cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1750588
title: Materials Data on TePb2S by Materials Project

description: PbTePbS is Caswellsilverite structured and crystallizes in the trigonal R-3m space group. The structure is three-dimensional. Pb2+ is bonded to three equivalent Te2- and three equivalent S2- atoms to form a mixture of edge and corner-sharing PbTe3S3 octahedra. The corner-sharing octahedral tilt angles are 0°. All Pb–Te bond lengths are 3.25 Å. All Pb–S bond lengths are 3.04 Å. Te2- is bonded to six equivalent Pb2+ atoms to form TePb6 octahedra that share corners with six equivalent SPb6 octahedra, edges with six equivalent TePb6 octahedra, and edges with six equivalent SPb6 octahedra. The corner-sharing octahedral tilt angles are 5°. S2- is bonded to six equivalent Pb2+ atoms to form SPb6 octahedra that share corners with six equivalent TePb6 octahedra, edges with six equivalent TePb6 octahedra, and edges with six equivalent SPb6 octahedra. The corner-sharing octahedral tilt angles are 5°.
DOI: 10.17188/1750589
title: Materials Data on Li2Cr4P4O15 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: 10.17188/1750590
title: Materials Data on SiH8(CBr)4 by Materials Project

description: SiH8(CBr)4 is Silicon tetrafluoride-derived structured and crystallizes in the tetragonal P-42_1c space group. The structure is zero-dimensional and consists of two tetrakis(bromomethyl)silane molecules. Si4+ is bonded in a tetrahedral geometry to four equivalent C2- atoms. All Si–C bond lengths are 1.89 Å. C2- is bonded to one Si4+, two H1+, and one Br1- atom to form distorted corner-sharing CSiH2Br tetrahedra. There is one shorter (1.09 Å) and one longer (1.10 Å) C–H bond length. The C–Br bond length is 1.97 Å. There are two inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a single-bond geometry to one C2- atom. In the second H1+ site, H1+ is bonded in a single-bond geometry to one C2- atom. Br1- is bonded in a single-bond geometry to one C2- atom.
DOI: 10.17188/1750591
title: Materials Data on NdGe5 by Materials Project

description: NdGe5 crystallizes in the orthorhombic Immm space group. The structure is three-dimensional. Nd is bonded in a 10-coordinate geometry to fourteen Ge atoms. There are a spread of Nd–Ge bond distances ranging from 3.13–3.53 Å. There are two inequivalent Ge sites. In the first Ge site, Ge is bonded in a 8-coordinate geometry to three equivalent Nd and five Ge atoms. There are a spread of Ge–Ge bond distances ranging from 2.58–2.94 Å. In the second Ge site, Ge is bonded in a 2-coordinate geometry to two equivalent Nd and eight equivalent Ge atoms.
DOI: 10.17188/1750594
title: Materials Data on In4Se3N2 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: 10.17188/1750595
title: Materials Data on Al4SiPd by Materials Project

description: PdAl4Si crystallizes in the trigonal R-3m space group. The structure is three-dimensional. Pd is bonded in a body-centered cubic geometry to eight Al atoms. There are two shorter (2.49 Å) and six longer (2.57 Å) Pd–Al bond lengths. There are two inequivalent Al sites. In the first Al site, Al is bonded to three equivalent Pd and one Si atom to form a mixture of distorted edge and corner-sharing AlSiPd3 tetrahedra. The Al–Si bond length is 2.68 Å. In the second Al site, Al is bonded to one Pd and three equivalent Si atoms to form a mixture of distorted edge and corner-sharing AlSi3Pd tetrahedra. All Al–Si bond lengths are 2.63 Å. Si is bonded in a body-centered cubic geometry to eight Al atoms.
DOI: 10.17188/1750596
title: Materials Data on NaZnBr3O5 by Materials Project

description: NaZnO5Br3 crystallizes in the trigonal R3 space group. The structure is two-dimensional and consists of three NaZnO5Br3 sheets oriented in the (0, 0, 1) direction. Na is bonded in a 3-coordinate geometry to three equivalent O and three equivalent Br atoms. All Na–O bond lengths are 2.77 Å. All Na–Br bond lengths are 3.31 Å. Zn is bonded in a trigonal planar geometry to three equivalent Br atoms. All Zn–Br bond lengths are 2.35 Å. There are three inequivalent O sites. In the first O site, O is bonded in a bent 120 degrees geometry to one Na and one O atom. The O–O bond length is 1.39 Å. In the second O site, O is bonded in a trigonal non-coplanar geometry to three equivalent O atoms. In the third O site, O is bonded in a distorted T-shaped geometry to three equivalent Br atoms. All O–Br bond lengths are 2.46 Å. Br is bonded in a 3-coordinate geometry to one Na, one Zn, and one O atom.
DOI: 10.17188/1750598
title: Materials Data on Co3Sb4(OF)6 by Materials Project

description: Co3Sb4O6F6 crystallizes in the cubic I-43m space group. The structure is three-dimensional. Co2+ is bonded to two equivalent O2- and four equivalent F1- atoms to form corner-sharing CoO2F4 octahedra. The corner-sharing octahedral tilt angles are 0°. Both Co–O bond lengths are 2.09 Å. All Co–F bond lengths are 2.08 Å. Sb3+ is bonded in a distorted T-shaped geometry to three equivalent O2- atoms. All Sb–O bond lengths are 2.01 Å. O2- is bonded in a trigonal planar geometry to one Co2+ and two equivalent Sb3+ atoms. F1- is bonded in a linear geometry to two equivalent Co2+ atoms.
DOI: 10.17188/1750599
title: Materials Data on Li4Mn(Ni2O5)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: 10.17188/1750600
title: Materials Data on K2CdAu by Materials Project

description: K2AuCd crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two K2AuCd ribbons oriented in the (0, 1, 0) direction. K is bonded in a linear geometry to one Au and one Cd atom. The K–Au bond length is 3.09 Å. The K–Cd bond length is 3.73 Å. Au is bonded in a linear geometry to two equivalent K atoms. Cd is bonded in a linear geometry to two equivalent K atoms.
DOI: 10.17188/1750601
title: Materials Data on V6O11F 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: 10.17188/1750602
title: Materials Data on Li3V4NiO12 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: 10.17188/1750603
title: Materials Data on HfFeAs by Materials Project

description: HfFeAs crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Hf is bonded in a 5-coordinate geometry to six equivalent Fe and five equivalent As atoms. There are a spread of Hf–Fe bond distances ranging from 2.83–3.03 Å. There are two shorter (2.74 Å) and three longer (2.75 Å) Hf–As bond lengths. Fe is bonded in a 4-coordinate geometry to six equivalent Hf and four equivalent As atoms. There are a spread of Fe–As bond distances ranging from 2.38–2.46 Å. As is bonded in a 9-coordinate geometry to five equivalent Hf and four equivalent Fe atoms.
DOI: 10.17188/1750604
title: Materials Data on BaPrCuTe3 by Materials Project

description: BaPrCuTe3 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. Ba2+ is bonded in a 8-coordinate geometry to eight Te2- atoms. There are a spread of Ba–Te bond distances ranging from 3.50–4.09 Å. Pr3+ is bonded to six Te2- atoms to form PrTe6 octahedra that share corners with two equivalent PrTe6 octahedra, edges with two equivalent PrTe6 octahedra, and edges with four equivalent CuTe4 tetrahedra. The corner-sharing octahedral tilt angles are 40°. There are two shorter (3.14 Å) and four longer (3.20 Å) Pr–Te bond lengths. Cu1+ is bonded to four Te2- atoms to form CuTe4 tetrahedra that share corners with two equivalent CuTe4 tetrahedra and edges with four equivalent PrTe6 octahedra. There are two shorter (2.67 Å) and two longer (2.77 Å) Cu–Te bond lengths. There are two inequivalent Te2- sites. In the first Te2- site, Te2- is bonded in a 6-coordinate geometry to three equivalent Ba2+, two equivalent Pr3+, and one Cu1+ atom. In the second Te2- site, Te2- is bonded to two equivalent Ba2+, two equivalent Pr3+, and two equivalent Cu1+ atoms to form a mixture of distorted corner and edge-sharing TeBa2Pr2Cu2 octahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1750605
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: 10.17188/1750606
title: Materials Data on Li6CoNiP2(CO7)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: 10.17188/1750607
title: Materials Data on Bi by Materials Project

description: Bi crystallizes in the orthorhombic Cmce space group. The structure is three-dimensional. there are two inequivalent Bi sites. In the first Bi site, Bi is bonded in a 10-coordinate geometry to ten Bi atoms. There are a spread of Bi–Bi bond distances ranging from 3.40–3.66 Å. In the second Bi site, Bi is bonded in a 5-coordinate geometry to eleven Bi atoms. There are a spread of Bi–Bi bond distances ranging from 3.24–3.63 Å.
DOI: 10.17188/1750608
title: Materials Data on Fe10O9F11 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: 10.17188/1750609
title: Materials Data on Li4Nb3Fe3(SnO8)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: 10.26188/13708744.v1
title: SupplementaryTable14_S5_NumberOfReadsMappingToPlasmodiumGenes

description: Total number of reads mapping to each Plasmodium gene for each sample.
DOI: 10.26188/13708744
title: SupplementaryTable14_S5_NumberOfReadsMappingToPlasmodiumGenes

description: Total number of reads mapping to each Plasmodium gene for each sample.
DOI: 10.17188/1750611
title: Materials Data on Mo5O14 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: 10.17188/1750612
title: Materials Data on Na(GaAu2)2 by Materials Project

description: Na(Au2Ga)2 is beta Plutonium-derived structured and crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Na is bonded in a 1-coordinate geometry to eleven Au and five Ga atoms. There are a spread of Na–Au bond distances ranging from 3.03–3.58 Å. There are a spread of Na–Ga bond distances ranging from 3.24–3.52 Å. There are four inequivalent Au sites. In the first Au site, Au is bonded in a 4-coordinate geometry to three equivalent Na, three Au, and three Ga atoms. There are a spread of Au–Au bond distances ranging from 2.84–3.05 Å. There are a spread of Au–Ga bond distances ranging from 2.61–2.72 Å. In the second Au site, Au is bonded in a 12-coordinate geometry to three equivalent Na, five Au, and four Ga atoms. There are a spread of Au–Au bond distances ranging from 2.96–3.04 Å. There are a spread of Au–Ga bond distances ranging from 2.67–2.86 Å. In the third Au site, Au is bonded in a 12-coordinate geometry to three equivalent Na, three Au, and three Ga atoms. There are one shorter (2.82 Å) and one longer (2.83 Å) Au–Au bond lengths. There are a spread of Au–Ga bond distances ranging from 2.69–3.18 Å. In the fourth Au site, Au is bonded in a 11-coordinate geometry to two equivalent Na, five Au, and four Ga atoms. There are a spread of Au–Ga bond distances ranging from 2.62–2.87 Å. There are two inequivalent Ga sites. In the first Ga site, Ga is bonded in a 9-coordinate geometry to two equivalent Na and seven Au atoms. In the second Ga site, Ga is bonded in a 11-coordinate geometry to three equivalent Na and seven Au atoms.
DOI: 10.17188/1750613
title: Materials Data on Sr2B5HO10 by Materials Project

description: Sr2B5O9(OH) crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are two inequivalent Sr2+ sites. In the first Sr2+ site, Sr2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Sr–O bond distances ranging from 2.53–2.91 Å. In the second Sr2+ site, Sr2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Sr–O bond distances ranging from 2.56–3.01 Å. There are five inequivalent B3+ sites. In the first B3+ site, B3+ is bonded to four O2- atoms to form corner-sharing BO4 tetrahedra. There are a spread of B–O bond distances ranging from 1.45–1.53 Å. In the second B3+ site, B3+ is bonded to four O2- atoms to form corner-sharing BO4 tetrahedra. There are a spread of B–O bond distances ranging from 1.45–1.57 Å. In the third B3+ site, B3+ is bonded in a trigonal planar geometry to three O2- atoms. There are a spread of B–O bond distances ranging from 1.36–1.40 Å. In the fourth B3+ site, B3+ is bonded in a trigonal planar geometry to three O2- atoms. There are a spread of B–O bond distances ranging from 1.34–1.42 Å. In the fifth B3+ site, B3+ is bonded to four O2- atoms to form corner-sharing BO4 tetrahedra. There are a spread of B–O bond distances ranging from 1.46–1.54 Å. H1+ is bonded in a single-bond geometry to one O2- atom. The H–O bond length is 0.97 Å. There are ten inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted bent 120 degrees geometry to two Sr2+ and two B3+ atoms. In the second O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Sr2+ and two B3+ atoms. In the third O2- site, O2- is bonded in a 2-coordinate geometry to two Sr2+, one B3+, and one H1+ atom. In the fourth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Sr2+ and two B3+ atoms. In the fifth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Sr2+ and two B3+ atoms. In the sixth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to two Sr2+ and two B3+ atoms. In the seventh O2- site, O2- is bonded in a distorted single-bond geometry to three Sr2+ and one B3+ atom. In the eighth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to two equivalent Sr2+ and two B3+ atoms. In the ninth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to two Sr2+ and two B3+ atoms. In the tenth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to two equivalent Sr2+ and two B3+ atoms.
DOI: 10.17188/1750615
title: Materials Data on Rb2Ba(Ge4O9)2 by Materials Project

description: Rb2Ba(Ge4O9)2 crystallizes in the trigonal P-3c1 space group. The structure is three-dimensional. Rb1+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Rb–O bond distances ranging from 2.77–2.97 Å. Ba2+ is bonded in a 10-coordinate geometry to ten O2- atoms. There are a spread of Ba–O bond distances ranging from 2.81–3.16 Å. There are seven inequivalent Ge4+ sites. In the first Ge4+ site, Ge4+ is bonded to six equivalent O2- atoms to form corner-sharing GeO6 octahedra. All Ge–O bond lengths are 1.94 Å. In the second Ge4+ site, Ge4+ is bonded to four O2- atoms to form GeO4 tetrahedra that share corners with two GeO6 octahedra and corners with two GeO4 tetrahedra. The corner-sharing octahedra tilt angles range from 48–52°. There are a spread of Ge–O bond distances ranging from 1.75–1.81 Å. In the third Ge4+ site, Ge4+ is bonded to six O2- atoms to form corner-sharing GeO6 octahedra. There is three shorter (1.91 Å) and three longer (1.92 Å) Ge–O bond length. In the fourth Ge4+ site, Ge4+ is bonded to four O2- atoms to form GeO4 tetrahedra that share corners with two GeO6 octahedra and corners with two GeO4 tetrahedra. The corner-sharing octahedra tilt angles range from 48–62°. There are a spread of Ge–O bond distances ranging from 1.76–1.80 Å. In the fifth Ge4+ site, Ge4+ is bonded to six O2- atoms to form corner-sharing GeO6 octahedra. There is three shorter (1.89 Å) and three longer (1.92 Å) Ge–O bond length. In the sixth Ge4+ site, Ge4+ is bonded to six equivalent O2- atoms to form corner-sharing GeO6 octahedra. All Ge–O bond lengths are 1.94 Å. In the seventh Ge4+ site, Ge4+ is bonded to four O2- atoms to form GeO4 tetrahedra that share corners with two GeO6 octahedra and corners with two GeO4 tetrahedra. The corner-sharing octahedra tilt angles range from 56–61°. There are a spread of Ge–O bond distances ranging from 1.77–1.84 Å. There are nine inequivalent O2- sites. In the first O2- site, O2- is bonded in a 2-coordinate geometry to one Rb1+ and two Ge4+ atoms. In the second O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Ba2+ and two Ge4+ atoms. In the third O2- site, O2- is bonded in a 3-coordinate geometry to one Ba2+ and two Ge4+ atoms. In the fourth O2- site, O2- is bonded in a distorted trigonal planar geometry to one Rb1+ and two Ge4+ atoms. In the fifth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Ba2+ and two Ge4+ atoms. In the sixth O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Rb1+ and two Ge4+ atoms. In the seventh O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Ba2+ and two Ge4+ atoms. In the eighth O2- site, O2- is bonded in a 2-coordinate geometry to two equivalent Rb1+ and two Ge4+ atoms. In the ninth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Rb1+, one Ba2+, and two Ge4+ atoms.
DOI: 10.17188/1750616
title: Materials Data on Al2FeRh 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: 10.17188/1750617
title: Materials Data on YbU2S3O2 by Materials Project

description: U2YbS3O2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. U+3.50+ is bonded in a 4-coordinate geometry to four equivalent S2- and four equivalent O2- atoms. All U–S bond lengths are 2.89 Å. All U–O bond lengths are 2.33 Å. Yb3+ is bonded to six S2- atoms to form a mixture of edge and corner-sharing YbS6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are four shorter (2.68 Å) and two longer (2.78 Å) Yb–S bond lengths. There are two inequivalent S2- sites. In the first S2- site, S2- is bonded in a 1-coordinate geometry to four equivalent U+3.50+ and one Yb3+ atom. In the second S2- site, S2- is bonded in a square co-planar geometry to four equivalent Yb3+ atoms. O2- is bonded to four equivalent U+3.50+ atoms to form a mixture of edge and corner-sharing OU4 tetrahedra.
DOI: 10.17188/1750618
title: Materials Data on CaMn3Cu3RuO12 by Materials Project

description: CaMn3RuCu3O12 crystallizes in the trigonal R-3 space group. The structure is three-dimensional. Ca2+ is bonded to twelve O2- atoms to form CaO12 cuboctahedra that share faces with two equivalent RuO6 octahedra and faces with six equivalent MnO6 octahedra. There are six shorter (2.60 Å) and six longer (2.63 Å) Ca–O bond lengths. Mn+3.67+ is bonded to six O2- atoms to form MnO6 octahedra that share corners with two equivalent RuO6 octahedra, corners with four equivalent MnO6 octahedra, and faces with two equivalent CaO12 cuboctahedra. The corner-sharing octahedral tilt angles are 43°. There is two shorter (1.97 Å) and four longer (2.02 Å) Mn–O bond length. Ru5+ is bonded to six equivalent O2- atoms to form RuO6 octahedra that share corners with six equivalent MnO6 octahedra and faces with two equivalent CaO12 cuboctahedra. The corner-sharing octahedral tilt angles are 43°. All Ru–O bond lengths are 1.97 Å. Cu2+ is bonded in a square co-planar geometry to four O2- atoms. There is two shorter (1.91 Å) and two longer (1.92 Å) Cu–O bond length. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to one Ca2+, one Mn+3.67+, one Ru5+, and one Cu2+ atom. In the second O2- site, O2- is bonded in a 3-coordinate geometry to one Ca2+, two equivalent Mn+3.67+, and one Cu2+ atom.
DOI: 10.17188/1750619
title: Materials Data on Mn8O13F3 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: 10.17188/1750620
title: Materials Data on YbPmCu2 by Materials Project

description: YbPmCu2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Yb is bonded in a body-centered cubic geometry to eight equivalent Cu atoms. All Yb–Cu bond lengths are 3.03 Å. Pm is bonded in a body-centered cubic geometry to eight equivalent Cu atoms. All Pm–Cu bond lengths are 3.03 Å. Cu is bonded in a body-centered cubic geometry to four equivalent Yb and four equivalent Pm atoms.
DOI: 10.17188/1750622
title: Materials Data on Ho3(CoGe2)2 by Materials Project

description: Ho3(CoGe2)2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Ho sites. In the first Ho site, Ho is bonded in a 12-coordinate geometry to four equivalent Co and eight Ge atoms. There are a spread of Ho–Co bond distances ranging from 2.86–3.20 Å. There are a spread of Ho–Ge bond distances ranging from 2.95–3.24 Å. In the second Ho site, Ho is bonded in a 6-coordinate geometry to eight Ge atoms. There are a spread of Ho–Ge bond distances ranging from 2.96–3.32 Å. Co is bonded in a 4-coordinate geometry to four equivalent Ho and four Ge atoms. There are a spread of Co–Ge bond distances ranging from 2.34–2.43 Å. There are two inequivalent Ge sites. In the first Ge site, Ge is bonded in a 10-coordinate geometry to six Ho, three equivalent Co, and one Ge atom. The Ge–Ge bond length is 2.96 Å. In the second Ge site, Ge is bonded in a 6-coordinate geometry to six Ho, one Co, and two equivalent Ge atoms. Both Ge–Ge bond lengths are 2.71 Å.