cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.154965.v1/t22
title: "Figure 8 (right,observed, fix others)" of "Search for $\gamma$H production and constraints on the Yukawa couplings of light quarks to the Higgs boson"

description: Constraints on the square of $|c_{\gamma\gamma}|$ (or $|\tilde{c}_{\gamma\gamma}|$) and $|c_{z\gamma}|$ (or $|\tilde{c}_{z\gamma}|$) from the combination of the $H\to b \bar b$ and $4\ell$ channels. The other couplings are either fixed to the null SM expectation (blue) or are left floating in the fit (red). Observed (solid) and expected (dashed) likelihood scans are shown. The dashed horizontal lines show the 68% and 95% CL intervals.
description: A search for $\gamma$H production is performed with the data from the CMS experiment at the LHC corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ at a proton-proton center-of-mass collision energy of $13~\mathrm{TeV}$. The analysis focuses on the topology of a boosted Higgs boson recoiling against a high-energy photon. The final states of H$\to{\text b}\bar{\text b}$ and $4\ell$ are analyzed. This study examines effective HZ$\gamma$ and H$\gamma\gamma$ anomalous couplings within the context of an effective field theory. In this approach, the production cross section for $\gamma$H is constrained to be $\sigma_{\gamma\mathrm{H}}&lt;16.4\,$fb at $95\%$ confidence level (CL). Simultaneous constraints on four anomalous couplings involving HZ$\gamma$ and H$\gamma\gamma$ are provided. Additionally, the production rate for H$\to4\ell$ is examined to assess potential enhancements in the Yukawa couplings between light quarks and the Higgs boson. Assuming the standard model values for the Yukawa couplings of the bottom and top quarks, the following simultaneous constraints are obtained: $\kappa_\mathrm{u}=(0.0\pm1.5)\times10^{3}$, $\kappa_\mathrm{d}=(0.0\pm7.1)\times10^{2}$, $\kappa_\mathrm{s}=0^{+33}_{-34}$, and $\kappa_\mathrm{c}=0.0^{+2.7}_{-3.0}$. This rules out the hypothesis that up-type or down-type quarks in the first or second generation have the same Yukawa couplings as those in the third generation, with a CL greater than $95\%$.
DOI: 10.17182/hepdata.154965.v1/t23
title: "Figure 8 (right,expected, fix others)" of "Search for $\gamma$H production and constraints on the Yukawa couplings of light quarks to the Higgs boson"

description: Constraints on the square of $|c_{\gamma\gamma}|$ (or $|\tilde{c}_{\gamma\gamma}|$) and $|c_{z\gamma}|$ (or $|\tilde{c}_{z\gamma}|$) from the combination of the $H\to b \bar b$ and $4\ell$ channels. The other couplings are either fixed to the null SM expectation (blue) or are left floating in the fit (red). Observed (solid) and expected (dashed) likelihood scans are shown. The dashed horizontal lines show the 68% and 95% CL intervals.
description: A search for $\gamma$H production is performed with the data from the CMS experiment at the LHC corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ at a proton-proton center-of-mass collision energy of $13~\mathrm{TeV}$. The analysis focuses on the topology of a boosted Higgs boson recoiling against a high-energy photon. The final states of H$\to{\text b}\bar{\text b}$ and $4\ell$ are analyzed. This study examines effective HZ$\gamma$ and H$\gamma\gamma$ anomalous couplings within the context of an effective field theory. In this approach, the production cross section for $\gamma$H is constrained to be $\sigma_{\gamma\mathrm{H}}&lt;16.4\,$fb at $95\%$ confidence level (CL). Simultaneous constraints on four anomalous couplings involving HZ$\gamma$ and H$\gamma\gamma$ are provided. Additionally, the production rate for H$\to4\ell$ is examined to assess potential enhancements in the Yukawa couplings between light quarks and the Higgs boson. Assuming the standard model values for the Yukawa couplings of the bottom and top quarks, the following simultaneous constraints are obtained: $\kappa_\mathrm{u}=(0.0\pm1.5)\times10^{3}$, $\kappa_\mathrm{d}=(0.0\pm7.1)\times10^{2}$, $\kappa_\mathrm{s}=0^{+33}_{-34}$, and $\kappa_\mathrm{c}=0.0^{+2.7}_{-3.0}$. This rules out the hypothesis that up-type or down-type quarks in the first or second generation have the same Yukawa couplings as those in the third generation, with a CL greater than $95\%$.
DOI: 10.17182/hepdata.154965.v1/t24
title: "Figure 9 (upper left,observed, float all)" of "Search for $\gamma$H production and constraints on the Yukawa couplings of light quarks to the Higgs boson"

description: Constraints on $\kappa_{u}$, $\kappa_{d}$, $\kappa_{s}$, and $\kappa_{c}$ are shown using the $H\to 4\ell$ channel.In scenario one (black), all couplings except the one being shown are fixed at their SM values. In scenario two (blue), the Yukawa couplings for the three other light quarks are left unconstrained, and BSM contributions are allowed: $\kappa_{ZZ}^2 \le 1$ and $\Gamma^\textrm{BSM}_H \ge 0$. Both observed (solid) and expected (dashed) constraints are presented. The dashed horizontal lines indicate the 68% and 95% CL intervals.
description: A search for $\gamma$H production is performed with the data from the CMS experiment at the LHC corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ at a proton-proton center-of-mass collision energy of $13~\mathrm{TeV}$. The analysis focuses on the topology of a boosted Higgs boson recoiling against a high-energy photon. The final states of H$\to{\text b}\bar{\text b}$ and $4\ell$ are analyzed. This study examines effective HZ$\gamma$ and H$\gamma\gamma$ anomalous couplings within the context of an effective field theory. In this approach, the production cross section for $\gamma$H is constrained to be $\sigma_{\gamma\mathrm{H}}&lt;16.4\,$fb at $95\%$ confidence level (CL). Simultaneous constraints on four anomalous couplings involving HZ$\gamma$ and H$\gamma\gamma$ are provided. Additionally, the production rate for H$\to4\ell$ is examined to assess potential enhancements in the Yukawa couplings between light quarks and the Higgs boson. Assuming the standard model values for the Yukawa couplings of the bottom and top quarks, the following simultaneous constraints are obtained: $\kappa_\mathrm{u}=(0.0\pm1.5)\times10^{3}$, $\kappa_\mathrm{d}=(0.0\pm7.1)\times10^{2}$, $\kappa_\mathrm{s}=0^{+33}_{-34}$, and $\kappa_\mathrm{c}=0.0^{+2.7}_{-3.0}$. This rules out the hypothesis that up-type or down-type quarks in the first or second generation have the same Yukawa couplings as those in the third generation, with a CL greater than $95\%$.
DOI: 10.17182/hepdata.154965.v1/t25
title: "Figure 9 (upper left,expected, float all)" of "Search for $\gamma$H production and constraints on the Yukawa couplings of light quarks to the Higgs boson"

description: Constraints on $\kappa_{u}$, $\kappa_{d}$, $\kappa_{s}$, and $\kappa_{c}$ are shown using the $H\to 4\ell$ channel.In scenario one (black), all couplings except the one being shown are fixed at their SM values. In scenario two (blue), the Yukawa couplings for the three other light quarks are left unconstrained, and BSM contributions are allowed: $\kappa_{ZZ}^2 \le 1$ and $\Gamma^\textrm{BSM}_H \ge 0$. Both observed (solid) and expected (dashed) constraints are presented. The dashed horizontal lines indicate the 68% and 95% CL intervals.
description: A search for $\gamma$H production is performed with the data from the CMS experiment at the LHC corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ at a proton-proton center-of-mass collision energy of $13~\mathrm{TeV}$. The analysis focuses on the topology of a boosted Higgs boson recoiling against a high-energy photon. The final states of H$\to{\text b}\bar{\text b}$ and $4\ell$ are analyzed. This study examines effective HZ$\gamma$ and H$\gamma\gamma$ anomalous couplings within the context of an effective field theory. In this approach, the production cross section for $\gamma$H is constrained to be $\sigma_{\gamma\mathrm{H}}&lt;16.4\,$fb at $95\%$ confidence level (CL). Simultaneous constraints on four anomalous couplings involving HZ$\gamma$ and H$\gamma\gamma$ are provided. Additionally, the production rate for H$\to4\ell$ is examined to assess potential enhancements in the Yukawa couplings between light quarks and the Higgs boson. Assuming the standard model values for the Yukawa couplings of the bottom and top quarks, the following simultaneous constraints are obtained: $\kappa_\mathrm{u}=(0.0\pm1.5)\times10^{3}$, $\kappa_\mathrm{d}=(0.0\pm7.1)\times10^{2}$, $\kappa_\mathrm{s}=0^{+33}_{-34}$, and $\kappa_\mathrm{c}=0.0^{+2.7}_{-3.0}$. This rules out the hypothesis that up-type or down-type quarks in the first or second generation have the same Yukawa couplings as those in the third generation, with a CL greater than $95\%$.
DOI: 10.17182/hepdata.154965.v1/t26
title: "Figure 9 (upper left,observed, fix others)" of "Search for $\gamma$H production and constraints on the Yukawa couplings of light quarks to the Higgs boson"

description: Constraints on $\kappa_{u}$, $\kappa_{d}$, $\kappa_{s}$, and $\kappa_{c}$ are shown using the $H\to 4\ell$ channel.In scenario one (black), all couplings except the one being shown are fixed at their SM values. In scenario two (blue), the Yukawa couplings for the three other light quarks are left unconstrained, and BSM contributions are allowed: $\kappa_{ZZ}^2 \le 1$ and $\Gamma^\textrm{BSM}_H \ge 0$. Both observed (solid) and expected (dashed) constraints are presented. The dashed horizontal lines indicate the 68% and 95% CL intervals.
description: A search for $\gamma$H production is performed with the data from the CMS experiment at the LHC corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ at a proton-proton center-of-mass collision energy of $13~\mathrm{TeV}$. The analysis focuses on the topology of a boosted Higgs boson recoiling against a high-energy photon. The final states of H$\to{\text b}\bar{\text b}$ and $4\ell$ are analyzed. This study examines effective HZ$\gamma$ and H$\gamma\gamma$ anomalous couplings within the context of an effective field theory. In this approach, the production cross section for $\gamma$H is constrained to be $\sigma_{\gamma\mathrm{H}}&lt;16.4\,$fb at $95\%$ confidence level (CL). Simultaneous constraints on four anomalous couplings involving HZ$\gamma$ and H$\gamma\gamma$ are provided. Additionally, the production rate for H$\to4\ell$ is examined to assess potential enhancements in the Yukawa couplings between light quarks and the Higgs boson. Assuming the standard model values for the Yukawa couplings of the bottom and top quarks, the following simultaneous constraints are obtained: $\kappa_\mathrm{u}=(0.0\pm1.5)\times10^{3}$, $\kappa_\mathrm{d}=(0.0\pm7.1)\times10^{2}$, $\kappa_\mathrm{s}=0^{+33}_{-34}$, and $\kappa_\mathrm{c}=0.0^{+2.7}_{-3.0}$. This rules out the hypothesis that up-type or down-type quarks in the first or second generation have the same Yukawa couplings as those in the third generation, with a CL greater than $95\%$.
DOI: 10.17182/hepdata.154965.v1/t27
title: "Figure 9 (upper left,expected, fix others)" of "Search for $\gamma$H production and constraints on the Yukawa couplings of light quarks to the Higgs boson"

description: Constraints on $\kappa_{u}$, $\kappa_{d}$, $\kappa_{s}$, and $\kappa_{c}$ are shown using the $H\to 4\ell$ channel.In scenario one (black), all couplings except the one being shown are fixed at their SM values. In scenario two (blue), the Yukawa couplings for the three other light quarks are left unconstrained, and BSM contributions are allowed: $\kappa_{ZZ}^2 \le 1$ and $\Gamma^\textrm{BSM}_H \ge 0$. Both observed (solid) and expected (dashed) constraints are presented. The dashed horizontal lines indicate the 68% and 95% CL intervals.
description: A search for $\gamma$H production is performed with the data from the CMS experiment at the LHC corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ at a proton-proton center-of-mass collision energy of $13~\mathrm{TeV}$. The analysis focuses on the topology of a boosted Higgs boson recoiling against a high-energy photon. The final states of H$\to{\text b}\bar{\text b}$ and $4\ell$ are analyzed. This study examines effective HZ$\gamma$ and H$\gamma\gamma$ anomalous couplings within the context of an effective field theory. In this approach, the production cross section for $\gamma$H is constrained to be $\sigma_{\gamma\mathrm{H}}&lt;16.4\,$fb at $95\%$ confidence level (CL). Simultaneous constraints on four anomalous couplings involving HZ$\gamma$ and H$\gamma\gamma$ are provided. Additionally, the production rate for H$\to4\ell$ is examined to assess potential enhancements in the Yukawa couplings between light quarks and the Higgs boson. Assuming the standard model values for the Yukawa couplings of the bottom and top quarks, the following simultaneous constraints are obtained: $\kappa_\mathrm{u}=(0.0\pm1.5)\times10^{3}$, $\kappa_\mathrm{d}=(0.0\pm7.1)\times10^{2}$, $\kappa_\mathrm{s}=0^{+33}_{-34}$, and $\kappa_\mathrm{c}=0.0^{+2.7}_{-3.0}$. This rules out the hypothesis that up-type or down-type quarks in the first or second generation have the same Yukawa couplings as those in the third generation, with a CL greater than $95\%$.
DOI: 10.17182/hepdata.154965.v1/t28
title: "Figure 9 (upper right,observed, float all)" of "Search for $\gamma$H production and constraints on the Yukawa couplings of light quarks to the Higgs boson"

description: Constraints on $\kappa_{u}$, $\kappa_{d}$, $\kappa_{s}$, and $\kappa_{c}$ are shown using the $H\to 4\ell$ channel.In scenario one (black), all couplings except the one being shown are fixed at their SM values. In scenario two (blue), the Yukawa couplings for the three other light quarks are left unconstrained, and BSM contributions are allowed: $\kappa_{ZZ}^2 \le 1$ and $\Gamma^\textrm{BSM}_H \ge 0$. Both observed (solid) and expected (dashed) constraints are presented. The dashed horizontal lines indicate the 68% and 95% CL intervals.
description: A search for $\gamma$H production is performed with the data from the CMS experiment at the LHC corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ at a proton-proton center-of-mass collision energy of $13~\mathrm{TeV}$. The analysis focuses on the topology of a boosted Higgs boson recoiling against a high-energy photon. The final states of H$\to{\text b}\bar{\text b}$ and $4\ell$ are analyzed. This study examines effective HZ$\gamma$ and H$\gamma\gamma$ anomalous couplings within the context of an effective field theory. In this approach, the production cross section for $\gamma$H is constrained to be $\sigma_{\gamma\mathrm{H}}&lt;16.4\,$fb at $95\%$ confidence level (CL). Simultaneous constraints on four anomalous couplings involving HZ$\gamma$ and H$\gamma\gamma$ are provided. Additionally, the production rate for H$\to4\ell$ is examined to assess potential enhancements in the Yukawa couplings between light quarks and the Higgs boson. Assuming the standard model values for the Yukawa couplings of the bottom and top quarks, the following simultaneous constraints are obtained: $\kappa_\mathrm{u}=(0.0\pm1.5)\times10^{3}$, $\kappa_\mathrm{d}=(0.0\pm7.1)\times10^{2}$, $\kappa_\mathrm{s}=0^{+33}_{-34}$, and $\kappa_\mathrm{c}=0.0^{+2.7}_{-3.0}$. This rules out the hypothesis that up-type or down-type quarks in the first or second generation have the same Yukawa couplings as those in the third generation, with a CL greater than $95\%$.
DOI: 10.17182/hepdata.154965.v1/t29
title: "Figure 9 (upper right,expected, float all)" of "Search for $\gamma$H production and constraints on the Yukawa couplings of light quarks to the Higgs boson"

description: Constraints on $\kappa_{u}$, $\kappa_{d}$, $\kappa_{s}$, and $\kappa_{c}$ are shown using the $H\to 4\ell$ channel.In scenario one (black), all couplings except the one being shown are fixed at their SM values. In scenario two (blue), the Yukawa couplings for the three other light quarks are left unconstrained, and BSM contributions are allowed: $\kappa_{ZZ}^2 \le 1$ and $\Gamma^\textrm{BSM}_H \ge 0$. Both observed (solid) and expected (dashed) constraints are presented. The dashed horizontal lines indicate the 68% and 95% CL intervals.
description: A search for $\gamma$H production is performed with the data from the CMS experiment at the LHC corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ at a proton-proton center-of-mass collision energy of $13~\mathrm{TeV}$. The analysis focuses on the topology of a boosted Higgs boson recoiling against a high-energy photon. The final states of H$\to{\text b}\bar{\text b}$ and $4\ell$ are analyzed. This study examines effective HZ$\gamma$ and H$\gamma\gamma$ anomalous couplings within the context of an effective field theory. In this approach, the production cross section for $\gamma$H is constrained to be $\sigma_{\gamma\mathrm{H}}&lt;16.4\,$fb at $95\%$ confidence level (CL). Simultaneous constraints on four anomalous couplings involving HZ$\gamma$ and H$\gamma\gamma$ are provided. Additionally, the production rate for H$\to4\ell$ is examined to assess potential enhancements in the Yukawa couplings between light quarks and the Higgs boson. Assuming the standard model values for the Yukawa couplings of the bottom and top quarks, the following simultaneous constraints are obtained: $\kappa_\mathrm{u}=(0.0\pm1.5)\times10^{3}$, $\kappa_\mathrm{d}=(0.0\pm7.1)\times10^{2}$, $\kappa_\mathrm{s}=0^{+33}_{-34}$, and $\kappa_\mathrm{c}=0.0^{+2.7}_{-3.0}$. This rules out the hypothesis that up-type or down-type quarks in the first or second generation have the same Yukawa couplings as those in the third generation, with a CL greater than $95\%$.
DOI: 10.3535/4ps-z72-1v3
title: Cyaniris semiargus (von Rottemburg, 1775)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/j17-zz7-pde
title: Lycaena phlaeas (Linnaeus, 1761)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.17182/hepdata.154965.v1/t30
title: "Figure 9 (upper right,observed, fix others)" of "Search for $\gamma$H production and constraints on the Yukawa couplings of light quarks to the Higgs boson"

description: Constraints on $\kappa_{u}$, $\kappa_{d}$, $\kappa_{s}$, and $\kappa_{c}$ are shown using the $H\to 4\ell$ channel.In scenario one (black), all couplings except the one being shown are fixed at their SM values. In scenario two (blue), the Yukawa couplings for the three other light quarks are left unconstrained, and BSM contributions are allowed: $\kappa_{ZZ}^2 \le 1$ and $\Gamma^\textrm{BSM}_H \ge 0$. Both observed (solid) and expected (dashed) constraints are presented. The dashed horizontal lines indicate the 68% and 95% CL intervals.
description: A search for $\gamma$H production is performed with the data from the CMS experiment at the LHC corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ at a proton-proton center-of-mass collision energy of $13~\mathrm{TeV}$. The analysis focuses on the topology of a boosted Higgs boson recoiling against a high-energy photon. The final states of H$\to{\text b}\bar{\text b}$ and $4\ell$ are analyzed. This study examines effective HZ$\gamma$ and H$\gamma\gamma$ anomalous couplings within the context of an effective field theory. In this approach, the production cross section for $\gamma$H is constrained to be $\sigma_{\gamma\mathrm{H}}&lt;16.4\,$fb at $95\%$ confidence level (CL). Simultaneous constraints on four anomalous couplings involving HZ$\gamma$ and H$\gamma\gamma$ are provided. Additionally, the production rate for H$\to4\ell$ is examined to assess potential enhancements in the Yukawa couplings between light quarks and the Higgs boson. Assuming the standard model values for the Yukawa couplings of the bottom and top quarks, the following simultaneous constraints are obtained: $\kappa_\mathrm{u}=(0.0\pm1.5)\times10^{3}$, $\kappa_\mathrm{d}=(0.0\pm7.1)\times10^{2}$, $\kappa_\mathrm{s}=0^{+33}_{-34}$, and $\kappa_\mathrm{c}=0.0^{+2.7}_{-3.0}$. This rules out the hypothesis that up-type or down-type quarks in the first or second generation have the same Yukawa couplings as those in the third generation, with a CL greater than $95\%$.
DOI: 10.17182/hepdata.154965.v1/t31
title: "Figure 9 (upper right,expected, fix others)" of "Search for $\gamma$H production and constraints on the Yukawa couplings of light quarks to the Higgs boson"

description: Constraints on $\kappa_{u}$, $\kappa_{d}$, $\kappa_{s}$, and $\kappa_{c}$ are shown using the $H\to 4\ell$ channel.In scenario one (black), all couplings except the one being shown are fixed at their SM values. In scenario two (blue), the Yukawa couplings for the three other light quarks are left unconstrained, and BSM contributions are allowed: $\kappa_{ZZ}^2 \le 1$ and $\Gamma^\textrm{BSM}_H \ge 0$. Both observed (solid) and expected (dashed) constraints are presented. The dashed horizontal lines indicate the 68% and 95% CL intervals.
description: A search for $\gamma$H production is performed with the data from the CMS experiment at the LHC corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ at a proton-proton center-of-mass collision energy of $13~\mathrm{TeV}$. The analysis focuses on the topology of a boosted Higgs boson recoiling against a high-energy photon. The final states of H$\to{\text b}\bar{\text b}$ and $4\ell$ are analyzed. This study examines effective HZ$\gamma$ and H$\gamma\gamma$ anomalous couplings within the context of an effective field theory. In this approach, the production cross section for $\gamma$H is constrained to be $\sigma_{\gamma\mathrm{H}}&lt;16.4\,$fb at $95\%$ confidence level (CL). Simultaneous constraints on four anomalous couplings involving HZ$\gamma$ and H$\gamma\gamma$ are provided. Additionally, the production rate for H$\to4\ell$ is examined to assess potential enhancements in the Yukawa couplings between light quarks and the Higgs boson. Assuming the standard model values for the Yukawa couplings of the bottom and top quarks, the following simultaneous constraints are obtained: $\kappa_\mathrm{u}=(0.0\pm1.5)\times10^{3}$, $\kappa_\mathrm{d}=(0.0\pm7.1)\times10^{2}$, $\kappa_\mathrm{s}=0^{+33}_{-34}$, and $\kappa_\mathrm{c}=0.0^{+2.7}_{-3.0}$. This rules out the hypothesis that up-type or down-type quarks in the first or second generation have the same Yukawa couplings as those in the third generation, with a CL greater than $95\%$.