cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.135986.v1/t9
title: "Table 8" of "Measurement of beauty-strange meson production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV via non-prompt $\mathrm{D_s}^{+}$ mesons"

description: Non-prompt $\mathrm{D}_{s}^{+}$ Raa in 30-50% collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.
description: The production yields of non-prompt $\mathrm{D}_{s}^{+}$ mesons, namely $\mathrm{D}_{s}^{+}$ mesons from beauty-hadron decays, were measured for the first time as a function of the transverse momentum ($p_{T}$) at midrapidity ($|y|&lt;0.5$) in central and semi-central Pb--Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_{NN}}=5.02~$TeV with the ALICE experiment at the LHC.The $\mathrm{D}_{s}^{\pm}$ mesons were reconstructed from the hadronic decay channel $\rm D_s^{+}\to \phi\pi^+$, with $\rm \phi\to K^-K^+$, in the $4
DOI: 10.17182/hepdata.135986.v1/t10
title: "Table 9" of "Measurement of beauty-strange meson production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV via non-prompt $\mathrm{D_s}^{+}$ mesons"

description: Non-prompt $\mathrm{D}_{s}^{+}$ over non-prompt $\mathrm{D}^{0}$ Raa in 0-10% collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.
description: The production yields of non-prompt $\mathrm{D}_{s}^{+}$ mesons, namely $\mathrm{D}_{s}^{+}$ mesons from beauty-hadron decays, were measured for the first time as a function of the transverse momentum ($p_{T}$) at midrapidity ($|y|&lt;0.5$) in central and semi-central Pb--Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_{NN}}=5.02~$TeV with the ALICE experiment at the LHC.The $\mathrm{D}_{s}^{\pm}$ mesons were reconstructed from the hadronic decay channel $\rm D_s^{+}\to \phi\pi^+$, with $\rm \phi\to K^-K^+$, in the $4
DOI: 10.17182/hepdata.135986.v1/t12
title: "Table 11" of "Measurement of beauty-strange meson production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV via non-prompt $\mathrm{D_s}^{+}$ mesons"

description: Non-prompt over prompt $\mathrm{D}_{s}^{+}$ Raa in 0-10% collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.
description: The production yields of non-prompt $\mathrm{D}_{s}^{+}$ mesons, namely $\mathrm{D}_{s}^{+}$ mesons from beauty-hadron decays, were measured for the first time as a function of the transverse momentum ($p_{T}$) at midrapidity ($|y|&lt;0.5$) in central and semi-central Pb--Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_{NN}}=5.02~$TeV with the ALICE experiment at the LHC.The $\mathrm{D}_{s}^{\pm}$ mesons were reconstructed from the hadronic decay channel $\rm D_s^{+}\to \phi\pi^+$, with $\rm \phi\to K^-K^+$, in the $4
DOI: 10.17182/hepdata.135986.v1/t13
title: "Table 12" of "Measurement of beauty-strange meson production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV via non-prompt $\mathrm{D_s}^{+}$ mesons"

description: Non-prompt over prompt $\mathrm{D}_{s}^{+}$ Raa in 0-10% collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.
description: The production yields of non-prompt $\mathrm{D}_{s}^{+}$ mesons, namely $\mathrm{D}_{s}^{+}$ mesons from beauty-hadron decays, were measured for the first time as a function of the transverse momentum ($p_{T}$) at midrapidity ($|y|&lt;0.5$) in central and semi-central Pb--Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_{NN}}=5.02~$TeV with the ALICE experiment at the LHC.The $\mathrm{D}_{s}^{\pm}$ mesons were reconstructed from the hadronic decay channel $\rm D_s^{+}\to \phi\pi^+$, with $\rm \phi\to K^-K^+$, in the $4
DOI: 10.17182/hepdata.135987.v1/t1
title: "Table 1a" of "Measurement of beauty production via non-prompt ${\rm D}^{0}$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Transverse-momentum-differential production yields of non-prompt $\rm D^0$ in central (0-10%) and mid-central (30-50%) Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV.
description: The production of non-prompt $\rm D^0$ mesons from beauty-hadron decays was measured at midrapidity ($|y| &lt; 0.5$) in Pb-Pb collisions at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{\text{NN}}}=5.02$ TeV with the ALICE experiment at the LHC. Their nuclear modification factor ($R_{\rm AA}$), measured for the first time down to $p_{\rm T}$ = 1 GeV/$c$  in the 0-10% and 30-50% centrality classes, indicates a significant suppression, up to a factor of about three, for $p_{\rm T}$ &gt; 5 GeV/$c$ in the 0-10% central Pb--Pb collisions.The data are described by models that include both collisional and radiative processes in the calculation of beauty-quark energy loss in the quark--gluon plasma, and quark recombination in addition to fragmentation as a hadronization mechanism. The ratio of the non-prompt to prompt $\rm D^0$-meson $R_{\rm AA}$ is larger than unity for $p_{\rm T}$ &gt; 4 GeV/$c$ in the 0-10% central Pb-Pb collisions, as predicted by models in which beauty quarks lose less energy than charm quarks in the quark-gluon plasma because of their larger mass.
DOI: 10.17182/hepdata.135987.v1/t2
title: "Table 1b" of "Measurement of beauty production via non-prompt ${\rm D}^{0}$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: The nuclear modification factor of non-prompt $\rm D^0$ as a function of transverse momentum in central (0-10%) and mid-central (30-50%) Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV.
description: The production of non-prompt $\rm D^0$ mesons from beauty-hadron decays was measured at midrapidity ($|y| &lt; 0.5$) in Pb-Pb collisions at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{\text{NN}}}=5.02$ TeV with the ALICE experiment at the LHC. Their nuclear modification factor ($R_{\rm AA}$), measured for the first time down to $p_{\rm T}$ = 1 GeV/$c$  in the 0-10% and 30-50% centrality classes, indicates a significant suppression, up to a factor of about three, for $p_{\rm T}$ &gt; 5 GeV/$c$ in the 0-10% central Pb--Pb collisions.The data are described by models that include both collisional and radiative processes in the calculation of beauty-quark energy loss in the quark--gluon plasma, and quark recombination in addition to fragmentation as a hadronization mechanism. The ratio of the non-prompt to prompt $\rm D^0$-meson $R_{\rm AA}$ is larger than unity for $p_{\rm T}$ &gt; 4 GeV/$c$ in the 0-10% central Pb-Pb collisions, as predicted by models in which beauty quarks lose less energy than charm quarks in the quark-gluon plasma because of their larger mass.
DOI: 10.17182/hepdata.135987.v1/t3
title: "Table 2" of "Measurement of beauty production via non-prompt ${\rm D}^{0}$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: The non-prompt to prompt $\rm D^0$-meson nuclear modification factor ratio as a function of transverse momentum in central (0-10%) Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV.
description: The production of non-prompt $\rm D^0$ mesons from beauty-hadron decays was measured at midrapidity ($|y| &lt; 0.5$) in Pb-Pb collisions at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{\text{NN}}}=5.02$ TeV with the ALICE experiment at the LHC. Their nuclear modification factor ($R_{\rm AA}$), measured for the first time down to $p_{\rm T}$ = 1 GeV/$c$  in the 0-10% and 30-50% centrality classes, indicates a significant suppression, up to a factor of about three, for $p_{\rm T}$ &gt; 5 GeV/$c$ in the 0-10% central Pb--Pb collisions.The data are described by models that include both collisional and radiative processes in the calculation of beauty-quark energy loss in the quark--gluon plasma, and quark recombination in addition to fragmentation as a hadronization mechanism. The ratio of the non-prompt to prompt $\rm D^0$-meson $R_{\rm AA}$ is larger than unity for $p_{\rm T}$ &gt; 4 GeV/$c$ in the 0-10% central Pb-Pb collisions, as predicted by models in which beauty quarks lose less energy than charm quarks in the quark-gluon plasma because of their larger mass.
DOI: 10.17182/hepdata.135991.v1/t1
title: "$a_0^W$ Limit" of "Search for high-mass exclusive $\gamma\gamma\to WW$ and $\gamma\gamma\to ZZ$ production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed upper limits on the AQGC operators $a^W_0/\Lambda^2$, with no unitarization. The $y$ axis shows the limit on the ratio 
of the observed cross section to the cross section predicted for each anomalous coupling value ($\sigma_\mathrm{AQGC}$).
description: A search is performed for exclusive high-mass $\gamma\gamma \to WW$ and $\gamma\gamma \to ZZ$ production in proton-proton collisions using intact forward protons reconstructed in near-beam detectors, with both weak bosons decaying into boosted and merged jets. The analysis is based on a sample of proton-proton collisions collected by the CMS and TOTEM experiments at $\sqrt{s}=13$~TeV, corresponding to an integrated luminosity of 100~$\mathrm{fb}^{-1}$. No excess above the standard model background prediction is observed, and upper limits are set on the $pp \to pWWp$ and $pp \to pZZp$ cross sections in a fiducial region defined by the diboson invariant mass $m(VV)&gt;1$~TeV (with $V =W,Z$) and proton fractional momentum loss $0.04 &lt; \xi &lt; 0.20$. The results are interpreted as new limits on dimension-6 and dimension-8 anomalous quartic gauge couplings.
DOI: 10.17182/hepdata.135991.v1/t2
title: "$a_C^W$ Limit" of "Search for high-mass exclusive $\gamma\gamma\to WW$ and $\gamma\gamma\to ZZ$ production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed upper limits on the AQGC operators $a^W_C/\Lambda^2$, with no unitarization. The $y$ axis shows the limit on the ratio 
of the observed cross section to the cross section predicted for each anomalous coupling value ($\sigma_\mathrm{AQGC}$).
description: A search is performed for exclusive high-mass $\gamma\gamma \to WW$ and $\gamma\gamma \to ZZ$ production in proton-proton collisions using intact forward protons reconstructed in near-beam detectors, with both weak bosons decaying into boosted and merged jets. The analysis is based on a sample of proton-proton collisions collected by the CMS and TOTEM experiments at $\sqrt{s}=13$~TeV, corresponding to an integrated luminosity of 100~$\mathrm{fb}^{-1}$. No excess above the standard model background prediction is observed, and upper limits are set on the $pp \to pWWp$ and $pp \to pZZp$ cross sections in a fiducial region defined by the diboson invariant mass $m(VV)&gt;1$~TeV (with $V =W,Z$) and proton fractional momentum loss $0.04 &lt; \xi &lt; 0.20$. The results are interpreted as new limits on dimension-6 and dimension-8 anomalous quartic gauge couplings.
DOI: 10.17182/hepdata.135991.v1/t3
title: "$a_0^Z$ Limit" of "Search for high-mass exclusive $\gamma\gamma\to WW$ and $\gamma\gamma\to ZZ$ production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed upper limits on the AQGC operators $a^Z_0/\Lambda^2$, with no unitarization. The $y$ axis shows the limit on the ratio 
of the observed cross section to the cross section predicted for each anomalous coupling value ($\sigma_\mathrm{AQGC}$).
description: A search is performed for exclusive high-mass $\gamma\gamma \to WW$ and $\gamma\gamma \to ZZ$ production in proton-proton collisions using intact forward protons reconstructed in near-beam detectors, with both weak bosons decaying into boosted and merged jets. The analysis is based on a sample of proton-proton collisions collected by the CMS and TOTEM experiments at $\sqrt{s}=13$~TeV, corresponding to an integrated luminosity of 100~$\mathrm{fb}^{-1}$. No excess above the standard model background prediction is observed, and upper limits are set on the $pp \to pWWp$ and $pp \to pZZp$ cross sections in a fiducial region defined by the diboson invariant mass $m(VV)&gt;1$~TeV (with $V =W,Z$) and proton fractional momentum loss $0.04 &lt; \xi &lt; 0.20$. The results are interpreted as new limits on dimension-6 and dimension-8 anomalous quartic gauge couplings.
DOI: 10.17182/hepdata.135991.v1/t4
title: "$a_C^Z$ Limit" of "Search for high-mass exclusive $\gamma\gamma\to WW$ and $\gamma\gamma\to ZZ$ production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed upper limits on the AQGC operators $a^Z_C/\Lambda^2$, with no unitarization. The $y$ axis shows the limit on the ratio 
of the observed cross section to the cross section predicted for each anomalous coupling value ($\sigma_\mathrm{AQGC}$).
description: A search is performed for exclusive high-mass $\gamma\gamma \to WW$ and $\gamma\gamma \to ZZ$ production in proton-proton collisions using intact forward protons reconstructed in near-beam detectors, with both weak bosons decaying into boosted and merged jets. The analysis is based on a sample of proton-proton collisions collected by the CMS and TOTEM experiments at $\sqrt{s}=13$~TeV, corresponding to an integrated luminosity of 100~$\mathrm{fb}^{-1}$. No excess above the standard model background prediction is observed, and upper limits are set on the $pp \to pWWp$ and $pp \to pZZp$ cross sections in a fiducial region defined by the diboson invariant mass $m(VV)&gt;1$~TeV (with $V =W,Z$) and proton fractional momentum loss $0.04 &lt; \xi &lt; 0.20$. The results are interpreted as new limits on dimension-6 and dimension-8 anomalous quartic gauge couplings.
DOI: 10.17182/hepdata.135991.v1/t10
title: "ZZ 2D limit plot" of "Search for high-mass exclusive $\gamma\gamma\to WW$ and $\gamma\gamma\to ZZ$ production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: {Expected and observed limits in the two-dimensional plane of $a^Z_0/\Lambda^2$ vs. $a^Z_C/\Lambda^2$. 
The limits are described by analytical ellipses of equation $(x-x0)^2/a^2 + (y-y0)^2/b^2 = 1$ and rotated counter-clockwise by $\theta$ degrees, where $x$ and $y$ in the equation correspond to the $a_0^Z$ and $a_C^Z$ couplings, respectively.
description: A search is performed for exclusive high-mass $\gamma\gamma \to WW$ and $\gamma\gamma \to ZZ$ production in proton-proton collisions using intact forward protons reconstructed in near-beam detectors, with both weak bosons decaying into boosted and merged jets. The analysis is based on a sample of proton-proton collisions collected by the CMS and TOTEM experiments at $\sqrt{s}=13$~TeV, corresponding to an integrated luminosity of 100~$\mathrm{fb}^{-1}$. No excess above the standard model background prediction is observed, and upper limits are set on the $pp \to pWWp$ and $pp \to pZZp$ cross sections in a fiducial region defined by the diboson invariant mass $m(VV)&gt;1$~TeV (with $V =W,Z$) and proton fractional momentum loss $0.04 &lt; \xi &lt; 0.20$. The results are interpreted as new limits on dimension-6 and dimension-8 anomalous quartic gauge couplings.
DOI: 10.17182/hepdata.135991.v1/t5
title: "Limits on LEP-like dimension-6 AQGC parameters" of "Search for high-mass exclusive $\gamma\gamma\to WW$ and $\gamma\gamma\to ZZ$ production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Limits on LEP-like dimension-6 anomalous quartic gauge coupling parameters, 
with and without unitarization via a clipping procedure.
description: A search is performed for exclusive high-mass $\gamma\gamma \to WW$ and $\gamma\gamma \to ZZ$ production in proton-proton collisions using intact forward protons reconstructed in near-beam detectors, with both weak bosons decaying into boosted and merged jets. The analysis is based on a sample of proton-proton collisions collected by the CMS and TOTEM experiments at $\sqrt{s}=13$~TeV, corresponding to an integrated luminosity of 100~$\mathrm{fb}^{-1}$. No excess above the standard model background prediction is observed, and upper limits are set on the $pp \to pWWp$ and $pp \to pZZp$ cross sections in a fiducial region defined by the diboson invariant mass $m(VV)&gt;1$~TeV (with $V =W,Z$) and proton fractional momentum loss $0.04 &lt; \xi &lt; 0.20$. The results are interpreted as new limits on dimension-6 and dimension-8 anomalous quartic gauge couplings.
DOI: 10.17182/hepdata.135991.v1/t6
title: "Limits on dimension-8 operators - vanishing $WWZ\gamma$ coupling" of "Search for high-mass exclusive $\gamma\gamma\to WW$ and $\gamma\gamma\to ZZ$ production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Conversion of limits on $a^W_0$ to dimension-8 $f_{M,i}$ operators, using the assumption of vanishing $WWZ\gamma$ couplings 
to eliminate some parameters. When quoting limits on one of the operators, the other is fixed to zero. 
The results for $|f_{M,0}/\Lambda^{4}|$ and $|f_{M,4}/\Lambda^{4}|$ are shown with and without clipping of the signal model at 1.4 TeV, 
when the other parameter is fixed to the SM value of zero.
description: A search is performed for exclusive high-mass $\gamma\gamma \to WW$ and $\gamma\gamma \to ZZ$ production in proton-proton collisions using intact forward protons reconstructed in near-beam detectors, with both weak bosons decaying into boosted and merged jets. The analysis is based on a sample of proton-proton collisions collected by the CMS and TOTEM experiments at $\sqrt{s}=13$~TeV, corresponding to an integrated luminosity of 100~$\mathrm{fb}^{-1}$. No excess above the standard model background prediction is observed, and upper limits are set on the $pp \to pWWp$ and $pp \to pZZp$ cross sections in a fiducial region defined by the diboson invariant mass $m(VV)&gt;1$~TeV (with $V =W,Z$) and proton fractional momentum loss $0.04 &lt; \xi &lt; 0.20$. The results are interpreted as new limits on dimension-6 and dimension-8 anomalous quartic gauge couplings.
DOI: 10.17182/hepdata.135991.v1/t7
title: "Limits on dimension-8 operators - all other couplings are zero." of "Search for high-mass exclusive $\gamma\gamma\to WW$ and $\gamma\gamma\to ZZ$ production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Conversion of limits on $a^W_0$ and $a^W_C$ to dimension-8 $f_{M,i}$ operators, 
using the assumption that all $f_{M,i}$ except one are equal to zero. The results are shown with and without clipping of the signal model at 1.4 TeV.
description: A search is performed for exclusive high-mass $\gamma\gamma \to WW$ and $\gamma\gamma \to ZZ$ production in proton-proton collisions using intact forward protons reconstructed in near-beam detectors, with both weak bosons decaying into boosted and merged jets. The analysis is based on a sample of proton-proton collisions collected by the CMS and TOTEM experiments at $\sqrt{s}=13$~TeV, corresponding to an integrated luminosity of 100~$\mathrm{fb}^{-1}$. No excess above the standard model background prediction is observed, and upper limits are set on the $pp \to pWWp$ and $pp \to pZZp$ cross sections in a fiducial region defined by the diboson invariant mass $m(VV)&gt;1$~TeV (with $V =W,Z$) and proton fractional momentum loss $0.04 &lt; \xi &lt; 0.20$. The results are interpreted as new limits on dimension-6 and dimension-8 anomalous quartic gauge couplings.
DOI: 10.17182/hepdata.135991.v1/t8
title: "WW 2D limit plot" of "Search for high-mass exclusive $\gamma\gamma\to WW$ and $\gamma\gamma\to ZZ$ production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: {Expected and observed limits in the two-dimensional plane of $a^W_0/\Lambda^2$ vs. $a^W_C/\Lambda^2$. 
The limits are described by analytical ellipses of equation $(x-x0)^2/a^2 + (y-y0)^2/b^2 = 1$ and rotated counter-clockwise by $\theta$ degrees, where $x$ and $y$ in the equation correspond to the $a_0^W$ and $a_C^W$ couplings, respectively.
description: A search is performed for exclusive high-mass $\gamma\gamma \to WW$ and $\gamma\gamma \to ZZ$ production in proton-proton collisions using intact forward protons reconstructed in near-beam detectors, with both weak bosons decaying into boosted and merged jets. The analysis is based on a sample of proton-proton collisions collected by the CMS and TOTEM experiments at $\sqrt{s}=13$~TeV, corresponding to an integrated luminosity of 100~$\mathrm{fb}^{-1}$. No excess above the standard model background prediction is observed, and upper limits are set on the $pp \to pWWp$ and $pp \to pZZp$ cross sections in a fiducial region defined by the diboson invariant mass $m(VV)&gt;1$~TeV (with $V =W,Z$) and proton fractional momentum loss $0.04 &lt; \xi &lt; 0.20$. The results are interpreted as new limits on dimension-6 and dimension-8 anomalous quartic gauge couplings.
DOI: 10.17182/hepdata.135991.v1/t9
title: "WW 2D clipped limit plot" of "Search for high-mass exclusive $\gamma\gamma\to WW$ and $\gamma\gamma\to ZZ$ production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: {Expected and observed limits in the two-dimensional plane of $a^W_0/\Lambda^2$ vs. $a^W_C/\Lambda^2$ 
with unitarization imposed by clipping the signal model at 1.4 TeV. 
The limits are described by analytical ellipses of equation $(x-x0)^2/a^2 + (y-y0)^2/b^2 = 1$ and rotated counter-clockwise by $\theta$ degrees, where $x$ and $y$ in the equation correspond to the $a_0^W$ and $a_C^W$ couplings, respectively.
description: A search is performed for exclusive high-mass $\gamma\gamma \to WW$ and $\gamma\gamma \to ZZ$ production in proton-proton collisions using intact forward protons reconstructed in near-beam detectors, with both weak bosons decaying into boosted and merged jets. The analysis is based on a sample of proton-proton collisions collected by the CMS and TOTEM experiments at $\sqrt{s}=13$~TeV, corresponding to an integrated luminosity of 100~$\mathrm{fb}^{-1}$. No excess above the standard model background prediction is observed, and upper limits are set on the $pp \to pWWp$ and $pp \to pZZp$ cross sections in a fiducial region defined by the diboson invariant mass $m(VV)&gt;1$~TeV (with $V =W,Z$) and proton fractional momentum loss $0.04 &lt; \xi &lt; 0.20$. The results are interpreted as new limits on dimension-6 and dimension-8 anomalous quartic gauge couplings.
DOI: 10.17182/hepdata.136027.v1/t2
title: "Table 2" of "Search for high-mass $W\gamma$ and $Z\gamma$ resonances using hadronic W/Z boson decays from 139 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector"

description: The jet mass distribution of large-$R$ jets originating from the hadronic decay of $W$ and $Z$ bosons produced from the decay of BSM bosons with mass $m_X = 4000$ GeV. The decays simulated are for the production models $q\bar{q'}\to X^{\pm} \to W^{\pm}\gamma$ with a spin-1 resonance $X^{\pm}$ and $gg\to X^0 \to Z\gamma$ with a spin-0 resonance $X^{0}$.
description: CERN-ATLAS. Search for high-mass $W\gamma$ and $Z\gamma$ resonances using hadronic $W/Z$ boson decays from 139 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector

A search for high-mass charged and neutral bosons decaying to $W\gamma$ and $Z\gamma$ final states is presented in this paper. The analysis uses a data sample of $\sqrt{s} = 13$~TeV proton--proton collisions with an integrated luminosity of 139~fb$^{-1}$ collected by the ATLAS detector during LHC Run~2 operation. The sensitivity of the search is determined using models of the production and decay of spin-1 charged bosons and spin-0/2 neutral bosons. The range of resonance masses explored extends from 1.0~TeV to 6.8~TeV. At these high resonance masses, it is beneficial to target the hadronic decays of the $W$ and $Z$ bosons because of their large branching fractions. The decay products of the high-momentum $W/Z$ bosons are strongly collimated and boosted-boson tagging techniques are employed to improve the sensitivity. No evidence of a signal above the Standard Model backgrounds is observed, and upper limits on the production cross-sections of these bosons times their branching fractions to $W\gamma$ and $Z\gamma$ are derived for various boson production models.