cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1741545
title: Materials Data on CeSe2 by Materials Project

description: CeSe2 is Low Tridymite-like structured and crystallizes in the tetragonal I4/mcm space group. The structure is three-dimensional. Ce4+ is bonded to four Se2- atoms to form corner-sharing CeSe4 tetrahedra. All Ce–Se bond lengths are 2.73 Å. There are four inequivalent Se2- sites. In the first Se2- site, Se2- is bonded in a bent 150 degrees geometry to two equivalent Ce4+ atoms. In the second Se2- site, Se2- is bonded in a bent 150 degrees geometry to two equivalent Ce4+ atoms. In the third Se2- site, Se2- is bonded in a bent 150 degrees geometry to two equivalent Ce4+ atoms. In the fourth Se2- site, Se2- is bonded in a bent 150 degrees geometry to two equivalent Ce4+ atoms.
DOI: 10.17188/1741546
title: Materials Data on Zr2AlTc by Materials Project

description: Zr2TcAl crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Zr2TcAl ribbons oriented in the (1, 0, 0) direction. Zr is bonded in a linear geometry to one Tc and one Al atom. The Zr–Tc bond length is 2.25 Å. The Zr–Al bond length is 2.83 Å. Tc is bonded in a linear geometry to two equivalent Zr atoms. Al is bonded in a linear geometry to two equivalent Zr atoms.
DOI: 10.17188/1741547
title: Materials Data on C3F5 by Materials Project

description: (CF2)2CF crystallizes in the triclinic P-1 space group. The structure is zero-dimensional and consists of sixteen difluoromethane molecules and eight fluoromethane molecules.
DOI: 10.17188/1741548
title: Materials Data on USiRu by Materials Project

description: URuSi crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. U is bonded in a 11-coordinate geometry to two equivalent U, four equivalent Ru, and five equivalent Si atoms. Both U–U bond lengths are 2.85 Å. There are three shorter (2.96 Å) and one longer (3.06 Å) U–Ru bond lengths. There are a spread of U–Si bond distances ranging from 2.89–3.04 Å. Ru is bonded in a 8-coordinate geometry to four equivalent U and four equivalent Si atoms. There are three shorter (2.46 Å) and one longer (2.47 Å) Ru–Si bond lengths. Si is bonded in a 9-coordinate geometry to five equivalent U and four equivalent Ru atoms.
DOI: 10.17188/1741549
title: Materials Data on Li6Fe2O5F2 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1741550
title: Materials Data on LiVF4 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1741551
title: Materials Data on ZrSbRh by Materials Project

description: ZrRhSb is half-Heusler structured and crystallizes in the cubic F-43m space group. The structure is three-dimensional. Zr is bonded to four equivalent Rh and six equivalent Sb atoms to form a mixture of distorted corner and face-sharing ZrSb6Rh4 tetrahedra. All Zr–Rh bond lengths are 2.75 Å. All Zr–Sb bond lengths are 3.17 Å. Rh is bonded in a body-centered cubic geometry to four equivalent Zr and four equivalent Sb atoms. All Rh–Sb bond lengths are 2.75 Å. Sb is bonded in a 10-coordinate geometry to six equivalent Zr and four equivalent Rh atoms.
DOI: 10.17188/1741552
title: Materials Data on NaAl6Fe3Si6B3O31 by Materials Project

description: NaFe3Al6B3Si6O31 crystallizes in the trigonal R3m space group. The structure is three-dimensional. Na is bonded in a 9-coordinate geometry to nine O atoms. There are a spread of Na–O bond distances ranging from 2.58–2.79 Å. Fe is bonded to six O atoms to form FeO6 octahedra that share corners with two equivalent SiO4 tetrahedra, edges with two equivalent FeO6 octahedra, and edges with two equivalent AlO6 octahedra. There are a spread of Fe–O bond distances ranging from 1.97–2.06 Å. Al is bonded to six O atoms to form AlO6 octahedra that share a cornercorner with one AlO6 octahedra, corners with three equivalent SiO4 tetrahedra, an edgeedge with one FeO6 octahedra, and edges with two equivalent AlO6 octahedra. The corner-sharing octahedral tilt angles are 47°. There are a spread of Al–O bond distances ranging from 1.90–2.02 Å. B is bonded in a trigonal planar geometry to three O atoms. There is two shorter (1.38 Å) and one longer (1.39 Å) B–O bond length. Si is bonded to four O atoms to form SiO4 tetrahedra that share a cornercorner with one FeO6 octahedra, corners with three equivalent AlO6 octahedra, and corners with two equivalent SiO4 tetrahedra. The corner-sharing octahedra tilt angles range from 49–57°. There are a spread of Si–O bond distances ranging from 1.62–1.64 Å. There are eight inequivalent O sites. In the first O site, O is bonded in a distorted bent 150 degrees geometry to one Na and two equivalent Si atoms. In the second O site, O is bonded in a 2-coordinate geometry to one Na and two equivalent Si atoms. In the third O site, O is bonded in a distorted trigonal planar geometry to one Fe, one Al, and one Si atom. In the fourth O site, O is bonded in a distorted trigonal planar geometry to two equivalent Al and one Si atom. In the fifth O site, O is bonded in a distorted trigonal planar geometry to two equivalent Al and one B atom. In the sixth O site, O is bonded in a trigonal non-coplanar geometry to three equivalent Fe atoms. In the seventh O site, O is bonded in a 1-coordinate geometry to one Na, two equivalent Fe, and one B atom. In the eighth O site, O is bonded in a distorted T-shaped geometry to one Fe and two equivalent Al atoms.
DOI: 10.17188/1741553
title: Materials Data on Li3TiCo3O8 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1741554
title: Materials Data on LaCe2Mn3O9 by Materials Project

description: Ce2LaMn3O9 is (Cubic) Perovskite-derived structured and crystallizes in the orthorhombic Cmmm space group. The structure is three-dimensional. Ce+3.50+ is bonded to twelve O2- atoms to form CeO12 cuboctahedra that share corners with five equivalent LaO12 cuboctahedra, corners with seven equivalent CeO12 cuboctahedra, faces with two equivalent LaO12 cuboctahedra, faces with four equivalent CeO12 cuboctahedra, and faces with eight MnO6 octahedra. There are a spread of Ce–O bond distances ranging from 2.74–2.79 Å. La3+ is bonded to twelve O2- atoms to form LaO12 cuboctahedra that share corners with two equivalent LaO12 cuboctahedra, corners with ten equivalent CeO12 cuboctahedra, faces with two equivalent LaO12 cuboctahedra, faces with four equivalent CeO12 cuboctahedra, and faces with eight MnO6 octahedra. There are a spread of La–O bond distances ranging from 2.78–2.80 Å. There are two inequivalent Mn+2.67+ sites. In the first Mn+2.67+ site, Mn+2.67+ is bonded to six O2- atoms to form MnO6 octahedra that share corners with six MnO6 octahedra, faces with four equivalent CeO12 cuboctahedra, and faces with four equivalent LaO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–1°. There is four shorter (1.96 Å) and two longer (1.97 Å) Mn–O bond length. In the second Mn+2.67+ site, Mn+2.67+ is bonded to six O2- atoms to form MnO6 octahedra that share corners with six MnO6 octahedra, faces with two equivalent LaO12 cuboctahedra, and faces with six equivalent CeO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–1°. All Mn–O bond lengths are 1.97 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted linear geometry to two equivalent Ce+3.50+, two equivalent La3+, and two Mn+2.67+ atoms. In the second O2- site, O2- is bonded in a distorted linear geometry to four equivalent Ce+3.50+ and two equivalent Mn+2.67+ atoms. In the third O2- site, O2- is bonded in a distorted linear geometry to three equivalent Ce+3.50+, one La3+, and two equivalent Mn+2.67+ atoms. In the fourth O2- site, O2- is bonded in a distorted linear geometry to two equivalent Ce+3.50+, two equivalent La3+, and two equivalent Mn+2.67+ atoms.
DOI: 10.17188/1741555
title: Materials Data on Li3Co4TeO8 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1741556
title: Materials Data on MnCoO4 by Materials Project

description: MnCoO4 is Hydrophilite-derived structured and crystallizes in the orthorhombic Imma space group. The structure is three-dimensional. Mn4+ is bonded to six O2- atoms to form MnO6 octahedra that share corners with eight equivalent CoO6 octahedra and edges with two equivalent MnO6 octahedra. The corner-sharing octahedra tilt angles range from 48–52°. There are a spread of Mn–O bond distances ranging from 1.91–1.94 Å. Co4+ is bonded to six O2- atoms to form CoO6 octahedra that share corners with eight equivalent MnO6 octahedra and edges with two equivalent CoO6 octahedra. The corner-sharing octahedra tilt angles range from 48–52°. There is two shorter (1.84 Å) and four longer (1.88 Å) Co–O bond length. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to one Mn4+ and two equivalent Co4+ atoms. In the second O2- site, O2- is bonded in a distorted trigonal planar geometry to two equivalent Mn4+ and one Co4+ atom.
DOI: 10.17188/1741557
title: Materials Data on ZrCrP by Materials Project

description: ZrCrP crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Zr is bonded in a 5-coordinate geometry to five equivalent P atoms. There are a spread of Zr–P bond distances ranging from 2.67–2.77 Å. Cr is bonded in a 4-coordinate geometry to four equivalent P atoms. There are a spread of Cr–P bond distances ranging from 2.42–2.52 Å. P is bonded in a 9-coordinate geometry to five equivalent Zr and four equivalent Cr atoms.
DOI: 10.17188/1741558
title: Materials Data on ZnCuP2O7 by Materials Project

description: CuZnP2O7 crystallizes in the monoclinic C2 space group. The structure is three-dimensional. Cu2+ is bonded to six O2- atoms to form distorted CuO6 octahedra that share corners with six equivalent PO4 tetrahedra. There are a spread of Cu–O bond distances ranging from 1.96–2.47 Å. Zn2+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Zn–O bond distances ranging from 1.99–2.65 Å. P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with three equivalent CuO6 octahedra and a cornercorner with one PO4 tetrahedra. The corner-sharing octahedra tilt angles range from 40–58°. There are a spread of P–O bond distances ranging from 1.52–1.60 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a 2-coordinate geometry to one Cu2+, one Zn2+, and one P5+ atom. In the second O2- site, O2- is bonded in a 2-coordinate geometry to one Cu2+, one Zn2+, and one P5+ atom. In the third O2- site, O2- is bonded in a distorted trigonal planar geometry to one Cu2+, one Zn2+, and one P5+ atom. In the fourth O2- site, O2- is bonded in a linear geometry to two equivalent P5+ atoms.
DOI: 10.17188/1741559
title: Materials Data on Li8(FeO2)5 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1741560
title: Materials Data on Bi14MoO24 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.5517/ccdc.csd.cc24bmx1
title: CCDC 1976433: Experimental Crystal Structure Determination

description: Related Article: Jing Yang, Hao-Ji Fang, Qian Cao, Zong-Wan Mao|2021|Chem.Commun.|57|1093|doi:10.1039/D0CC07104H
DOI: 10.17188/1741561
title: Materials Data on ErCoO3 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1741562
title: Materials Data on Li2FeSiO4 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1741563
title: Materials Data on V6H4O13 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1741565
title: Materials Data on BaDyFe4O7 by Materials Project

description: BaDyFe4O7 is Hausmannite-derived structured and crystallizes in the monoclinic P2_1 space group. The structure is three-dimensional. Ba2+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Ba–O bond distances ranging from 2.78–3.01 Å. Dy3+ is bonded to six O2- atoms to form DyO6 octahedra that share corners with twelve FeO4 tetrahedra. There are a spread of Dy–O bond distances ranging from 2.25–2.36 Å. There are four inequivalent Fe+2.25+ sites. In the first Fe+2.25+ site, Fe+2.25+ is bonded to four O2- atoms to form FeO4 tetrahedra that share corners with three equivalent DyO6 octahedra and corners with six FeO4 tetrahedra. The corner-sharing octahedra tilt angles range from 47–58°. There are a spread of Fe–O bond distances ranging from 1.91–1.95 Å. In the second Fe+2.25+ site, Fe+2.25+ is bonded to four O2- atoms to form FeO4 tetrahedra that share corners with three equivalent DyO6 octahedra and corners with six FeO4 tetrahedra. The corner-sharing octahedra tilt angles range from 53–67°. There are a spread of Fe–O bond distances ranging from 1.97–2.07 Å. In the third Fe+2.25+ site, Fe+2.25+ is bonded to four O2- atoms to form FeO4 tetrahedra that share corners with three equivalent DyO6 octahedra and corners with six FeO4 tetrahedra. The corner-sharing octahedra tilt angles range from 52–67°. There are a spread of Fe–O bond distances ranging from 2.00–2.08 Å. In the fourth Fe+2.25+ site, Fe+2.25+ is bonded to four O2- atoms to form FeO4 tetrahedra that share corners with three equivalent DyO6 octahedra and corners with six FeO4 tetrahedra. The corner-sharing octahedra tilt angles range from 48–64°. There are a spread of Fe–O bond distances ranging from 1.97–2.13 Å. There are seven inequivalent O2- sites. In the first O2- site, O2- is bonded in a 3-coordinate geometry to one Ba2+, one Dy3+, and two Fe+2.25+ atoms. In the second O2- site, O2- is bonded in a 4-coordinate geometry to one Ba2+, one Dy3+, and two Fe+2.25+ atoms. In the third O2- site, O2- is bonded in a 4-coordinate geometry to one Ba2+, one Dy3+, and two Fe+2.25+ atoms. In the fourth O2- site, O2- is bonded in a 4-coordinate geometry to one Ba2+, one Dy3+, and two Fe+2.25+ atoms. In the fifth O2- site, O2- is bonded to one Ba2+, one Dy3+, and two Fe+2.25+ atoms to form distorted corner-sharing OBaDyFe2 tetrahedra. In the sixth O2- site, O2- is bonded in a 4-coordinate geometry to one Ba2+, one Dy3+, and two Fe+2.25+ atoms. In the seventh O2- site, O2- is bonded to four Fe+2.25+ atoms to form corner-sharing OFe4 tetrahedra.
DOI: 10.17188/1741566
title: Materials Data on Tb2CoGe2 by Materials Project

description: Tb2CoGe2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Tb sites. In the first Tb site, Tb is bonded in a 6-coordinate geometry to two equivalent Co and six Ge atoms. Both Tb–Co bond lengths are 3.19 Å. There are a spread of Tb–Ge bond distances ranging from 2.91–3.10 Å. In the second Tb site, Tb is bonded in a 2-coordinate geometry to four equivalent Co and seven Ge atoms. There are a spread of Tb–Co bond distances ranging from 3.03–3.12 Å. There are a spread of Tb–Ge bond distances ranging from 2.93–3.24 Å. Co is bonded in a 10-coordinate geometry to six Tb and four Ge atoms. There are a spread of Co–Ge bond distances ranging from 2.40–2.55 Å. There are two inequivalent Ge sites. In the first Ge site, Ge is bonded in a 9-coordinate geometry to seven Tb, one Co, and one Ge atom. The Ge–Ge bond length is 2.70 Å. In the second Ge site, Ge is bonded in a 10-coordinate geometry to six Tb, three equivalent Co, and one Ge atom. The Ge–Ge bond length is 2.85 Å.
DOI: 10.17188/1741567
title: Materials Data on NaCuSI by Materials Project

description: NaCuSI is alpha Po-derived structured and crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. Na1+ is bonded to four equivalent S2- and two equivalent I1- atoms to form NaS4I2 octahedra that share corners with six equivalent NaS4I2 octahedra, edges with four equivalent NaS4I2 octahedra, and edges with eight equivalent CuS2I4 octahedra. The corner-sharing octahedral tilt angles are 0°. All Na–S bond lengths are 2.81 Å. Both Na–I bond lengths are 2.84 Å. Cu2+ is bonded to two equivalent S2- and four equivalent I1- atoms to form CuS2I4 octahedra that share corners with six equivalent CuS2I4 octahedra, edges with four equivalent CuS2I4 octahedra, and edges with eight equivalent NaS4I2 octahedra. The corner-sharing octahedral tilt angles are 0°. Both Cu–S bond lengths are 2.84 Å. All Cu–I bond lengths are 2.81 Å. S2- is bonded to four equivalent Na1+ and two equivalent Cu2+ atoms to form SNa4Cu2 octahedra that share corners with six equivalent SNa4Cu2 octahedra, edges with four equivalent SNa4Cu2 octahedra, and edges with eight equivalent INa2Cu4 octahedra. The corner-sharing octahedral tilt angles are 0°. I1- is bonded to two equivalent Na1+ and four equivalent Cu2+ atoms to form INa2Cu4 octahedra that share corners with six equivalent INa2Cu4 octahedra, edges with four equivalent INa2Cu4 octahedra, and edges with eight equivalent SNa4Cu2 octahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1741568
title: Materials Data on TlC4S4N by Materials Project

description: TlC4NS4 crystallizes in the triclinic P-1 space group. The structure is one-dimensional and consists of one TlC4NS4 ribbon oriented in the (1, 0, 0) direction. Tl1+ is bonded in a 5-coordinate geometry to five S2- atoms. There are a spread of Tl–S bond distances ranging from 3.00–3.75 Å. There are four inequivalent C+2.50+ sites. In the first C+2.50+ site, C+2.50+ is bonded in a linear geometry to two C+2.50+ atoms. There is one shorter (1.26 Å) and one longer (1.30 Å) C–C bond length. In the second C+2.50+ site, C+2.50+ is bonded in a distorted single-bond geometry to one C+2.50+ and one N3- atom. The C–N bond length is 1.27 Å. In the third C+2.50+ site, C+2.50+ is bonded in a linear geometry to one C+2.50+ and one S2- atom. The C–S bond length is 1.56 Å. In the fourth C+2.50+ site, C+2.50+ is bonded in a single-bond geometry to one N3- atom. The C–N bond length is 1.21 Å. N3- is bonded in a linear geometry to two C+2.50+ atoms. There are four inequivalent S2- sites. In the first S2- site, S2- is bonded in a distorted single-bond geometry to one Tl1+, one C+2.50+, and one S2- atom. The S–S bond length is 2.70 Å. In the second S2- site, S2- is bonded in a 3-coordinate geometry to two equivalent Tl1+ and one S2- atom. The S–S bond length is 2.02 Å. In the third S2- site, S2- is bonded in a 3-coordinate geometry to one Tl1+ and two S2- atoms. The S–S bond length is 1.99 Å. In the fourth S2- site, S2- is bonded in a distorted trigonal non-coplanar geometry to one Tl1+ and two S2- atoms.
DOI: 10.17188/1741569
title: Materials Data on EuIn4Ni by Materials Project

description: EuNiIn4 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are two inequivalent Eu sites. In the first Eu site, Eu is bonded in a 5-coordinate geometry to two equivalent Ni and thirteen In atoms. There are one shorter (3.46 Å) and one longer (3.51 Å) Eu–Ni bond lengths. There are a spread of Eu–In bond distances ranging from 3.32–3.73 Å. In the second Eu site, Eu is bonded in a 5-coordinate geometry to two equivalent Ni and thirteen In atoms. There are one shorter (3.47 Å) and one longer (3.51 Å) Eu–Ni bond lengths. There are a spread of Eu–In bond distances ranging from 3.30–3.72 Å. There are two inequivalent Ni sites. In the first Ni site, Ni is bonded in a 9-coordinate geometry to two equivalent Eu and seven In atoms. There are a spread of Ni–In bond distances ranging from 2.56–2.79 Å. In the second Ni site, Ni is bonded in a 9-coordinate geometry to two equivalent Eu and seven In atoms. There are a spread of Ni–In bond distances ranging from 2.56–2.79 Å. There are eight inequivalent In sites. In the first In site, In is bonded in a 12-coordinate geometry to three Eu, three Ni, and one In atom. The In–In bond length is 3.23 Å. In the second In site, In is bonded in a 12-coordinate geometry to three Eu, three Ni, and one In atom. The In–In bond length is 3.23 Å. In the third In site, In is bonded in a 2-coordinate geometry to three Eu, one Ni, and four In atoms. There are a spread of In–In bond distances ranging from 3.15–3.19 Å. In the fourth In site, In is bonded in a 12-coordinate geometry to three Eu, three Ni, and one In atom. The In–In bond length is 3.24 Å. In the fifth In site, In is bonded in a 2-coordinate geometry to three Eu, one Ni, and four In atoms. There are a spread of In–In bond distances ranging from 3.15–3.18 Å. In the sixth In site, In is bonded in a 10-coordinate geometry to four Eu and six In atoms. In the seventh In site, In is bonded in a 10-coordinate geometry to four Eu and six In atoms. The In–In bond length is 3.25 Å. In the eighth In site, In is bonded in a 12-coordinate geometry to three Eu, three Ni, and one In atom.
DOI: 10.17188/1741570
title: Materials Data on Ca2InHg by Materials Project

description: Ca2HgIn is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ca is bonded in a body-centered cubic geometry to four equivalent Hg and four equivalent In atoms. All Ca–Hg bond lengths are 3.32 Å. All Ca–In bond lengths are 3.32 Å. Hg is bonded in a body-centered cubic geometry to eight equivalent Ca atoms. In is bonded in a body-centered cubic geometry to eight equivalent Ca atoms.
DOI: 10.15468/ezpcct
title: Emesis planeca n. comb. (Lepidoptera: Riodinidae): a new combination revealed by molecular evidence with a description of its morphological variation

description: This dataset contains the digitized treatments in Plazi based on the original journal article Trujano-Ortega, Marysol, Callaghan, Curtis J., García-Vázquez, Uri Omar, Luis-Martínez, Armando, Ávalos-Hernández, Omar, Llorente-Bousquets, Jorge (2020): Emesis planeca n. comb. (Lepidoptera: Riodinidae): a new combination revealed by molecular evidence with a description of its morphological variation. Zootaxa 4853 (2): 218-234, DOI: https://doi.org/10.11646/zootaxa.4853.2.4