cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1664113
title: Materials Data on MnV2O10 by Materials Project

description: V2MnO10 crystallizes in the monoclinic Cc space group. The structure is three-dimensional. there are two inequivalent V sites. In the first V site, V is bonded in a 5-coordinate geometry to five O atoms. There are a spread of V–O bond distances ranging from 1.68–2.03 Å. In the second V site, V is bonded in a 5-coordinate geometry to five O atoms. There are a spread of V–O bond distances ranging from 1.68–2.03 Å. Mn is bonded in a distorted octahedral geometry to six O atoms. There are a spread of Mn–O bond distances ranging from 2.03–2.70 Å. There are ten inequivalent O sites. In the first O site, O is bonded in a distorted bent 120 degrees geometry to one V and one Mn atom. In the second O site, O is bonded in a single-bond geometry to one O atom. The O–O bond length is 1.24 Å. In the third O site, O is bonded in a distorted bent 150 degrees geometry to one V and one Mn atom. In the fourth O site, O is bonded in a bent 120 degrees geometry to one Mn and one O atom. The O–O bond length is 1.23 Å. In the fifth O site, O is bonded in a bent 150 degrees geometry to one V and one Mn atom. In the sixth O site, O is bonded in a trigonal non-coplanar geometry to three V atoms. In the seventh O site, O is bonded in a single-bond geometry to one O atom. In the eighth O site, O is bonded in a bent 120 degrees geometry to one Mn and one O atom. In the ninth O site, O is bonded in a trigonal non-coplanar geometry to three V atoms. In the tenth O site, O is bonded in a bent 150 degrees geometry to one V and one Mn atom.
DOI: 10.17188/1664114
title: Materials Data on LiNd2Rh by Materials Project

description: LiNd2Rh is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Li is bonded in a body-centered cubic geometry to eight equivalent Nd atoms. All Li–Nd bond lengths are 3.14 Å. Nd is bonded in a distorted body-centered cubic geometry to four equivalent Li and four equivalent Rh atoms. All Nd–Rh bond lengths are 3.14 Å. Rh is bonded in a body-centered cubic geometry to eight equivalent Nd atoms.
DOI: 10.17188/1664115
title: Materials Data on Li3BH6 by Materials Project

description: Li6BH4BH4(H2)2 crystallizes in the triclinic P1 space group. The structure is three-dimensional and consists of two hydrogen molecules, one BH4 cluster, and one Li6BH4 framework. In the BH4 cluster, B3- is bonded in a tetrahedral geometry to four H atoms. All B–H bond lengths are 1.23 Å. There are four inequivalent H sites. In the first H site, H is bonded in a single-bond geometry to one B3- atom. In the second H site, H is bonded in a single-bond geometry to one B3- atom. In the third H site, H is bonded in a single-bond geometry to one B3- atom. In the fourth H site, H is bonded in a single-bond geometry to one B3- atom. In the Li6BH4 framework, there are six inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a distorted water-like geometry to two H atoms. There is one shorter (1.85 Å) and one longer (1.88 Å) Li–H bond length. In the second Li1+ site, Li1+ is bonded in a 3-coordinate geometry to one B3- and two H atoms. The Li–B bond length is 2.27 Å. There is one shorter (1.81 Å) and one longer (1.97 Å) Li–H bond length. In the third Li1+ site, Li1+ is bonded in a single-bond geometry to one H atom. The Li–H bond length is 1.89 Å. In the fourth Li1+ site, Li1+ is bonded in a 2-coordinate geometry to two H atoms. There is one shorter (1.91 Å) and one longer (1.94 Å) Li–H bond length. In the fifth Li1+ site, Li1+ is bonded in a water-like geometry to two H atoms. There is one shorter (1.83 Å) and one longer (1.84 Å) Li–H bond length. In the sixth Li1+ site, Li1+ is bonded in a distorted bent 120 degrees geometry to two H atoms. There is one shorter (1.86 Å) and one longer (1.91 Å) Li–H bond length. B3- is bonded in a 2-coordinate geometry to one Li1+ and two H atoms. There is one shorter (1.25 Å) and one longer (1.28 Å) B–H bond length. There are four inequivalent H sites. In the first H site, H is bonded in a distorted T-shaped geometry to three Li1+ atoms. In the second H site, H is bonded in a distorted trigonal non-coplanar geometry to two Li1+ and one B3- atom. In the third H site, H is bonded in a distorted T-shaped geometry to two Li1+ and one B3- atom. In the fourth H site, H is bonded in a 4-coordinate geometry to four Li1+ atoms.
DOI: 10.17188/1664116
title: Materials Data on LaGa3Pd by Materials Project

description: LaPdGa3 crystallizes in the tetragonal I-4m2 space group. The structure is three-dimensional. La is bonded in a 12-coordinate geometry to four equivalent Pd and twelve Ga atoms. All La–Pd bond lengths are 3.44 Å. There are eight shorter (3.32 Å) and four longer (3.44 Å) La–Ga bond lengths. Pd is bonded to four equivalent La and eight Ga atoms to form distorted PdLa4Ga8 cuboctahedra that share corners with four equivalent GaLa4Ga4Pd4 cuboctahedra, corners with twelve equivalent PdLa4Ga8 cuboctahedra, edges with two equivalent GaLa4Ga4Pd4 cuboctahedra, faces with four equivalent PdLa4Ga8 cuboctahedra, and faces with four equivalent GaLa4Ga4Pd4 cuboctahedra. There are four shorter (2.58 Å) and four longer (3.07 Å) Pd–Ga bond lengths. There are two inequivalent Ga sites. In the first Ga site, Ga is bonded in a 2-coordinate geometry to four equivalent La, two equivalent Pd, and three Ga atoms. There are one shorter (2.54 Å) and two longer (2.58 Å) Ga–Ga bond lengths. In the second Ga site, Ga is bonded to four equivalent La, four equivalent Pd, and four equivalent Ga atoms to form GaLa4Ga4Pd4 cuboctahedra that share corners with four equivalent PdLa4Ga8 cuboctahedra, corners with twelve equivalent GaLa4Ga4Pd4 cuboctahedra, edges with two equivalent PdLa4Ga8 cuboctahedra, faces with four equivalent PdLa4Ga8 cuboctahedra, and faces with four equivalent GaLa4Ga4Pd4 cuboctahedra.
DOI: 10.17188/1664117
title: Materials Data on CsSm(MoO4)2 by Materials Project

description: CsSm(MoO4)2 crystallizes in the orthorhombic Pccm space group. The structure is three-dimensional. Cs1+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are four shorter (3.15 Å) and four longer (3.37 Å) Cs–O bond lengths. Sm3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are four shorter (2.37 Å) and four longer (2.54 Å) Sm–O bond lengths. Mo6+ is bonded in a tetrahedral geometry to four O2- atoms. There are a spread of Mo–O bond distances ranging from 1.75–1.87 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal planar geometry to two equivalent Sm3+ and one Mo6+ atom. In the second O2- site, O2- is bonded in a 2-coordinate geometry to one Cs1+, one Sm3+, and one Mo6+ atom. In the third O2- site, O2- is bonded in a distorted single-bond geometry to two equivalent Cs1+ and one Mo6+ atom.
DOI: 10.17188/1664118
title: Materials Data on PtRh2(NCl)10 by Materials Project

description: (RhCl)2Pt(N2Cl3)2(N2)2(NCl)2 crystallizes in the monoclinic C2/m space group. The structure is zero-dimensional and consists of eight ammonia molecules, four chloramine molecules, two Pt(N2Cl3)2 clusters, and four RhCl clusters. In each Pt(N2Cl3)2 cluster, Pt2+ is bonded in an octahedral geometry to six Cl1- atoms. There are four shorter (2.34 Å) and two longer (2.35 Å) Pt–Cl bond lengths. N+0.20+ is bonded in a distorted water-like geometry to one Cl1- atom. The N–Cl bond length is 2.41 Å. There are three inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a single-bond geometry to one Pt2+ atom. In the second Cl1- site, Cl1- is bonded in a single-bond geometry to one Pt2+ atom. In the third Cl1- site, Cl1- is bonded in a 1-coordinate geometry to one Pt2+ and two equivalent N+0.20+ atoms. In each RhCl cluster, Rh3+ is bonded in a 4-coordinate geometry to one Cl1- atom. The Rh–Cl bond length is 2.35 Å. Cl1- is bonded in a single-bond geometry to one Rh3+ atom.
DOI: 10.17188/1664119
title: Materials Data on Sr2NdNb(CuO4)2 by Materials Project

description: Sr2NdNbCu2O8 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Sr2+ sites. In the first Sr2+ site, Sr2+ is bonded in a 10-coordinate geometry to ten O2- atoms. There are a spread of Sr–O bond distances ranging from 2.64–2.94 Å. In the second Sr2+ site, Sr2+ is bonded in a 10-coordinate geometry to ten O2- atoms. There are a spread of Sr–O bond distances ranging from 2.68–2.91 Å. Nd3+ is bonded in a body-centered cubic geometry to eight O2- atoms. There are a spread of Nd–O bond distances ranging from 2.44–2.59 Å. Nb5+ is bonded to six O2- atoms to form NbO6 octahedra that share corners with four equivalent NbO6 octahedra and corners with two equivalent CuO5 square pyramids. The corner-sharing octahedral tilt angles are 29°. There is two shorter (1.97 Å) and four longer (2.02 Å) Nb–O bond length. Cu2+ is bonded to five O2- atoms to form CuO5 square pyramids that share a cornercorner with one NbO6 octahedra and corners with four equivalent CuO5 square pyramids. The corner-sharing octahedral tilt angles are 5°. There are four shorter (1.97 Å) and one longer (2.22 Å) Cu–O bond lengths. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two equivalent Sr2+ and two equivalent Nb5+ atoms. In the second O2- site, O2- is bonded in a 6-coordinate geometry to two Sr2+, two equivalent Nd3+, and two equivalent Cu2+ atoms. In the third O2- site, O2- is bonded in a 6-coordinate geometry to four Sr2+, one Nb5+, and one Cu2+ atom. In the fourth O2- site, O2- is bonded to two Sr2+, two equivalent Nd3+, and two equivalent Cu2+ atoms to form distorted edge-sharing OSr2Nd2Cu2 octahedra. In the fifth O2- site, O2- is bonded in a 2-coordinate geometry to two equivalent Sr2+ and two equivalent Nb5+ atoms. In the sixth O2- site, O2- is bonded in a 6-coordinate geometry to two Sr2+, two equivalent Nd3+, and two equivalent Cu2+ atoms.
DOI: 10.17188/1664121
title: Materials Data on Pr3Si by Materials Project

description: Pr3Si crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Pr is bonded in a 2-coordinate geometry to four equivalent Si atoms. There are two shorter (3.17 Å) and two longer (3.58 Å) Pr–Si bond lengths. Si is bonded to twelve equivalent Pr atoms to form a mixture of distorted corner and face-sharing SiPr12 cuboctahedra.
DOI: 10.17188/1664122
title: Materials Data on DyEr3 by Materials Project

description: Er3Dy is Magnesium-derived structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Er is bonded to eight equivalent Er and four equivalent Dy atoms to form ErDy4Er8 cuboctahedra that share corners with four equivalent DyEr12 cuboctahedra, corners with fourteen equivalent ErDy4Er8 cuboctahedra, edges with six equivalent DyEr12 cuboctahedra, edges with twelve equivalent ErDy4Er8 cuboctahedra, faces with four equivalent DyEr12 cuboctahedra, and faces with sixteen equivalent ErDy4Er8 cuboctahedra. There are a spread of Er–Er bond distances ranging from 3.49–3.60 Å. There are two shorter (3.49 Å) and two longer (3.59 Å) Er–Dy bond lengths. Dy is bonded to twelve equivalent Er atoms to form DyEr12 cuboctahedra that share corners with six equivalent DyEr12 cuboctahedra, corners with twelve equivalent ErDy4Er8 cuboctahedra, edges with eighteen equivalent ErDy4Er8 cuboctahedra, faces with eight equivalent DyEr12 cuboctahedra, and faces with twelve equivalent ErDy4Er8 cuboctahedra.
DOI: 10.17188/1664123
title: Materials Data on MgZn5 by Materials Project

description: MgZn5 is alpha Samarium-derived structured and crystallizes in the hexagonal P-6m2 space group. The structure is three-dimensional. Mg is bonded to six equivalent Mg and six equivalent Zn atoms to form MgMg6Zn6 cuboctahedra that share corners with six equivalent MgMg6Zn6 cuboctahedra, corners with twelve equivalent ZnZn12 cuboctahedra, edges with six equivalent MgMg6Zn6 cuboctahedra, edges with twelve equivalent ZnMg3Zn9 cuboctahedra, faces with six equivalent MgMg6Zn6 cuboctahedra, and faces with fourteen ZnMg3Zn9 cuboctahedra. All Mg–Mg bond lengths are 2.80 Å. All Mg–Zn bond lengths are 2.99 Å. There are three inequivalent Zn sites. In the first Zn site, Zn is bonded to three equivalent Mg and nine Zn atoms to form ZnMg3Zn9 cuboctahedra that share corners with eighteen ZnMg3Zn9 cuboctahedra, edges with six equivalent MgMg6Zn6 cuboctahedra, edges with twelve ZnMg3Zn9 cuboctahedra, faces with six equivalent MgMg6Zn6 cuboctahedra, and faces with fourteen ZnMg3Zn9 cuboctahedra. There are six shorter (2.80 Å) and three longer (2.83 Å) Zn–Zn bond lengths. In the second Zn site, Zn is bonded to twelve Zn atoms to form ZnZn12 cuboctahedra that share corners with six equivalent MgMg6Zn6 cuboctahedra, corners with twelve equivalent ZnZn12 cuboctahedra, edges with eighteen ZnMg3Zn9 cuboctahedra, a faceface with one MgMg6Zn6 cuboctahedra, and faces with nineteen ZnMg3Zn9 cuboctahedra. There are six shorter (2.80 Å) and three longer (2.85 Å) Zn–Zn bond lengths. In the third Zn site, Zn is bonded to twelve Zn atoms to form ZnZn12 cuboctahedra that share corners with eighteen ZnMg3Zn9 cuboctahedra, edges with eighteen ZnZn12 cuboctahedra, and faces with twenty ZnMg3Zn9 cuboctahedra. All Zn–Zn bond lengths are 2.80 Å.
DOI: 10.17188/1664124
title: Materials Data on K3Ga by Materials Project

description: (K)3Ga crystallizes in the tetragonal I4/mmm space group. The structure is zero-dimensional and consists of two gallium, elemental molecules and six kalium molecules.
DOI: 10.17188/1664125
title: Materials Data on Fe6O7F5 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: 10.17188/1664127
title: Materials Data on Ca3Fe2Cl2O5 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: 10.17188/1664128
title: Materials Data on Sc11Ga10 by Materials Project

description: Sc11Ga10 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. there are four inequivalent Sc sites. In the first Sc site, Sc is bonded in a 4-coordinate geometry to nine Ga atoms. There are a spread of Sc–Ga bond distances ranging from 3.06–3.44 Å. In the second Sc site, Sc is bonded in a 7-coordinate geometry to seven Ga atoms. There are a spread of Sc–Ga bond distances ranging from 2.72–3.22 Å. In the third Sc site, Sc is bonded in a 7-coordinate geometry to seven Ga atoms. There are a spread of Sc–Ga bond distances ranging from 2.74–2.98 Å. In the fourth Sc site, Sc is bonded to seven Ga atoms to form a mixture of distorted face, edge, and corner-sharing ScGa7 pentagonal bipyramids. There are a spread of Sc–Ga bond distances ranging from 2.82–3.11 Å. There are five inequivalent Ga sites. In the first Ga site, Ga is bonded in a 2-coordinate geometry to eight Sc and two Ga atoms. There are one shorter (2.60 Å) and one longer (2.96 Å) Ga–Ga bond lengths. In the second Ga site, Ga is bonded in a 9-coordinate geometry to nine Sc atoms. In the third Ga site, Ga is bonded in a 11-coordinate geometry to seven Sc and four Ga atoms. Both Ga–Ga bond lengths are 2.63 Å. In the fourth Ga site, Ga is bonded in a 8-coordinate geometry to eight Sc atoms. In the fifth Ga site, Ga is bonded in a 6-coordinate geometry to eight Sc and one Ga atom. The Ga–Ga bond length is 2.78 Å.
DOI: 10.17188/1664129
title: Materials Data on U2(Al3Ir)3 by Materials Project

description: U2(IrAl3)3 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. U is bonded in a 11-coordinate geometry to six Ir and eleven Al atoms. There are four shorter (3.43 Å) and two longer (3.46 Å) U–Ir bond lengths. There are a spread of U–Al bond distances ranging from 3.04–3.17 Å. There are two inequivalent Ir sites. In the first Ir site, Ir is bonded in a 8-coordinate geometry to four equivalent U and eight Al atoms. There are a spread of Ir–Al bond distances ranging from 2.56–2.65 Å. In the second Ir site, Ir is bonded in a 8-coordinate geometry to four equivalent U and eight Al atoms. There are a spread of Ir–Al bond distances ranging from 2.54–2.63 Å. There are four inequivalent Al sites. In the first Al site, Al is bonded in a 2-coordinate geometry to two equivalent U and two equivalent Ir atoms. In the second Al site, Al is bonded in a 3-coordinate geometry to three equivalent U and three Ir atoms. In the third Al site, Al is bonded in a 3-coordinate geometry to two equivalent U and three Ir atoms. In the fourth Al site, Al is bonded in a 2-coordinate geometry to two equivalent U and two equivalent Ir atoms.
DOI: 10.17188/1664130
title: Materials Data on Li2Fe3(P2O7)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: 10.17188/1664131
title: Materials Data on LuTaTiO6 by Materials Project

description: LuTiTaO6 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Lu3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Lu–O bond distances ranging from 2.21–2.63 Å. Ti4+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Ti–O bond distances ranging from 1.79–2.31 Å. Ta5+ is bonded to six O2- atoms to form distorted corner-sharing TaO6 octahedra. The corner-sharing octahedral tilt angles are 55°. There are a spread of Ta–O bond distances ranging from 1.87–2.21 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a 3-coordinate geometry to two equivalent Lu3+ and one Ti4+ atom. In the second O2- site, O2- is bonded in a 3-coordinate geometry to two equivalent Lu3+ and one Ta5+ atom. In the third O2- site, O2- is bonded in a 3-coordinate geometry to two equivalent Ti4+ and one Ta5+ atom. In the fourth O2- site, O2- is bonded in a distorted trigonal planar geometry to one Ti4+ and two equivalent Ta5+ atoms. In the fifth O2- site, O2- is bonded in a 3-coordinate geometry to two equivalent Lu3+, one Ti4+, and one Ta5+ atom. In the sixth O2- site, O2- is bonded in a 3-coordinate geometry to two equivalent Lu3+, one Ti4+, and one Ta5+ atom.
DOI: 10.17188/1664132
title: Materials Data on CaSnS3 by Materials Project

description: CaSnS3 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. Ca2+ is bonded to seven S2- atoms to form distorted CaS7 pentagonal bipyramids that share corners with two equivalent SnS6 octahedra, edges with four equivalent SnS6 octahedra, and edges with six equivalent CaS7 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 47°. There are a spread of Ca–S bond distances ranging from 2.85–2.90 Å. Sn4+ is bonded to six S2- atoms to form SnS6 octahedra that share corners with four equivalent SnS6 octahedra, corners with two equivalent CaS7 pentagonal bipyramids, edges with four equivalent SnS6 octahedra, and edges with four equivalent CaS7 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 8°. There are two shorter (2.41 Å) and four longer (2.84 Å) Sn–S bond lengths. There are two inequivalent S2- sites. In the first S2- site, S2- is bonded to one Ca2+ and four equivalent Sn4+ atoms to form SCaSn4 square pyramids that share corners with four equivalent SCaSn4 square pyramids, corners with six equivalent SCa3Sn tetrahedra, edges with four equivalent SCaSn4 square pyramids, and edges with four equivalent SCa3Sn tetrahedra. In the second S2- site, S2- is bonded to three equivalent Ca2+ and one Sn4+ atom to form distorted SCa3Sn tetrahedra that share corners with three equivalent SCaSn4 square pyramids, corners with ten equivalent SCa3Sn tetrahedra, edges with two equivalent SCaSn4 square pyramids, and edges with three equivalent SCa3Sn tetrahedra.
DOI: 10.17188/1664133
title: Materials Data on Ni3(AsO4)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: 10.17188/1664134
title: Materials Data on Ba(MnN2)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: 10.17188/1664135
title: Materials Data on Li3VPCO7 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: 10.15468/dl.8jpf5p
title: Occurrence Download

description: A dataset containing 391354 species occurrences available in GBIF matching the query:
{
 "TaxonKey" : [
 "is Sus scrofa Linnaeus, 1758"
 ]
}

 The dataset includes 391354 records from 3135 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0089229-240321170329656/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.6084/m9.figshare.20226827
title: Additional file 16 of Combined nature and human selections reshaped peach fruit metabolome

description: Additional file 16: Table S15. Gene co-expression modules constructed based on gene expression profiles.
DOI: 10.6084/m9.figshare.20226836.v1
title: Additional file 19 of Combined nature and human selections reshaped peach fruit metabolome

description: Additional file 19: Table S18. List of identified cis-eQTLs.
DOI: 10.6084/m9.figshare.19703729
title: Additional file 5 of Rice (Oryza sativa L.) cytochrome P450 protein 716A subfamily CYP716A16 regulates disease resistance

description: Additional file 5: Supplementary Table S4. The primers sequences used in this study.
DOI: 10.6084/m9.figshare.20226848
title: Additional file 22 of Combined nature and human selections reshaped peach fruit metabolome

description: Additional file 22: Table S21. Browning indexes (△A) of the 186 peach accessions.
DOI: 10.6084/m9.figshare.20226851.v1
title: Additional file 23 of Combined nature and human selections reshaped peach fruit metabolome

description: Additional file 23: Table S22. Correlation between metabolite contents and browning indexes.
DOI: 10.6084/m9.figshare.19703805.v1
title: Additional file 8 of Integrative analysis of circRNA, miRNA, and mRNA profiles to reveal ceRNA regulation in chicken muscle development from the embryonic to post-hatching periods

description: Additional file 8: Table S8. The miRNAs identified in our previous study.