# Quantum Black Holes INSPIRE search

VALUE (GeV) DOCUMENT ID TECN  COMMENT
• • • We do not use the following data for averages, fits, limits, etc. • • •
1
 2018 BA
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit j}}$
2
 2018 CM
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \mu}}$ , ${{\mathit e}}{{\mathit \tau}}$ , ${{\mathit \mu}}{{\mathit \tau}}$
3
 2018 AT
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \mu}}$
4
 2018 DD
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ dijet, ang. distrib.
5
 2017 AK
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$
6
 2017 CP
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$
7
 2016 BE
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit e}}{{\mathit \mu}}$
8
 2015 V
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$
9
 2014 AL
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \ell}}{{\mathit j}}$
10
 2014 V
ATLS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit e}}{{\mathit e}}$ , ${{\mathit \mu}}{{\mathit \mu}}$
11
 2013 A
CMS ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit j}}{{\mathit j}}$
1  AABOUD 2018BA use 36.7 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for quantum black hole decays to final states with a photon and a jet. No excess of events above the expected level of Standard Model background was observed. Exclusion limits at 95$\%$ C.L. are set on mass thresholds for black hole production in ADD (6 extra dimensions) and RS1 models. Assuming the black hole mass threshold is equal to the Planck scale, mass thresholds below 7.1 TeV and 4.4 TeV are excluded for the ADD and RS1 models, respectively. These limits supersede those in AAD 2016AI.
2  AABOUD 2018CM use 36.1 ${\mathrm {fb}}{}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for quantum black hole decays with different-flavor high-mass dilepton final states. No excess of events above the expected level of Standard Model background was observed. Exclusion limits at 95$\%$ C.L. are set on mass thresholds for black hole production in ADD (6 extra dimensions) and RS1 models. Assuming the black hole mass threshold is equal to the higher-dimensional Planck scale, mass thresholds below 5.6 (3.4), 4.9 (2.9), and 4.5 (2.6) TeV are excluded in the ${{\mathit e}}{{\mathit \mu}}$ , ${{\mathit e}}{{\mathit \tau}}$ and ${{\mathit \mu}}{{\mathit \tau}}$ channels for the ADD (RS1) models, respectively. These limits supersede those in AABOUD 2016P.
3  SIRUNYAN 2018AT use 35.9 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for quantum black hole decays to ${{\mathit e}}{{\mathit \mu}}$ final states. In Figure 4, lower mass limits of 5.3, 5.5 and 5.6 TeV are placed in a model with 4, 5 and 6 extra dimensions, respectively, and a lower mass limit of 3.6 TeV is found for a single warped dimension.
4  SIRUNYAN 2018DD use 35.9 fb${}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for quantum black hole decays in dijet angular distributions. A lower mass limit of 5.9 (8.2) TeV is placed in the RS (ADD) model with one (six) extra dimension(s).
5  AABOUD 2017AK use 37 ${\mathrm {fb}}{}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for quantum black hole decays to final states with dijets. No excess of events above the expected level of Standard Model background was observed. Exclusion limits at 95$\%$ C.L. are set on mass thresholds for black hole production in an ADD (6 extra dimensions) model. Assuming the black hole mass threshold is equal to the higher-dimensional Planck scale, mass thresholds below 8.9 TeV are excluded.
6  SIRUNYAN 2017CP use 2.3 ${\mathrm {fb}}{}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV to search for quantum black holes decaying to dijet final states. No excess of events above the expected level of standard model background was observed. Limits on the quantum black hole mass threshold are set as a function of the higher-dimensional Planck scale, under the assumption that the mass threshold must exceed the above Planck scale. Depending on the model, mass thresholds in the range up to $5.1 - 9.0$ TeV are excluded.
7  KHACHATRYAN 2016BE use 19.7 ${\mathrm {fb}}{}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV to search for quantum black holes undergoing lepton flavor violating decay to the ${{\mathit e}}{{\mathit \mu}}$ final state. No excess of events above the expected level of standard model background was observed. Exclusion limits at 95$\%$ CL are set on mass thresholds for black hole production in the ADD ($2 - 6$ flat extra dimensions), RS1 (1 warped extra dimension), and a model with a Planck scale at the TeV scale from a renormalization of the gravitational constant (no extra dimensions). Limits on the black hole mass threshold are set assuming that it is equal to the higher-dimensional Planck scale. Mass thresholds for quantum black holes in the range up to $3.15 - 3.63$ TeV are excluded in the ADD model. In the RS1 model, mass thresholds below 2.81 TeV are excluded in the PDG convention for the Schwarzschild radius. In the model with no extra dimensions, mass thresholds below 1.99 TeV are excluded.
8  KHACHATRYAN 2015V use 19.7 ${\mathrm {fb}}{}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV to search for quantum black holes decaying to dijet final states. No excess of events above the expected level of standard model background was observed. Exclusion limits at 95$\%$ CL are set on mass thresholds for black hole production in the ADD ($2 - 6$ flat extra dimensions) and RS1 (1 warped extra dimension) model. Limits on the black hole mass threshold are set as a function of the higher-dimensional Planck scale, under the assumption that the mass threshold must exceed the above Planck scale. Depending on the model, mass thresholds in the range up to $5.0 - 6.3$ TeV are excluded. This paper supersedes CHATRCHYAN 2013AD.
9  AAD 2014AL use 20.3 ${\mathrm {fb}}{}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV to search for quantum black hole decays to final states with high-invariant-mass lepton + jet. No excess of events above the expected level of Standard Model background was observed. Exclusion limits at 95$\%$ C.L. are set on mass thresholds for black hole production in an ADD (6 extra dimensions) model. Assuming the black hole mass threshold is equal to the higher-dimensional Planck scale, mass thresholds below 5.3 TeV are excluded.
10  AAD 2014V use 20.3 (20.5) ${\mathrm {fb}}{}^{-1}$ of data in the dielectron (dimuon) channels from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV to search for quantum black hole decays involving high-mass dilepton resonances. No excess of events above the expected level of Standard Model background was observed. Exclusion limits at 95$\%$ C.L. are set on mass thresholds for black hole production in ADD (6 extra dimensions) and RS1 models. Assuming the black hole mass threshold is equal to the higher-dimensional Planck scale, mass thresholds below 3.65 TeV and 2.24 TeV are excluded for the ADD and RS1 models, respectively.
11  CHATRCHYAN 2013A use 5 ${\mathrm {fb}}{}^{-1}$ of data from ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 7 TeV to search for quantum black holes decaying to dijet final states. No excess of events above the expected level of standard model background was observed. Exclusion limits at 95$\%$ CL are set on mass thresholds for black hole production in the ADD ($2 - 6$ flat extra dimensions) and RS (1 warped extra dimension) model. Limits on the black hole mass threshold are set as a function of the higher-dimensional Planck scale, under assumption that the mass threshold must exceed the above Planck scale. Depending on the model, mass thresholds in the range up to $4.0 - 5.3$ TeV are excluded.
References:
 AABOUD 2018BA
EPJ C78 102 Search for new phenomena in high-mass final states with a photon and a jet from $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector
 AABOUD 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
 SIRUNYAN 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
 SIRUNYAN 2018AT
JHEP 1804 073 Search for lepton-flavor violating decays of heavy resonances and quantum black holes to e? final states in proton-proton collisions at $\sqrt{s}=13$ TeV
 AABOUD 2017AK
PR D96 052004 Search for New Phenomena in Dijet Events using 37 ${\mathrm {fb}}{}^{-1}$ of ${{\mathit p}}{{\mathit p}}$ Collision Data Collected at $\sqrt {s }$ = 13 TeV with the ATLAS Detector
 SIRUNYAN 2017CP
PL B774 279 Search for black holes in high-multiplicity final states in proton-proton collisions at $\sqrt{s}=$13 TeV
 KHACHATRYAN 2016BE
EPJ C76 317 Search for Lepton Flavour Violating Decays of Heavy Resonances and Quantum Black Holes to an ${{\mathit e}}{{\mathit \mu}}$ Pair in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
 KHACHATRYAN 2015V
PR D91 052009 Search for Resonances and Quantum Black Holes using Dijet Mass Spectra in Proton-Proton Collisions at $\sqrt {s }$ = 8 TeV
PR D90 052005 Search for High-Mass Dilepton Resonances in ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV with the ATLAS Detector
PRL 112 091804 Search for Quantum Black Hole Production in High-Invariant-Mass Lepton+Jet Final States using ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 8 TeV and the ATLAS Detector
JHEP 1301 013 Search for Narrow Resonances and Quantum Black Holes in Inclusive and ${\mathit {\mathit b}}$-Tagged Dijet Mass Spectra from ${{\mathit p}}{{\mathit p}}$ Collisions at $\sqrt {s }$ = 7 TeV