cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.136099.v1/t4
title: "Table 4" of "Measurement of prompt charged-particle production in proton-proton collisions at a centre-of-mass energy of 13 TeV"

description: Correlation for the uncertainties of the differential cross-section of prompt inclusive production of long-lived charged particles.
description: No data abstract available.
DOI: 10.17182/hepdata.136099.v1/t5
title: "Table 5" of "Measurement of prompt charged-particle production in proton-proton collisions at a centre-of-mass energy of 13 TeV"

description: Correlation for the uncertainties of the differential cross-section of prompt inclusive production of long-lived charged particles.
description: No data abstract available.
DOI: 10.17182/hepdata.136099.v1/t6
title: "Table 6" of "Measurement of prompt charged-particle production in proton-proton collisions at a centre-of-mass energy of 13 TeV"

description: Correlation for the uncertainties of the differential cross-section of prompt inclusive production of long-lived charged particles.
description: No data abstract available.
DOI: 10.17182/hepdata.136099.v2/t1
title: "Table 1" of "Measurement of prompt charged-particle production in proton-proton collisions at a centre-of-mass energy of 13 TeV"

description: Double differential cross-sections of prompt inclusive production of long-lived negatively charged particles as a function of transverse momentum and pseudorapidity.
description: No data abstract available.
DOI: 10.17182/hepdata.136099.v2/t2
title: "Table 2" of "Measurement of prompt charged-particle production in proton-proton collisions at a centre-of-mass energy of 13 TeV"

description: Double differential cross-sections of prompt inclusive production of long-lived positively charged particles as a function of transverse momentum and pseudorapidity.
description: No data abstract available.
DOI: 10.17182/hepdata.136099.v2/t3
title: "Table 3" of "Measurement of prompt charged-particle production in proton-proton collisions at a centre-of-mass energy of 13 TeV"

description: Correlation for the uncertainties of the differential cross-section of prompt inclusive production of long-lived charged particles.
description: No data abstract available.
DOI: 10.17182/hepdata.136099.v2/t4
title: "Table 4" of "Measurement of prompt charged-particle production in proton-proton collisions at a centre-of-mass energy of 13 TeV"

description: Correlation for the uncertainties of the differential cross-section of prompt inclusive production of long-lived charged particles.
description: No data abstract available.
DOI: 10.17182/hepdata.136099.v2/t5
title: "Table 5" of "Measurement of prompt charged-particle production in proton-proton collisions at a centre-of-mass energy of 13 TeV"

description: Correlation for the uncertainties of the differential cross-section of prompt inclusive production of long-lived charged particles.
description: No data abstract available.
DOI: 10.17182/hepdata.136099.v2/t6
title: "Table 6" of "Measurement of prompt charged-particle production in proton-proton collisions at a centre-of-mass energy of 13 TeV"

description: Correlation for the uncertainties of the differential cross-section of prompt inclusive production of long-lived charged particles.
description: No data abstract available.
DOI: 10.17182/hepdata.136180.v1/t1
title: "Table 1" of "First measurement of $\rm \Omega_c^0$ production in pp collisions at $\sqrt{s}=13$ TeV"

description: The $p_{\rm T}$-differential production cross section of inclusive $\rm \Omega_c^0$ baryons multiplied by the branching ratio into $\rm \Omega^-\pi^+$ for $|{\it y}|&lt;0.5$ in pp collisions at $\sqrt{s}=13$ TeV.
description: The inclusive production of the charm-strange baryon $\rm \Omega_c^0$ is measured for the first time via its hadronic decay into $\rm \Omega^-\pi^+$ at midrapidity ($|{\it y}|&lt;0.5$) in proton-proton (pp) collisions at the centre-of-mass energy $\sqrt{s}=13$ TeV with the ALICE detector at the LHC. The transverse momentum ($p_{\rm T}$) differential cross section multiplied by the branching ratio is presented in the interval $2
DOI: 10.17182/hepdata.136180.v1/t2
title: "Table 2" of "First measurement of $\rm \Omega_c^0$ production in pp collisions at $\sqrt{s}=13$ TeV"

description: $\rm BR(\Omega_{c}^{0} \rightarrow \Omega^{-}\pi^{+}) \times {\it \sigma}(\Omega_{c}^{0})/{\it \sigma}(D^{0})$ as a function of $p_{\rm T}$ in pp collisions at $\sqrt{s}=13$ TeV for $|{\it y}|&lt;0.5$.
description: The inclusive production of the charm-strange baryon $\rm \Omega_c^0$ is measured for the first time via its hadronic decay into $\rm \Omega^-\pi^+$ at midrapidity ($|{\it y}|&lt;0.5$) in proton-proton (pp) collisions at the centre-of-mass energy $\sqrt{s}=13$ TeV with the ALICE detector at the LHC. The transverse momentum ($p_{\rm T}$) differential cross section multiplied by the branching ratio is presented in the interval $2
DOI: 10.17182/hepdata.136180.v1/t3
title: "Table 3" of "First measurement of $\rm \Omega_c^0$ production in pp collisions at $\sqrt{s}=13$ TeV"

description: $\rm BR(\Omega_{c}^{0} \rightarrow \Omega^{-}\pi^{+}) \times {\it \sigma}(\Omega_{c}^{0})/{\it \sigma}(\Xi_c^0)$ as a function of $p_{\rm T}$ in pp collisions at $\sqrt{s}=13$ TeV for $|{\it y}|&lt;0.5$.
description: The inclusive production of the charm-strange baryon $\rm \Omega_c^0$ is measured for the first time via its hadronic decay into $\rm \Omega^-\pi^+$ at midrapidity ($|{\it y}|&lt;0.5$) in proton-proton (pp) collisions at the centre-of-mass energy $\sqrt{s}=13$ TeV with the ALICE detector at the LHC. The transverse momentum ($p_{\rm T}$) differential cross section multiplied by the branching ratio is presented in the interval $2
DOI: 10.17182/hepdata.136309.v1/t1
title: "Table 1" of "$\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $p_{\mathrm T}$-differential yield of $\frac{\mathrm{K^{*0}} + \overline{\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~$8.16 TeV (NSD).
description: No data abstract available.
DOI: 10.17182/hepdata.136309.v1/t2
title: "Table 2" of "$\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $p_{\mathrm T}$-differential yield of $\frac{\mathrm{K^{*0}} + \overline{\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 0-5%).
description: No data abstract available.
DOI: 10.17182/hepdata.136309.v1/t3
title: "Table 3" of "$\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $p_{\mathrm T}$-differential yield of $\frac{\mathrm{K^{*0}} + \overline{\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 5-10%).
description: No data abstract available.
DOI: 10.17182/hepdata.136309.v1/t4
title: "Table 4" of "$\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $p_{\mathrm T}$-differential yield of $\frac{\mathrm{K^{*0}} + \overline{\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 10-20%).
description: No data abstract available.
DOI: 10.17182/hepdata.136309.v1/t5
title: "Table 5" of "$\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $p_{\mathrm T}$-differential yield of $\frac{\mathrm{K^{*0}} + \overline{\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 20-40%).
description: No data abstract available.
DOI: 10.17182/hepdata.136309.v1/t6
title: "Table 6" of "$\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $p_{\mathrm T}$-differential yield of $\frac{\mathrm{K^{*0}} + \overline{\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 40-60%).
description: No data abstract available.
DOI: 10.17182/hepdata.136309.v1/t7
title: "Table 7" of "$\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $p_{\mathrm T}$-differential yield of $\frac{\mathrm{K^{*0}} + \overline{\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 60-80%).
description: No data abstract available.
DOI: 10.17182/hepdata.136309.v1/t8
title: "Table 8" of "$\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $p_{\mathrm T}$-differential yield of $\frac{\mathrm{K^{*0}} + \overline{\mathrm{K^{*0}}}}{2}$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 80-100%).
description: No data abstract available.
DOI: 10.17182/hepdata.136309.v1/t10
title: "Table 10" of "$\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $p_{\mathrm T}$-differential yield of $\phi$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 0-5%).
description: No data abstract available.
DOI: 10.17182/hepdata.136309.v1/t11
title: "Table 11" of "$\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $p_{\mathrm T}$-differential yield of $\phi$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 5-10%).
description: No data abstract available.
DOI: 10.17182/hepdata.136309.v1/t12
title: "Table 12" of "$\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $p_{\mathrm T}$-differential yield of $\phi$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 10-20%).
description: No data abstract available.
DOI: 10.17182/hepdata.136309.v1/t13
title: "Table 13" of "$\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $p_{\mathrm T}$-differential yield of $\phi$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 20-40%).
description: No data abstract available.
DOI: 10.17182/hepdata.136309.v1/t14
title: "Table 14" of "$\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $p_{\mathrm T}$-differential yield of $\phi$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 40-60%).
description: No data abstract available.
DOI: 10.17182/hepdata.136309.v1/t15
title: "Table 15" of "$\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $p_{\mathrm T}$-differential yield of $\phi$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 60-80%).
description: No data abstract available.
DOI: 10.17182/hepdata.136309.v1/t9
title: "Table 9" of "$\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $p_{\mathrm T}$-differential yield of $\phi$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~$8.16 TeV (NSD).
description: No data abstract available.
DOI: 10.17182/hepdata.136309.v1/t16
title: "Table 16" of "$\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $p_{\mathrm T}$-differential yield of $\phi$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~$8.16 TeV (Multiplicity class 80-100%).
description: No data abstract available.
DOI: 10.17182/hepdata.136309.v1/t17
title: "Table 17" of "$\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $p_{\mathrm T}$-differential $R_{\mathrm{pPb}}$ of K$^{*0}$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~$8.16 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.136309.v1/t18
title: "Table 18" of "$\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $p_{\mathrm T}$-differential $R_{\mathrm{pPb}}$ of $\phi$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~$8.16 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.136309.v1/t19
title: "Table 19" of "$\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $p_{\mathrm T}$-differential $R_{\mathrm{pPb}}$ of K$^{*0}$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~$5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.136309.v1/t20
title: "Table 20" of "$\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $p_{\mathrm T}$-differential $R_{\mathrm{pPb}}$ of $\phi$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~$5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.136309.v1/t21
title: "Table 21" of "$\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $p_{\mathrm T}$-differential $R_{\mathrm{pPb}}$ of $\Xi$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~$5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.136309.v1/t22
title: "Table 22" of "$\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"

description: $p_{\mathrm T}$-differential $R_{\mathrm{pPb}}$ of $\Omega$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}~=~$5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.136310.v1/t1
title: "Table 1" of "First measurement of antideuteron number fluctuations at energies available at the Large Hadron Collider"

description: Second order to first order cumulant ratio of the $\overline{d}$ multiplicity distribution as a function of collision centrality in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV.
description: Measurements of antideuteron number fluctuations in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV using the ALICE detector at the CERN LHC. Second order cumulant to fitrst order cumulant ratios of antideuteron multiplicity distributions are reported as a function of collision centrality. Furthermore, pearson correlations between measured antideuteron and antiproton are also presented as a function of collision centrality as well as pseudorapidity acceptance.
DOI: 10.17182/hepdata.136310.v1/t2
title: "Table 2" of "First measurement of antideuteron number fluctuations at energies available at the Large Hadron Collider"

description: Pearson correlation between the measured $\overline{p}$ and $\overline{d}$ as a function of collision centrality in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV.
description: Measurements of antideuteron number fluctuations in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV using the ALICE detector at the CERN LHC. Second order cumulant to fitrst order cumulant ratios of antideuteron multiplicity distributions are reported as a function of collision centrality. Furthermore, pearson correlations between measured antideuteron and antiproton are also presented as a function of collision centrality as well as pseudorapidity acceptance.
DOI: 10.17182/hepdata.136310.v1/t3
title: "Table 3" of "First measurement of antideuteron number fluctuations at energies available at the Large Hadron Collider"

description: Dependence of $\overline{p}$-$\overline{d}$ correlation on pseudorapidity acceptance of $\overline{p}$ and $\overline{d}$ selection in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV. Results are for 0.0--10.0$\%$ collision centrality.
description: Measurements of antideuteron number fluctuations in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV using the ALICE detector at the CERN LHC. Second order cumulant to fitrst order cumulant ratios of antideuteron multiplicity distributions are reported as a function of collision centrality. Furthermore, pearson correlations between measured antideuteron and antiproton are also presented as a function of collision centrality as well as pseudorapidity acceptance.
DOI: 10.17182/hepdata.136310.v1/t5
title: "Table 5" of "First measurement of antideuteron number fluctuations at energies available at the Large Hadron Collider"

description: Dependence of $\overline{p}$-$\overline{d}$ correlation on pseudorapidity acceptance of $\overline{p}$ and $\overline{d}$ selection in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV. Results are for 50.0--60.0$\%$ collision centrality.
description: Measurements of antideuteron number fluctuations in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV using the ALICE detector at the CERN LHC. Second order cumulant to fitrst order cumulant ratios of antideuteron multiplicity distributions are reported as a function of collision centrality. Furthermore, pearson correlations between measured antideuteron and antiproton are also presented as a function of collision centrality as well as pseudorapidity acceptance.
DOI: 10.17182/hepdata.136310.v1/t4
title: "Table 4" of "First measurement of antideuteron number fluctuations at energies available at the Large Hadron Collider"

description: Dependence of $\overline{p}$-$\overline{d}$ correlation on pseudorapidity acceptance of $\overline{p}$ and $\overline{d}$ selection in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV. Results are for 20.0--30.0$\%$ collision centrality.
description: Measurements of antideuteron number fluctuations in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV using the ALICE detector at the CERN LHC. Second order cumulant to fitrst order cumulant ratios of antideuteron multiplicity distributions are reported as a function of collision centrality. Furthermore, pearson correlations between measured antideuteron and antiproton are also presented as a function of collision centrality as well as pseudorapidity acceptance.
DOI: 10.17182/hepdata.136515.v2/t1
title: "Table 1" of "Search for exclusive Higgs and $Z$ boson decays to $\omega\gamma$ and Higgs boson decays to $K^{*}\gamma$ with the ATLAS detector"

description: Numbers of observed and expected background events for the $m_{\mathcal{M}\gamma}$ ranges of interest. Each expected background and the corresponding uncertainty of its mean is obtained from a background-only fit to the data; the uncertainty does not take into account statistical fluctuations in each mass range. Expected $Z$ and Higgs boson signal contributions, with their corresponding total systematic uncertainty, are shown for reference branching fractions of $10^{-6}$ and $10^{-4}$, respectively.
description: CERN-LHC, ATLAS. Searches for the exclusive decays of the Higgs boson to an $\omega$ meson and a photon or a $K^{*}$ meson and a photon can probe flavour-conserving and flavour-violating Higgs boson couplings to light quarks, respectively. Searches for these decays, along with the analogous $Z$ boson decay to an $\omega$ meson and a photon, are performed with a $pp$ collision data sample corresponding to integrated luminosities of up to 134 fb$^{-1}$ collected at $\sqrt{s}=13$ TeV with the ATLAS detector at the CERN Large Hadron Collider. The obtained 95% confidence-level upper limits on the respective branching fractions are ${\cal B}(H\rightarrow\omega\gamma)&lt; 5.5\times 10^{-4}$, ${\cal B}(H\rightarrow K^{*}\gamma)&lt; 2.2\times10^{-4}$ and ${\cal B}(Z\rightarrow \omega\gamma)&lt;3.9\times 10^{-6}$. The limits for $H\rightarrow \omega\gamma$ and $Z\rightarrow \omega\gamma$ are 370 times and 140 times the Standard Model expected values, respectively. The result for $Z\rightarrow \omega\gamma$ corresponds to a two-orders-of-magnitude improvement over a the limit obtained by the DELPHI experiment at LEP.
DOI: 10.17182/hepdata.136515.v2/t2
title: "Table 2" of "Search for exclusive Higgs and $Z$ boson decays to $\omega\gamma$ and Higgs boson decays to $K^{*}\gamma$ with the ATLAS detector"

description: Expected and observed branching fraction limits at the 95% CL for $H/Z\rightarrow \omega\gamma$ and $H\rightarrow K^{*}\gamma$.
description: CERN-LHC, ATLAS. Searches for the exclusive decays of the Higgs boson to an $\omega$ meson and a photon or a $K^{*}$ meson and a photon can probe flavour-conserving and flavour-violating Higgs boson couplings to light quarks, respectively. Searches for these decays, along with the analogous $Z$ boson decay to an $\omega$ meson and a photon, are performed with a $pp$ collision data sample corresponding to integrated luminosities of up to 134 fb$^{-1}$ collected at $\sqrt{s}=13$ TeV with the ATLAS detector at the CERN Large Hadron Collider. The obtained 95% confidence-level upper limits on the respective branching fractions are ${\cal B}(H\rightarrow\omega\gamma)&lt; 5.5\times 10^{-4}$, ${\cal B}(H\rightarrow K^{*}\gamma)&lt; 2.2\times10^{-4}$ and ${\cal B}(Z\rightarrow \omega\gamma)&lt;3.9\times 10^{-6}$. The limits for $H\rightarrow \omega\gamma$ and $Z\rightarrow \omega\gamma$ are 370 times and 140 times the Standard Model expected values, respectively. The result for $Z\rightarrow \omega\gamma$ corresponds to a two-orders-of-magnitude improvement over a the limit obtained by the DELPHI experiment at LEP.
DOI: 10.17182/hepdata.136515.v1/t1
title: "Table 2" of "Search for exclusive Higgs and $Z$ boson decays to $\omega\gamma$ and Higgs boson decays to $K^{*}\gamma$ with the ATLAS detector"

description: Numbers of observed and expected background events for the $m_{\mathcal{M}\gamma}$ ranges of interest. Each expected background and the corresponding uncertainty of its mean is obtained from a background-only fit to the data; the uncertainty does not take into account statistical fluctuations in each mass range. Expected $Z$ and Higgs boson signal contributions, with their corresponding total systematic uncertainty, are shown for reference branching fractions of $10^{-6}$ and $10^{-4}$, respectively.
description: CERN-LHC, ATLAS. Searches for the exclusive decays of the Higgs boson to an $\omega$ meson and a photon or a $K^{*}$ meson and a photon can probe flavour-conserving and flavour-violating Higgs boson couplings to light quarks, respectively. Searches for these decays, along with the analogous $Z$ boson decay to an $\omega$ meson and a photon, are performed with a $pp$ collision data sample corresponding to integrated luminosities of up to 134 fb$^{-1}$ collected at $\sqrt{s}=13$ TeV with the ATLAS detector at the CERN Large Hadron Collider. The obtained 95% confidence-level upper limits on the respective branching fractions are ${\cal B}(H\rightarrow\omega\gamma)&lt; 1.5\times 10^{-4}$, ${\cal B}(H\rightarrow K^{*}\gamma)&lt; 8.9\times10^{-5}$ and ${\cal B}(Z\rightarrow \omega\gamma)&lt;3.8\times 10^{-7}$. The limits for $H\rightarrow \omega\gamma$ and $Z\rightarrow \omega\gamma$ are 100 times and 17 times the Standard Model expected values, respectively. The result for $Z\rightarrow \omega\gamma$ corresponds to a three-orders-of-magnitude improvement over a previously set limit.