cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.154965.v1/t32
title: "Figure 9 (lower 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/t33
title: "Figure 9 (lower 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/t34
title: "Figure 9 (lower 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/t35
title: "Figure 9 (lower 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/t36
title: "Figure 9 ( lower 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/t37
title: "Figure 9 ( lower 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: 10.3535/7gh-60s-mfx
title: Ochropacha duplaris (Linnaeus, 1761)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/plz-t10-63m
title: Agrochola (Anchoscelis) Guenée, 1839

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.17182/hepdata.154965.v1/t38
title: "Figure 9 ( lower 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/t39
title: "Figure 9 ( lower 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 $95\%$.
DOI: 10.3535/xwn-f6w-w9b
title: Exaeretia ciniflonella Zeller, 1846

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/7h0-c5f-174
title: Scopariinae

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/838-nva-7km
title: Parastichtis suspecta Hübner, 1809

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/f49-jpg-9t0
title: Sedina buettneri Hering, 1858

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/sag-ajp-jbv
title: Glaucopsyche alexis (Poda, 1761)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/xpm-70d-y3p
title: Euxoa (Euxoa) tritici Linnaeus, 1761

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/dmr-cmv-l89
title: Cyaniris semiargus (von Rottemburg, 1775)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/j7h-1wk-h9h
title: Agriphila poliellus Treitschke, 1832

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/t91-nzb-arv
title: Catoptria falsella [Denis & Schiffermüller], 1775

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/b0n-hx7-11z
title: Scopariinae

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/nyq-8ew-cc9
title: Eupsilia transversa Hufnagel, 1766

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/a36-kck-70r
title: Amphipoea fucosa Freyer, 1830

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/h1e-eh3-p1g
title: Parastichtis suspecta Hübner, 1809

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/tlj-q1r-3ah
title: Amphipoea fucosa Freyer, 1830

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/wws-qg2-t9c
title: Amphipoea fucosa Freyer, 1830

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/e4x-l3r-l0j
title: Glaucopsyche alexis (Poda, 1761)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/y0t-1rt-e7z
title: Charanyca (Rusina) Stephens, 1829

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/17v-nk2-rva
title: Charanyca (Rusina) Stephens, 1829

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/2xy-sbg-183
title: Lycaena Fabricius, 1807

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/2a6-d29-9rx
title: Agriphila inquinatella [Denis & Schiffermüller], 1775

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/yvr-dyy-r2j
title: Agriphila inquinatella [Denis & Schiffermüller], 1775

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/eyc-d4z-drk
title: Cyaniris semiargus (von Rottemburg, 1775)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/rkp-hgb-cc5
title: Tholera decimalis Poda, 1761

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/3ky-nzv-33l
title: Patania Moore, 1888

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/te2-w9z-r4p
title: Glaucopsyche alexis (Poda, 1761)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/wc6-xwz-d3s
title: Pieris napi (Linnaeus, 1758)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/bed-tz5-ses
title: Bryophila (Bryoleuca) raptricula ([Denis & Schiffermüller], 1775)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/wg3-0va-vrl
title: Cucullia gnaphalii (Hübner, 1813)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/0zd-8d8-l4q
title: Zygaena Fabricius, 1775

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/xb0-2fe-afc
title: Diacrisia sannio (Linnaeus, 1758)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/2dh-60n-yf2
title: Agriphila inquinatella [Denis & Schiffermüller], 1775

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/3zn-ewn-zz5
title: Euxoa (Euxoa) obelisca [Denis & Schiffermüller], 1775

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/lj3-1n8-nr6
title: Glaucopsyche alexis (Poda, 1761)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/m59-ker-amq
title: Mythimna (Mythimna) impura Hübner, 1808

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/srq-jb4-ayr
title: Chersotis cuprea [Denis & Schiffermüller], 1775

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/79p-13v-y8w
title: Tholera decimalis Poda, 1761

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.