cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1724687
title: Materials Data on TbCrTeO6 by Materials Project

description: TbCrTeO6 is beta Vanadium nitride-derived structured and crystallizes in the trigonal P-31c space group. The structure is three-dimensional. Tb3+ is bonded to six equivalent O2- atoms to form TbO6 octahedra that share corners with six equivalent CrO6 octahedra and edges with three equivalent TeO6 octahedra. The corner-sharing octahedral tilt angles are 60°. All Tb–O bond lengths are 2.28 Å. Cr5+ is bonded to six equivalent O2- atoms to form CrO6 octahedra that share corners with six equivalent TbO6 octahedra and corners with six equivalent TeO6 octahedra. The corner-sharing octahedra tilt angles range from 42–60°. All Cr–O bond lengths are 2.10 Å. Te4+ is bonded to six equivalent O2- atoms to form TeO6 octahedra that share corners with six equivalent CrO6 octahedra and edges with three equivalent TbO6 octahedra. The corner-sharing octahedral tilt angles are 42°. All Te–O bond lengths are 1.97 Å. O2- is bonded in a distorted trigonal planar geometry to one Tb3+, one Cr5+, and one Te4+ atom.
DOI: 10.17188/1724688
title: Materials Data on Ca3Zn by Materials Project

description: Ca3Zn is alpha bismuth trifluoride structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. there are two inequivalent Ca sites. In the first Ca site, Ca is bonded in a body-centered cubic geometry to eight equivalent Ca atoms. All Ca–Ca bond lengths are 3.45 Å. In the second Ca site, Ca is bonded to four equivalent Ca and four equivalent Zn atoms to form a mixture of distorted face, edge, and corner-sharing CaCa4Zn4 tetrahedra. All Ca–Zn bond lengths are 3.45 Å. Zn is bonded in a body-centered cubic geometry to eight equivalent Ca atoms.
DOI: 10.17188/1724689
title: Materials Data on LaFe8Si5 by Materials Project

description: LaFe8Si5 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. La3+ is bonded in a 10-coordinate geometry to ten Si4- atoms. There are a spread of La–Si bond distances ranging from 3.19–3.36 Å. There are seven inequivalent Fe+2.12+ sites. In the first Fe+2.12+ site, Fe+2.12+ is bonded to one Fe+2.12+ and four Si4- atoms to form distorted FeFeSi4 tetrahedra that share corners with two equivalent FeFe6Si6 cuboctahedra, corners with two equivalent FeFeSi4 tetrahedra, an edgeedge with one FeFe8Si4 cuboctahedra, an edgeedge with one FeFeSi4 tetrahedra, and a faceface with one FeFeSi4 tetrahedra. The Fe–Fe bond length is 2.48 Å. There are a spread of Fe–Si bond distances ranging from 2.34–2.40 Å. In the second Fe+2.12+ site, Fe+2.12+ is bonded in a 5-coordinate geometry to two Fe+2.12+ and five Si4- atoms. There are one shorter (2.49 Å) and one longer (2.51 Å) Fe–Fe bond lengths. There are a spread of Fe–Si bond distances ranging from 2.35–2.46 Å. In the third Fe+2.12+ site, Fe+2.12+ is bonded to six Fe+2.12+ and six Si4- atoms to form distorted corner-sharing FeFe6Si6 cuboctahedra. Both Fe–Fe bond lengths are 2.41 Å. There are two shorter (2.33 Å) and four longer (2.38 Å) Fe–Si bond lengths. In the fourth Fe+2.12+ site, Fe+2.12+ is bonded to eight Fe+2.12+ and four equivalent Si4- atoms to form distorted edge-sharing FeFe8Si4 cuboctahedra. There are two shorter (2.41 Å) and two longer (2.47 Å) Fe–Fe bond lengths. All Fe–Si bond lengths are 2.35 Å. In the fifth Fe+2.12+ site, Fe+2.12+ is bonded in a 9-coordinate geometry to three Fe+2.12+ and four Si4- atoms. There are one shorter (2.33 Å) and one longer (2.34 Å) Fe–Fe bond lengths. There are two shorter (2.47 Å) and two longer (2.53 Å) Fe–Si bond lengths. In the sixth Fe+2.12+ site, Fe+2.12+ is bonded in a 2-coordinate geometry to one Fe+2.12+ and six Si4- atoms. There are a spread of Fe–Si bond distances ranging from 2.31–2.60 Å. In the seventh Fe+2.12+ site, Fe+2.12+ is bonded in a 10-coordinate geometry to five Fe+2.12+ and five Si4- atoms. There are three shorter (2.51 Å) and two longer (2.53 Å) Fe–Si bond lengths. There are three inequivalent Si4- sites. In the first Si4- site, Si4- is bonded in a 11-coordinate geometry to two equivalent La3+, eight Fe+2.12+, and one Si4- atom. The Si–Si bond length is 2.59 Å. In the second Si4- site, Si4- is bonded in a 11-coordinate geometry to two equivalent La3+, eight Fe+2.12+, and one Si4- atom. The Si–Si bond length is 2.58 Å. In the third Si4- site, Si4- is bonded in a 12-coordinate geometry to two equivalent La3+, six Fe+2.12+, and four Si4- atoms.
DOI: 10.17188/1724690
title: Materials Data on NaMnCrF6 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: 10.17188/1724691
title: Materials Data on NaCr(SO4)2 by Materials Project

description: NaCr(SO4)2 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Na1+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Na–O bond distances ranging from 2.36–2.75 Å. Cr3+ is bonded to six O2- atoms to form CrO6 octahedra that share corners with six SO4 tetrahedra. There are a spread of Cr–O bond distances ranging from 2.00–2.05 Å. There are two inequivalent S6+ sites. In the first S6+ site, S6+ is bonded to four O2- atoms to form SO4 tetrahedra that share corners with three equivalent CrO6 octahedra. The corner-sharing octahedra tilt angles range from 38–41°. There is one shorter (1.45 Å) and three longer (1.50 Å) S–O bond length. In the second S6+ site, S6+ is bonded to four O2- atoms to form SO4 tetrahedra that share corners with three equivalent CrO6 octahedra. The corner-sharing octahedra tilt angles range from 25–39°. There are a spread of S–O bond distances ranging from 1.46–1.50 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Cr3+ and one S6+ atom. In the second O2- site, O2- is bonded in a bent 150 degrees geometry to one Cr3+ and one S6+ atom. In the third O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Na1+ and one S6+ atom. In the fourth O2- site, O2- is bonded in a 1-coordinate geometry to three equivalent Na1+ and one S6+ atom. In the fifth O2- site, O2- is bonded in a bent 150 degrees geometry to one Cr3+ and one S6+ atom. In the sixth O2- site, O2- is bonded in a 3-coordinate geometry to one Na1+, one Cr3+, and one S6+ atom.
DOI: 10.17188/1724692
title: Materials Data on Na2InAgF6 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: 10.17188/1724693
title: Materials Data on YFe6Co5W by Materials Project

description: YWFe6Co5 crystallizes in the orthorhombic Imm2 space group. The structure is three-dimensional. Y is bonded in a 12-coordinate geometry to one W, twelve Fe, and seven Co atoms. The Y–W bond length is 3.16 Å. There are a spread of Y–Fe bond distances ranging from 3.03–3.22 Å. There are a spread of Y–Co bond distances ranging from 2.93–3.04 Å. W is bonded in a 1-coordinate geometry to one Y, six Fe, and seven Co atoms. There are four shorter (2.64 Å) and two longer (2.65 Å) W–Fe bond lengths. There are a spread of W–Co bond distances ranging from 2.36–2.85 Å. There are three inequivalent Fe sites. In the first Fe site, Fe is bonded to two equivalent Y, one W, four Fe, and five Co atoms to form a mixture of distorted corner, edge, and face-sharing FeY2Fe4Co5W cuboctahedra. There are a spread of Fe–Fe bond distances ranging from 2.34–2.43 Å. There are a spread of Fe–Co bond distances ranging from 2.40–2.60 Å. In the second Fe site, Fe is bonded to two equivalent Y, two equivalent W, four equivalent Fe, and four Co atoms to form a mixture of distorted corner, edge, and face-sharing FeY2Fe4Co4W2 cuboctahedra. There are two shorter (2.59 Å) and two longer (2.68 Å) Fe–Co bond lengths. In the third Fe site, Fe is bonded to two equivalent Y, four equivalent Fe, and six Co atoms to form a mixture of corner, edge, and face-sharing FeY2Fe4Co6 cuboctahedra. There are a spread of Fe–Co bond distances ranging from 2.56–2.71 Å. There are three inequivalent Co sites. In the first Co site, Co is bonded in a 12-coordinate geometry to one Y, two equivalent W, six Fe, and five Co atoms. There are a spread of Co–Co bond distances ranging from 2.36–2.92 Å. In the second Co site, Co is bonded in a distorted single-bond geometry to one Y, one W, six Fe, and six Co atoms. Both Co–Co bond lengths are 2.65 Å. In the third Co site, Co is bonded in a 12-coordinate geometry to two equivalent Y, one W, six Fe, and three Co atoms.
DOI: 10.17188/1724694
title: Materials Data on NaHgCl3O2 by Materials Project

description: NaHgO2Cl3 crystallizes in the orthorhombic Pnma space group. The structure is one-dimensional and consists of four NaHgO2Cl3 ribbons oriented in the (1, 0, 0) direction. Na is bonded to three O and one Cl atom to form distorted corner-sharing NaClO3 tetrahedra. There are two shorter (2.32 Å) and one longer (2.36 Å) Na–O bond lengths. The Na–Cl bond length is 2.90 Å. Hg is bonded in a linear geometry to two Cl atoms. There are one shorter (2.35 Å) and one longer (2.37 Å) Hg–Cl bond lengths. There are two inequivalent O sites. In the first O site, O is bonded in a trigonal planar geometry to two equivalent Na and one Cl atom. The O–Cl bond length is 1.64 Å. In the second O site, O is bonded in a single-bond geometry to one Na atom. There are three inequivalent Cl sites. In the first Cl site, Cl is bonded in a water-like geometry to one Na and one Hg atom. In the second Cl site, Cl is bonded in a single-bond geometry to one O atom. In the third Cl site, Cl is bonded in a single-bond geometry to one Hg atom.
DOI: 10.17188/1724695
title: Materials Data on Li9V3P8O29 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: 10.17188/1724696
title: Materials Data on Cr2(PO4)3 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: 10.17188/1724697
title: Materials Data on Ca3(TaN2)2 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: 10.17188/1724698
title: Materials Data on VCd2BiO6 by Materials Project

description: VCd2BiO6 crystallizes in the orthorhombic Cmc2_1 space group. The structure is three-dimensional. V5+ is bonded to four O2- atoms to form VO4 tetrahedra that share corners with eight equivalent CdO6 octahedra. The corner-sharing octahedra tilt angles range from 51–70°. There are a spread of V–O bond distances ranging from 1.72–1.77 Å. Cd2+ is bonded to six O2- atoms to form distorted CdO6 octahedra that share corners with four equivalent CdO6 octahedra, corners with four equivalent VO4 tetrahedra, and an edgeedge with one CdO6 octahedra. The corner-sharing octahedra tilt angles range from 53–65°. There are a spread of Cd–O bond distances ranging from 2.30–2.43 Å. Bi3+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of Bi–O bond distances ranging from 2.26–2.58 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal planar geometry to one V5+ and two equivalent Cd2+ atoms. In the second O2- site, O2- is bonded to two equivalent Cd2+ and two equivalent Bi3+ atoms to form a mixture of edge and corner-sharing OCd2Bi2 tetrahedra. In the third O2- site, O2- is bonded in a 1-coordinate geometry to one V5+, two equivalent Cd2+, and one Bi3+ atom. In the fourth O2- site, O2- is bonded in a 3-coordinate geometry to one V5+ and two equivalent Cd2+ atoms.
DOI: 10.17188/1724699
title: Materials Data on HfTiRu2 by Materials Project

description: HfTiRu2 crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two HfTiRu2 ribbons oriented in the (1, 0, 0) direction. Hf is bonded in a linear geometry to two equivalent Ru atoms. Both Hf–Ru bond lengths are 2.30 Å. Ti is bonded in a linear geometry to two equivalent Ru atoms. Both Ti–Ru bond lengths are 2.12 Å. Ru is bonded in a linear geometry to one Hf and one Ti atom.
DOI: 10.17188/1724700
title: Materials Data on LaAl3Ni2 by Materials Project

description: LaNi2Al3 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. La is bonded in a 7-coordinate geometry to two equivalent La, eight equivalent Ni, and eleven Al atoms. Both La–La bond lengths are 3.51 Å. There are four shorter (3.52 Å) and four longer (3.63 Å) La–Ni bond lengths. There are a spread of La–Al bond distances ranging from 3.18–3.55 Å. Ni is bonded in a 6-coordinate geometry to four equivalent La and six Al atoms. There are a spread of Ni–Al bond distances ranging from 2.40–2.53 Å. There are two inequivalent Al sites. In the first Al site, Al is bonded in a 11-coordinate geometry to three equivalent La, four equivalent Ni, and four Al atoms. There are two shorter (2.64 Å) and two longer (2.73 Å) Al–Al bond lengths. In the second Al site, Al is bonded in a 11-coordinate geometry to four equivalent La, four equivalent Ni, and one Al atom.
DOI: 10.17188/1724702
title: Materials Data on Li2MnVP2(O4F)2 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: 10.17188/1724703
title: Materials Data on CrN2 by Materials Project

description: CrN2 is Keatite-like structured and crystallizes in the monoclinic P2/m space group. The structure is three-dimensional. there are seven inequivalent Cr6+ sites. In the first Cr6+ site, Cr6+ is bonded to four N3- atoms to form corner-sharing CrN4 tetrahedra. There is two shorter (1.72 Å) and two longer (1.73 Å) Cr–N bond length. In the second Cr6+ site, Cr6+ is bonded to four N3- atoms to form corner-sharing CrN4 tetrahedra. There is two shorter (1.72 Å) and two longer (1.73 Å) Cr–N bond length. In the third Cr6+ site, Cr6+ is bonded to four N3- atoms to form corner-sharing CrN4 tetrahedra. There are a spread of Cr–N bond distances ranging from 1.72–1.74 Å. In the fourth Cr6+ site, Cr6+ is bonded to four N3- atoms to form corner-sharing CrN4 tetrahedra. There are a spread of Cr–N bond distances ranging from 1.72–1.74 Å. In the fifth Cr6+ site, Cr6+ is bonded to four N3- atoms to form corner-sharing CrN4 tetrahedra. There are a spread of Cr–N bond distances ranging from 1.72–1.74 Å. In the sixth Cr6+ site, Cr6+ is bonded to four N3- atoms to form corner-sharing CrN4 tetrahedra. There is two shorter (1.72 Å) and two longer (1.73 Å) Cr–N bond length. In the seventh Cr6+ site, Cr6+ is bonded to four N3- atoms to form corner-sharing CrN4 tetrahedra. There is two shorter (1.72 Å) and two longer (1.73 Å) Cr–N bond length. There are eighteen inequivalent N3- sites. In the first N3- site, N3- is bonded in a bent 150 degrees geometry to two equivalent Cr6+ atoms. In the second N3- site, N3- is bonded in a bent 150 degrees geometry to two equivalent Cr6+ atoms. In the third N3- site, N3- is bonded in a linear geometry to two equivalent Cr6+ atoms. In the fourth N3- site, N3- is bonded in a bent 150 degrees geometry to two equivalent Cr6+ atoms. In the fifth N3- site, N3- is bonded in a linear geometry to two equivalent Cr6+ atoms. In the sixth N3- site, N3- is bonded in a linear geometry to two equivalent Cr6+ atoms. In the seventh N3- site, N3- is bonded in a linear geometry to two equivalent Cr6+ atoms. In the eighth N3- site, N3- is bonded in a bent 150 degrees geometry to two Cr6+ atoms. In the ninth N3- site, N3- is bonded in a bent 150 degrees geometry to two Cr6+ atoms. In the tenth N3- site, N3- is bonded in a bent 150 degrees geometry to two Cr6+ atoms. In the eleventh N3- site, N3- is bonded in a linear geometry to two Cr6+ atoms. In the twelfth N3- site, N3- is bonded in a linear geometry to two Cr6+ atoms. In the thirteenth N3- site, N3- is bonded in a bent 150 degrees geometry to two Cr6+ atoms. In the fourteenth N3- site, N3- is bonded in a bent 150 degrees geometry to two Cr6+ atoms. In the fifteenth N3- site, N3- is bonded in a bent 150 degrees geometry to two equivalent Cr6+ atoms. In the sixteenth N3- site, N3- is bonded in a bent 150 degrees geometry to two Cr6+ atoms. In the seventeenth N3- site, N3- is bonded in a bent 150 degrees geometry to two Cr6+ atoms. In the eighteenth N3- site, N3- is bonded in a bent 150 degrees geometry to two Cr6+ atoms.
DOI: 10.17188/1724704
title: Materials Data on Li2VPO4F 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: 10.17188/1724705
title: Materials Data on TiH by Materials Project

description: TiH is Halite, Rock Salt structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ti is bonded to six equivalent H atoms to form a mixture of edge and corner-sharing TiH6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Ti–H bond lengths are 2.09 Å. H is bonded to six equivalent Ti atoms to form a mixture of edge and corner-sharing HTi6 octahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1724706
title: Materials Data on Mn3TeO8 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: 10.17188/1724707
title: Materials Data on In(GaAu)2 by Materials Project

description: Au2InGa2 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Au is bonded in a 8-coordinate geometry to three equivalent In and four equivalent Ga atoms. All Au–In bond lengths are 2.90 Å. There are one shorter (2.66 Å) and three longer (2.68 Å) Au–Ga bond lengths. In is bonded in a 6-coordinate geometry to six equivalent Au atoms. Ga is bonded to four equivalent Au atoms to form a mixture of edge and corner-sharing GaAu4 tetrahedra.
DOI: 10.17188/1724708
title: Materials Data on Be4CuSi by Materials Project

description: Be4CuSi is Hexagonal Laves-derived structured and crystallizes in the cubic F-43m space group. The structure is three-dimensional. Be is bonded to six equivalent Be, three equivalent Cu, and three equivalent Si atoms to form a mixture of corner, edge, and face-sharing BeBe6Cu3Si3 cuboctahedra. All Be–Be bond lengths are 2.16 Å. All Be–Cu bond lengths are 2.54 Å. All Be–Si bond lengths are 2.54 Å. Cu is bonded in a 12-coordinate geometry to twelve equivalent Be and four equivalent Si atoms. All Cu–Si bond lengths are 2.65 Å. Si is bonded in a 12-coordinate geometry to twelve equivalent Be and four equivalent Cu atoms.
DOI: 10.17188/1724709
title: Materials Data on Lu4NiB13 by Materials Project

description: Lu4NiB13 crystallizes in the tetragonal P4/mnc space group. The structure is three-dimensional. Lu3+ is bonded in a 6-coordinate geometry to fifteen B+1.15- atoms. There are a spread of Lu–B bond distances ranging from 2.51–2.87 Å. Ni3+ is bonded in a 8-coordinate geometry to eight equivalent B+1.15- atoms. All Ni–B bond lengths are 2.15 Å. There are three inequivalent B+1.15- sites. In the first B+1.15- site, B+1.15- is bonded in a cuboctahedral geometry to four equivalent Lu3+ and eight equivalent B+1.15- atoms. All B–B bond lengths are 2.08 Å. In the second B+1.15- site, B+1.15- is bonded in a 3-coordinate geometry to six equivalent Lu3+ and three B+1.15- atoms. There is two shorter (1.76 Å) and one longer (1.86 Å) B–B bond length. In the third B+1.15- site, B+1.15- is bonded in a 9-coordinate geometry to four equivalent Lu3+, one Ni3+, and four B+1.15- atoms. Both B–B bond lengths are 1.80 Å.
DOI: 10.5281/zenodo.4489991
title: LA INVESTIGACIÓN CIENTÍFICA SOBRE LA GUACAMAYA VERDE (Ara militaris Linnaeus, 1766) Y LA COTORRA SERRANA (Rhynchopsitta pachyrhyncha Swainson‎, ‎1827): ANÁLISIS BIBLIOMÉTRICO = THE SCIENTIFIC RESEARCH ON MILITARY MACAW (Ara militaris Linnaeus, 1766) AND THICK-BILLED PARROT (Rhynchopsitta pachyrhyncha Swainson, 1827): BIBLIOMETRIC ANALYSIS

description: Research data from an article with the abstract: Thick-billed Parrot (<em>Rhynchopsitta pachyrhyncha</em>) and Military Macaw (<em>Ara militaris</em>) are two species of endangered parrots due to habitats destruction and land-use change. Review the actual scientific research and its trends helps to assess whether the efforts made contribute to efficient conservation. The goal of this work is to obtain an overview of the scientific research on these birds, as well as to identify the most studied topics and those ones necessary to be research. 82 records related to this matter were obtained from Scopus and Web of Science databases, which were published from 1967 to 2019. Unidimensional and bidimensional bibliometric indicators were realyzed. The least inquired topics correspond to pathologies, controlled studies, animal experimentation and molecular biology. Important topics were proposed for research and conservation of this species.
DOI: 10.5281/zenodo.4489990
title: LA INVESTIGACIÓN CIENTÍFICA SOBRE LA GUACAMAYA VERDE (Ara militaris Linnaeus, 1766) Y LA COTORRA SERRANA (Rhynchopsitta pachyrhyncha Swainson‎, ‎1827): ANÁLISIS BIBLIOMÉTRICO = THE SCIENTIFIC RESEARCH ON MILITARY MACAW (Ara militaris Linnaeus, 1766) AND THICK-BILLED PARROT (Rhynchopsitta pachyrhyncha Swainson, 1827): BIBLIOMETRIC ANALYSIS

description: Research data from an article with the abstract: Thick-billed Parrot (<em>Rhynchopsitta pachyrhyncha</em>) and Military Macaw (<em>Ara militaris</em>) are two species of endangered parrots due to habitats destruction and land-use change. Review the actual scientific research and its trends helps to assess whether the efforts made contribute to efficient conservation. The goal of this work is to obtain an overview of the scientific research on these birds, as well as to identify the most studied topics and those ones necessary to be research. 82 records related to this matter were obtained from Scopus and Web of Science databases, which were published from 1967 to 2019. Unidimensional and bidimensional bibliometric indicators were realyzed. The least inquired topics correspond to pathologies, controlled studies, animal experimentation and molecular biology. Important topics were proposed for research and conservation of this species.