$, resonance in 20.3 fb${}^{-1}$ at 8 TeV data; limits placed on massive RS graviton (Fig. 4).

³⁹ KRASZNAHORKAY 2016 report ${{\mathit p}}$ ${}^{7}{}^{}\mathrm {Li}$ $\rightarrow$ ${}^{8}{}^{}\mathrm {Be}$ ${{\mathit e}}{{\overline{\mathit e}}}$ ${{\mathit N}}$ 5${{\mathit \sigma}}$ resonance at 16.7 MeV-- possible evidence for nuclear interference or new light boson. However, such nuclear interference was ruled out already by ZANG 2017.

⁴⁰ LEES 2015E search for long-lived neutral particles produced in ${{\mathit e}^{+}}{{\mathit e}^{-}}$ collisions in the Upsilon region, which decays into ${{\mathit e}^{+}}{{\mathit e}^{-}}$, ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$, ${{\mathit e}^{\pm}}{{\mathit \mu}^{\mp}}$, ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$, ${{\mathit K}^{+}}{{\mathit K}^{-}}$, or ${{\mathit \pi}^{\pm}}{{\mathit K}^{\mp}}$. See their Fig. 2 for cross section limits.

⁴¹ ADAMS 1997B search for a hadron-like neutral particle produced in ${{\mathit p}}{{\mathit N}}$ interactions, which decays into a ${{\mathit \rho}^{0}}$ and a weakly interacting massive particle. Upper limits are given for the ratio to ${{\mathit K}_{{{L}}}}~$production for the mass range $1.2 - 5$ GeV and lifetime $10^{-9} - 10^{-4}~$s. See also our Light Gluino Section.

⁴² GALLAS 1995 limit is for a weakly interacting neutral particle produced in 800 GeV/$\mathit c$ ${{\mathit p}}{{\mathit N}}$ interactions decaying with a lifetime of $10^{-4} - 10^{-8}~$s. See their Figs.$~$8 and 9. Similar limits are obtained for a stable particle with interaction cross section $10^{-29} - 10^{-33}$ cm${}^{2}$. See Fig.$~$10.

⁴³ AKESSON 1991 limit is from weakly interacting neutral long-lived particles produced in ${{\mathit p}}{{\mathit N}}$ reaction at 450 GeV/$\mathit c$ performed at CERN$~$SPS. Bourquin-Gaillard formula is used as the production model. The above limit is for $\tau ~>~10^{-7}~$s. For $\tau ~>~10^{-9}~$s, $\sigma ~<~10^{-30}~$cm${}^{−2}$/nucleon is obtained.

⁴⁴ BADIER 1986 looked for long-lived particles at 300 GeV ${{\mathit \pi}^{-}}$ beam dump. The limit applies for nonstrongly interacting neutral or charged particles with mass $>$2 GeV. The limit applies for particle modes, ${{\mathit \mu}^{+}}{{\mathit \pi}^{-}}$, ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$, ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ X, ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{\pm}}$ etc. See their figure 5 for the contours of limits in the mass-$\tau $ plane for each mode.

⁴⁵ GUSTAFSON 1976 is a 300 GeV FNAL experiment looking for heavy ($\mathit m$ $>$2 GeV) long-lived neutral hadrons in the M4 neutral beam. The above typical value is for $\mathit m$ = 3 GeV and assumes an interaction cross section of 1 mb. Values as a function of mass and interaction cross section are given in figure 2.

References:

AFANACIEV

2025

EPJ C85 763

Search for the X17 particle in $^{7}\mathrm{Li}(\mathrm{p},\mathrm{e}^+ \mathrm{e}^{-}) ^{8}\mathrm{Be}$ processes with the MEG II detector

ALRAHMAN

2025

PRL 134 151801

Search for a Hidden Sector Scalar from Kaon Decay in the Di-Muon Final State at ICARUS

2025O

JHEP 2502 036

Search for long-lived heavy neutral leptons in proton-proton collision events with a lepton-jet pair associated with a secondary vertex at $\sqrt{s}$ = 13 TeV

2024CD

JHEP 2411 126

Search for new particles in events with a hadronically decaying W or Z boson and large missing transverse momentum at $\sqrt{s}$ = 13 TeV using the ATLAS detector

2024AE

JHEP 2404 118

Combination of searches for heavy spin-1 resonances using 139 fb$^{-1}$ of proton-proton collision data at $\sqrt{s} = 13$ TeV with the ATLAS detector

2024S

PR D109 032010

Search for quantum black hole production in lepton+jet final states using proton-proton collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector

2024E

PRL 132 081801

Search for new phenomena in two-body invariant mass distributions using unsupervised machine learning for anomaly detection at $\sqrt{s} = 13$ TeV with the ATLAS detector

2024BV

PL B858 139007

Search for pair production of boosted Higgs bosons via vector-boson fusion in the $b\bar{b}b\bar{b}$ final state using $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector

2024AC

JHEP 2406 183

Search for long-lived heavy neutrinos in the decays of B mesons produced in proton-proton collisions at $\sqrt{s}$ = 13 TeV

2024AZ

JHEP 2412 172

Model-independent search for pair production of new bosons decaying into muons in proton-proton collisions at $\sqrt{s}$ = 13 TeV

2024AB

JHEP 2406 123

Search for heavy neutral leptons in final states with electrons, muons, and hadronically decaying tau leptons in proton-proton collisions at $\sqrt{s}$ =13 TeV

2023P

JHEP 2307 176

Model-independent search for the presence of new physics in events including $H\rightarrow\gamma\gamma$ with $\sqrt{s}$ = 13 TeV pp data recorded by the ATLAS detector at the LHC

TUMASYAN

2023BF

EPJ C83 827

A search for new physics in central exclusive production using the missing mass technique with the CMS detector and the CMS-TOTEM precision proton spectrometer

TUMASYAN

2023BC

JHEP 2312 189

Search for resonances in events with photon and jet final states 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} $

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

2020AL

JHEP 2010 156

Searches for low-mass dimuon resonances

2020Z

JHEP 2003 051

Search for physics beyond the standard model in multilepton final states in proton-proton collisions at $\sqrt{s} =$ 13 TeV

2020AY

PL B808 135578

Measurement of the $\Upsilon$(1S) pair production cross section and search for resonances decaying to $\Upsilon$(1S)$\mu^+\mu^-$ in proton-proton collisions at $\sqrt{s} =$ 13 TeV

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

2019H

PR D99 012008

A search for pairs of highly collimated photon-jets in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector

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

2018CM

PR D98 092008

Search for lepton-flavor violation in different-flavor, high-mass final states in $pp$ collisions at $\sqrt s=13$ TeV with the ATLAS detector

2018CJ

PR D98 052008

Combination of searches for heavy resonances decaying into bosonic and leptonic final states using 36??fb$^{-1}$ of proton-proton collision data at $\sqrt{s} = 13$ TeV with the ATLAS detector

2018AJ

PRL 120 061801

Search for Dark Photons Produced in 13�TeV $pp$ Collisions

PRL 120 231802

Search for a Hypothetical 16.7�MeV Gauge Boson and Dark Photons in the NA64 Experiment at CERN

2018A

PR D97 072002

Search for vector mediator of Dark Matter production in invisible decay mode

MARSICANO

PR D98 015031

Dark photon production through positron annihilation in beam-dump experiments

2018DA

JHEP 1811 042

Search for black holes and sphalerons in high-multiplicity final states in proton-proton collisions at $ \sqrt{s}=13 $ TeV

2018BB

JHEP 1806 120

Search for high-mass resonances in dilepton final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV

2018ED

JHEP 1811 172

Search for heavy resonances decaying into a vector boson and a Higgs boson in final states with charged leptons, neutrinos and b quarks at $ \sqrt{s}=13 $ TeV

2018DU

PR D98 092001

Search for physics beyond the standard model in high-mass diphoton events from proton-proton collisions at $\sqrt{s} =$ 13 TeV

2018DR

JHEP 1811 161

Search for resonances in the mass spectrum of muon pairs produced in association with b quark jets in proton-proton collisions at $\sqrt{s} =$ 8 and 13 TeV

2018DD

EPJ C78 789

Search for new physics in dijet angular distributions using proton?proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models

2017B

PL B765 32

Search for New Resonances Decaying to a ${{\mathit W}}$ or ${{\mathit Z}}$ Boson and a Higgs Boson in the ${{\mathit \ell}^{+}}{{\mathit \ell}^{-}}{\mathit {\mathit b}}{\mathit {\overline{\mathit b}}}$, ${{\mathit \ell}}{{\mathit \nu}}{\mathit {\mathit b}}{\mathit {\overline{\mathit b}}}$, and ${{\mathit \nu}}{{\overline{\mathit \nu}}}{\mathit {\mathit b}}{\mathit {\overline{\mathit b}}}$ Channels with ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 13 TeV with the ATLAS Detector

2017BR

EPJ C77 812

Updated Search for Long-Lived Particles Decaying to Jet Pairs

2016R

PL B755 285

Combination of Searches for ${{\mathit W}}{{\mathit W}}$, ${{\mathit W}}{{\mathit Z}}$, and ${{\mathit Z}}{{\mathit Z}}$ Resonances in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector

2016O

PL B760 520

Search for TeV-Scale Gravity Signatures in High-Mass Final States with Leptons and Jets with the ATLAS Detector at $\sqrt {s }$ = 13 TeV

KRASZNAHORKAY