cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.158364.v1/t9
title: "Figure 6a" of "Search for a new scalar resonance decaying to a Higgs boson and another new scalar particle in the final state with two bottom quarks and two photons in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed(expected) upper limits on the $\sigma\mathcal{B}$ for the X to $Y(\gamma\gamma)H(bb)$ signal with the different $m_Y$ hypotheses are shown with solid(dashed) lines. The inner (green) band and the outer (yellow) band indicate the regions containing $68\%$ and $95\%$, respectively, of the distribution of limits expected under the background-only hypothesis. This plot shows the set of mass points with the lowest $m_X = 240GeV$
description: A search for a new scalar resonance, X, decaying to a standard model Higgs boson and another new scalar particle, Y, is presented. The Higgs boson further decays to a pair of b quarks, while the Y particle decays to a pair of photons. The search is performed in the mass range 240--1000GeV for the resonance X, and in the mass range 70--800GeV for the particle Y, using proton-proton collision data collected by the CMS experiment at $\sqrt{s}=13TeV$, corresponding to an integrated luminosity of $132fb^{-1}$. In general, the data are found to be compatible with the standard model expectation. Observed (expected) upper limits on the product of the production cross section and the relevant branching fraction at $95%$ confidence level are extracted for the $X\rightarrow YH$ process, and are found to be within the range of 0.05--2.69(0.08--1.94)fb depending on $m_{X}$ and $m_{Y}$. The most significant deviation from the background-only hypothesis is observed for X and Y masses of $300$ and $77GeV$, respectively, with a local (global) significance of 3.33 (0.65) standard deviations.
DOI: 10.17182/hepdata.158371.v1/t1
title: "Nonresonant upper limits" of "Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $γγττ$ final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed and expected 95% CL upper limits on the nonresonant $\mathrm{HH}$ production cross section, $\sigma(\mathrm{pp} \to \mathrm{HH})$, as a function of the Higgs boson self-coupling strength modifier $\kappa_\lambda$. All Higgs boson couplings other than $\lambda$ are assumed to have the values predicted in the SM.
description: The results of a search for the production of two scalar bosons in final states with two photons and two tau leptons are presented. The search considers both nonresonant production of a Higgs boson pair, $\mathrm{HH}$, and resonant production via a new boson $\mathrm{X}$ which decays either to $\mathrm{HH}$ or to $\mathrm{H}$ and a new scalar $\mathrm{Y}$. The analysis uses up to 138 fb$^{-1}$ of proton-proton collision data, recorded between 2016 and 2018 by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV. No evidence for signal is found in the data. For the nonresonant production, the observed (expected) upper limit at 95% confidence level (CL) on the $\mathrm{HH}$ production cross section is set at 930 (740) fb, corresponding to 33 (26) times the standard model prediction. At 95% CL, $\mathrm{HH}$ production is observed (expected) to be excluded for values of $\kappa_\lambda$ outside the range between -12 (-9.4) and 17 (15). Observed (expected) upper limits at 95% CL for the $\mathrm{X} \to \mathrm{HH}$ cross section are found to be within 160 to 2200 (200 to 1800) fb, depending on the mass of $\mathrm{X}$. In the $\mathrm{X} \to \mathrm{YH}$ production scenario, the observed (expected) upper limits vary between 0.059 -1.2 fb (0.87 -0.68 fb) for the $\mathrm{X} \to \mathrm{Y}(\to\tau\tau)\mathrm{H}(\to\gamma\gamma)$ search. For the $\mathrm{X} \to \mathrm{Y}(\to\gamma\gamma)\mathrm{H}(\to\tau\tau)$ search the observed (expected) upper limits vary between 0.69 -15 fb (0.73 -8.3 fb) in the low $\mathrm{Y}$ mass search, tightening constraints on the NMSSM, and between 0.64 -10 fb (0.70 -7.6 fb) in the high $\mathrm{Y}$ mass search.
DOI: 10.17182/hepdata.158371.v1/t2
title: "Upper limits on EFT benchmarks" of "Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $γγττ$ final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed and expected 95% CL upper limits on the nonresonant $\mathrm{HH}$ production cross section, $\sigma(\mathrm{pp} \to \mathrm{HH})$, for thirteen different BSM benchmark scenarios from [arXiv:1507.02245, arXiv:1806.05162] which consider different values of the couplings, $\kappa_\lambda$, $\kappa_t$, $c_{2g}$, $c_g$, and $c_2$ (defined in Table 1).
description: The results of a search for the production of two scalar bosons in final states with two photons and two tau leptons are presented. The search considers both nonresonant production of a Higgs boson pair, $\mathrm{HH}$, and resonant production via a new boson $\mathrm{X}$ which decays either to $\mathrm{HH}$ or to $\mathrm{H}$ and a new scalar $\mathrm{Y}$. The analysis uses up to 138 fb$^{-1}$ of proton-proton collision data, recorded between 2016 and 2018 by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV. No evidence for signal is found in the data. For the nonresonant production, the observed (expected) upper limit at 95% confidence level (CL) on the $\mathrm{HH}$ production cross section is set at 930 (740) fb, corresponding to 33 (26) times the standard model prediction. At 95% CL, $\mathrm{HH}$ production is observed (expected) to be excluded for values of $\kappa_\lambda$ outside the range between -12 (-9.4) and 17 (15). Observed (expected) upper limits at 95% CL for the $\mathrm{X} \to \mathrm{HH}$ cross section are found to be within 160 to 2200 (200 to 1800) fb, depending on the mass of $\mathrm{X}$. In the $\mathrm{X} \to \mathrm{YH}$ production scenario, the observed (expected) upper limits vary between 0.059 -1.2 fb (0.87 -0.68 fb) for the $\mathrm{X} \to \mathrm{Y}(\to\tau\tau)\mathrm{H}(\to\gamma\gamma)$ search. For the $\mathrm{X} \to \mathrm{Y}(\to\gamma\gamma)\mathrm{H}(\to\tau\tau)$ search the observed (expected) upper limits vary between 0.69 -15 fb (0.73 -8.3 fb) in the low $\mathrm{Y}$ mass search, tightening constraints on the NMSSM, and between 0.64 -10 fb (0.70 -7.6 fb) in the high $\mathrm{Y}$ mass search.
DOI: 10.17182/hepdata.158371.v1/t3
title: "$\mathrm{X}^{(0)} \to \mathrm{HH}$ limits" of "Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $γγττ$ final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed and expected 95% CL upper limits on the cross section for the resonant production of a new spin-0 particle $\mathrm{X}^{(0)}$ which decays to Higgs boson pairs, $\sigma(\mathrm{pp} \to \mathrm{X}^{(0)} \to \mathrm{HH})$, given for different values of $m_\mathrm{X}$ in the range 260-1000 GeV.
description: The results of a search for the production of two scalar bosons in final states with two photons and two tau leptons are presented. The search considers both nonresonant production of a Higgs boson pair, $\mathrm{HH}$, and resonant production via a new boson $\mathrm{X}$ which decays either to $\mathrm{HH}$ or to $\mathrm{H}$ and a new scalar $\mathrm{Y}$. The analysis uses up to 138 fb$^{-1}$ of proton-proton collision data, recorded between 2016 and 2018 by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV. No evidence for signal is found in the data. For the nonresonant production, the observed (expected) upper limit at 95% confidence level (CL) on the $\mathrm{HH}$ production cross section is set at 930 (740) fb, corresponding to 33 (26) times the standard model prediction. At 95% CL, $\mathrm{HH}$ production is observed (expected) to be excluded for values of $\kappa_\lambda$ outside the range between -12 (-9.4) and 17 (15). Observed (expected) upper limits at 95% CL for the $\mathrm{X} \to \mathrm{HH}$ cross section are found to be within 160 to 2200 (200 to 1800) fb, depending on the mass of $\mathrm{X}$. In the $\mathrm{X} \to \mathrm{YH}$ production scenario, the observed (expected) upper limits vary between 0.059 -1.2 fb (0.87 -0.68 fb) for the $\mathrm{X} \to \mathrm{Y}(\to\tau\tau)\mathrm{H}(\to\gamma\gamma)$ search. For the $\mathrm{X} \to \mathrm{Y}(\to\gamma\gamma)\mathrm{H}(\to\tau\tau)$ search the observed (expected) upper limits vary between 0.69 -15 fb (0.73 -8.3 fb) in the low $\mathrm{Y}$ mass search, tightening constraints on the NMSSM, and between 0.64 -10 fb (0.70 -7.6 fb) in the high $\mathrm{Y}$ mass search.
DOI: 10.17182/hepdata.158371.v1/t4
title: "$\mathrm{X}^{(2)} \to \mathrm{HH}$ limits" of "Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $γγττ$ final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed and expected 95% CL upper limits on the cross section for the resonant production of a new spin-2 particle $\mathrm{X}^{(2)}$ which decays to Higgs boson pairs, $\sigma(\mathrm{pp} \to \mathrm{X}^{(2)} \to \mathrm{HH})$, given for different values of $m_\mathrm{X}$ in the range 260-1000 GeV.
description: The results of a search for the production of two scalar bosons in final states with two photons and two tau leptons are presented. The search considers both nonresonant production of a Higgs boson pair, $\mathrm{HH}$, and resonant production via a new boson $\mathrm{X}$ which decays either to $\mathrm{HH}$ or to $\mathrm{H}$ and a new scalar $\mathrm{Y}$. The analysis uses up to 138 fb$^{-1}$ of proton-proton collision data, recorded between 2016 and 2018 by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV. No evidence for signal is found in the data. For the nonresonant production, the observed (expected) upper limit at 95% confidence level (CL) on the $\mathrm{HH}$ production cross section is set at 930 (740) fb, corresponding to 33 (26) times the standard model prediction. At 95% CL, $\mathrm{HH}$ production is observed (expected) to be excluded for values of $\kappa_\lambda$ outside the range between -12 (-9.4) and 17 (15). Observed (expected) upper limits at 95% CL for the $\mathrm{X} \to \mathrm{HH}$ cross section are found to be within 160 to 2200 (200 to 1800) fb, depending on the mass of $\mathrm{X}$. In the $\mathrm{X} \to \mathrm{YH}$ production scenario, the observed (expected) upper limits vary between 0.059 -1.2 fb (0.87 -0.68 fb) for the $\mathrm{X} \to \mathrm{Y}(\to\tau\tau)\mathrm{H}(\to\gamma\gamma)$ search. For the $\mathrm{X} \to \mathrm{Y}(\to\gamma\gamma)\mathrm{H}(\to\tau\tau)$ search the observed (expected) upper limits vary between 0.69 -15 fb (0.73 -8.3 fb) in the low $\mathrm{Y}$ mass search, tightening constraints on the NMSSM, and between 0.64 -10 fb (0.70 -7.6 fb) in the high $\mathrm{Y}$ mass search.
DOI: 10.17182/hepdata.158371.v1/t5
title: "$\text{Y} \to \tau\tau$ limits ($m_\text{X}$ stacks)" of "Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $γγττ$ final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed and expected 95% CL upper limits on the cross section for the resonant production of a new scalar particle $\mathrm{X}$ which decays to a SM Higgs boson and a new scalar particle $\mathrm{Y}$ which subsequently decay to a pair of photons and a pair of tau leptons, $\sigma(\mathrm{pp} \to \mathrm{X} \to \mathrm{YH} \to \gamma\gamma\tau\tau)$. The limits are shown for different values of $m_\mathrm{Y}$ in the range 50-800 GeV and at particular values of $m_\mathrm{X}$ in the range 300-1000 GeV.
description: The results of a search for the production of two scalar bosons in final states with two photons and two tau leptons are presented. The search considers both nonresonant production of a Higgs boson pair, $\mathrm{HH}$, and resonant production via a new boson $\mathrm{X}$ which decays either to $\mathrm{HH}$ or to $\mathrm{H}$ and a new scalar $\mathrm{Y}$. The analysis uses up to 138 fb$^{-1}$ of proton-proton collision data, recorded between 2016 and 2018 by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV. No evidence for signal is found in the data. For the nonresonant production, the observed (expected) upper limit at 95% confidence level (CL) on the $\mathrm{HH}$ production cross section is set at 930 (740) fb, corresponding to 33 (26) times the standard model prediction. At 95% CL, $\mathrm{HH}$ production is observed (expected) to be excluded for values of $\kappa_\lambda$ outside the range between -12 (-9.4) and 17 (15). Observed (expected) upper limits at 95% CL for the $\mathrm{X} \to \mathrm{HH}$ cross section are found to be within 160 to 2200 (200 to 1800) fb, depending on the mass of $\mathrm{X}$. In the $\mathrm{X} \to \mathrm{YH}$ production scenario, the observed (expected) upper limits vary between 0.059 -1.2 fb (0.87 -0.68 fb) for the $\mathrm{X} \to \mathrm{Y}(\to\tau\tau)\mathrm{H}(\to\gamma\gamma)$ search. For the $\mathrm{X} \to \mathrm{Y}(\to\gamma\gamma)\mathrm{H}(\to\tau\tau)$ search the observed (expected) upper limits vary between 0.69 -15 fb (0.73 -8.3 fb) in the low $\mathrm{Y}$ mass search, tightening constraints on the NMSSM, and between 0.64 -10 fb (0.70 -7.6 fb) in the high $\mathrm{Y}$ mass search.
DOI: 10.17182/hepdata.158371.v1/t6
title: "$\text{Y} \to \tau\tau$ limits ($m_\text{Y}$ stacks)" of "Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $γγττ$ final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed and expected 95% CL upper limits on the cross section for the resonant production of a new scalar particle $\mathrm{X}$ which decays to a SM Higgs boson and a new scalar particle $\mathrm{Y}$ which subsequently decay to a pair of photons and a pair of tau leptons, $\sigma(\mathrm{pp} \to \mathrm{X} \to \mathrm{YH} \to \gamma\gamma\tau\tau)$. The limits are shown for different values of $m_\mathrm{X}$ in the range 300-1000 GeV and at particular values of $m_\mathrm{Y}$ in the range 50-800 GeV.
description: The results of a search for the production of two scalar bosons in final states with two photons and two tau leptons are presented. The search considers both nonresonant production of a Higgs boson pair, $\mathrm{HH}$, and resonant production via a new boson $\mathrm{X}$ which decays either to $\mathrm{HH}$ or to $\mathrm{H}$ and a new scalar $\mathrm{Y}$. The analysis uses up to 138 fb$^{-1}$ of proton-proton collision data, recorded between 2016 and 2018 by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV. No evidence for signal is found in the data. For the nonresonant production, the observed (expected) upper limit at 95% confidence level (CL) on the $\mathrm{HH}$ production cross section is set at 930 (740) fb, corresponding to 33 (26) times the standard model prediction. At 95% CL, $\mathrm{HH}$ production is observed (expected) to be excluded for values of $\kappa_\lambda$ outside the range between -12 (-9.4) and 17 (15). Observed (expected) upper limits at 95% CL for the $\mathrm{X} \to \mathrm{HH}$ cross section are found to be within 160 to 2200 (200 to 1800) fb, depending on the mass of $\mathrm{X}$. In the $\mathrm{X} \to \mathrm{YH}$ production scenario, the observed (expected) upper limits vary between 0.059 -1.2 fb (0.87 -0.68 fb) for the $\mathrm{X} \to \mathrm{Y}(\to\tau\tau)\mathrm{H}(\to\gamma\gamma)$ search. For the $\mathrm{X} \to \mathrm{Y}(\to\gamma\gamma)\mathrm{H}(\to\tau\tau)$ search the observed (expected) upper limits vary between 0.69 -15 fb (0.73 -8.3 fb) in the low $\mathrm{Y}$ mass search, tightening constraints on the NMSSM, and between 0.64 -10 fb (0.70 -7.6 fb) in the high $\mathrm{Y}$ mass search.
DOI: 10.17182/hepdata.158371.v1/t7
title: "$\text{Y} \to \tau\tau$ limits (2D)" of "Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $γγττ$ final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed and expected 95% CL upper limits on the cross section for the resonant production of a new scalar particle $\mathrm{X}$ which decays to a SM Higgs boson and a new scalar particle $\mathrm{Y}$ which subsequently decay to a pair of photons and a pair of tau leptons, $\sigma(\mathrm{pp} \to \mathrm{X} \to \mathrm{YH} \to \gamma\gamma\tau\tau)$. The limits are shown for different values of $m_\mathrm{X}$ in the range 300-1000 GeV and $m_\mathrm{Y}$ in the range 50-800 GeV.
description: The results of a search for the production of two scalar bosons in final states with two photons and two tau leptons are presented. The search considers both nonresonant production of a Higgs boson pair, $\mathrm{HH}$, and resonant production via a new boson $\mathrm{X}$ which decays either to $\mathrm{HH}$ or to $\mathrm{H}$ and a new scalar $\mathrm{Y}$. The analysis uses up to 138 fb$^{-1}$ of proton-proton collision data, recorded between 2016 and 2018 by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV. No evidence for signal is found in the data. For the nonresonant production, the observed (expected) upper limit at 95% confidence level (CL) on the $\mathrm{HH}$ production cross section is set at 930 (740) fb, corresponding to 33 (26) times the standard model prediction. At 95% CL, $\mathrm{HH}$ production is observed (expected) to be excluded for values of $\kappa_\lambda$ outside the range between -12 (-9.4) and 17 (15). Observed (expected) upper limits at 95% CL for the $\mathrm{X} \to \mathrm{HH}$ cross section are found to be within 160 to 2200 (200 to 1800) fb, depending on the mass of $\mathrm{X}$. In the $\mathrm{X} \to \mathrm{YH}$ production scenario, the observed (expected) upper limits vary between 0.059 -1.2 fb (0.87 -0.68 fb) for the $\mathrm{X} \to \mathrm{Y}(\to\tau\tau)\mathrm{H}(\to\gamma\gamma)$ search. For the $\mathrm{X} \to \mathrm{Y}(\to\gamma\gamma)\mathrm{H}(\to\tau\tau)$ search the observed (expected) upper limits vary between 0.69 -15 fb (0.73 -8.3 fb) in the low $\mathrm{Y}$ mass search, tightening constraints on the NMSSM, and between 0.64 -10 fb (0.70 -7.6 fb) in the high $\mathrm{Y}$ mass search.
DOI: 10.17182/hepdata.158371.v1/t8
title: "Low-mass $\text{Y}\to\gamma\gamma$ limits ($m_\text{X}$ stacks)" of "Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $γγττ$ final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed and expected 95% CL upper limits on the cross section for the resonant production of a new scalar particle $\mathrm{X}$ which decays to a SM Higgs boson and a new scalar particle $\mathrm{Y}$, multiplied by the $\mathrm{Y} \to \gamma\gamma$ branching fraction, $\sigma(\mathrm{pp} \to \mathrm{X} \to \mathrm{YH})B(\mathrm{Y} \to \gamma\gamma)$. The limits are shown for different values of $m_\mathrm{Y}$ in the range 70-125 GeV and at particular values of $m_\mathrm{X}$ in the range 300-1000 GeV.
description: The results of a search for the production of two scalar bosons in final states with two photons and two tau leptons are presented. The search considers both nonresonant production of a Higgs boson pair, $\mathrm{HH}$, and resonant production via a new boson $\mathrm{X}$ which decays either to $\mathrm{HH}$ or to $\mathrm{H}$ and a new scalar $\mathrm{Y}$. The analysis uses up to 138 fb$^{-1}$ of proton-proton collision data, recorded between 2016 and 2018 by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV. No evidence for signal is found in the data. For the nonresonant production, the observed (expected) upper limit at 95% confidence level (CL) on the $\mathrm{HH}$ production cross section is set at 930 (740) fb, corresponding to 33 (26) times the standard model prediction. At 95% CL, $\mathrm{HH}$ production is observed (expected) to be excluded for values of $\kappa_\lambda$ outside the range between -12 (-9.4) and 17 (15). Observed (expected) upper limits at 95% CL for the $\mathrm{X} \to \mathrm{HH}$ cross section are found to be within 160 to 2200 (200 to 1800) fb, depending on the mass of $\mathrm{X}$. In the $\mathrm{X} \to \mathrm{YH}$ production scenario, the observed (expected) upper limits vary between 0.059 -1.2 fb (0.87 -0.68 fb) for the $\mathrm{X} \to \mathrm{Y}(\to\tau\tau)\mathrm{H}(\to\gamma\gamma)$ search. For the $\mathrm{X} \to \mathrm{Y}(\to\gamma\gamma)\mathrm{H}(\to\tau\tau)$ search the observed (expected) upper limits vary between 0.69 -15 fb (0.73 -8.3 fb) in the low $\mathrm{Y}$ mass search, tightening constraints on the NMSSM, and between 0.64 -10 fb (0.70 -7.6 fb) in the high $\mathrm{Y}$ mass search.
DOI: 10.17182/hepdata.158371.v1/t10
title: "Low-mass $\text{Y}\to\gamma\gamma$ limits (2D)" of "Search for the nonresonant and resonant production of a Higgs boson in association with an additional scalar boson in the $γγττ$ final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed and expected 95% CL upper limits on the cross section for the resonant production of a new scalar particle $\mathrm{X}$ which decays to a SM Higgs boson and a new scalar particle $\mathrm{Y}$, multiplied by the $\mathrm{Y} \to \gamma\gamma$ branching fraction, $\sigma(\mathrm{pp} \to \mathrm{X} \to \mathrm{YH})B(\mathrm{Y} \to \gamma\gamma)$. The limits are shown for different values of $m_\mathrm{X}$ in the range 300-1000 GeV and $m_\mathrm{Y}$ in the range 70-125 GeV.
description: The results of a search for the production of two scalar bosons in final states with two photons and two tau leptons are presented. The search considers both nonresonant production of a Higgs boson pair, $\mathrm{HH}$, and resonant production via a new boson $\mathrm{X}$ which decays either to $\mathrm{HH}$ or to $\mathrm{H}$ and a new scalar $\mathrm{Y}$. The analysis uses up to 138 fb$^{-1}$ of proton-proton collision data, recorded between 2016 and 2018 by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV. No evidence for signal is found in the data. For the nonresonant production, the observed (expected) upper limit at 95% confidence level (CL) on the $\mathrm{HH}$ production cross section is set at 930 (740) fb, corresponding to 33 (26) times the standard model prediction. At 95% CL, $\mathrm{HH}$ production is observed (expected) to be excluded for values of $\kappa_\lambda$ outside the range between -12 (-9.4) and 17 (15). Observed (expected) upper limits at 95% CL for the $\mathrm{X} \to \mathrm{HH}$ cross section are found to be within 160 to 2200 (200 to 1800) fb, depending on the mass of $\mathrm{X}$. In the $\mathrm{X} \to \mathrm{YH}$ production scenario, the observed (expected) upper limits vary between 0.059 -1.2 fb (0.87 -0.68 fb) for the $\mathrm{X} \to \mathrm{Y}(\to\tau\tau)\mathrm{H}(\to\gamma\gamma)$ search. For the $\mathrm{X} \to \mathrm{Y}(\to\gamma\gamma)\mathrm{H}(\to\tau\tau)$ search the observed (expected) upper limits vary between 0.69 -15 fb (0.73 -8.3 fb) in the low $\mathrm{Y}$ mass search, tightening constraints on the NMSSM, and between 0.64 -10 fb (0.70 -7.6 fb) in the high $\mathrm{Y}$ mass search.