cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1745462
title: Materials Data on LiEr4(HCl)4 by Materials Project

description: LiEr4(HCl)4 crystallizes in the trigonal R-3m space group. The structure is two-dimensional and consists of three LiEr4(HCl)4 sheets oriented in the (0, 0, 1) direction. Li is bonded to six equivalent Cl atoms to form edge-sharing LiCl6 octahedra. All Li–Cl bond lengths are 2.58 Å. There are two inequivalent Er sites. In the first Er site, Er is bonded in a 7-coordinate geometry to four H and three equivalent Cl atoms. There are one shorter (2.17 Å) and three longer (2.18 Å) Er–H bond lengths. All Er–Cl bond lengths are 2.86 Å. In the second Er site, Er is bonded in a 7-coordinate geometry to four H and three equivalent Cl atoms. There are three shorter (2.21 Å) and one longer (2.27 Å) Er–H bond lengths. All Er–Cl bond lengths are 2.71 Å. There are two inequivalent H sites. In the first H site, H is bonded to four Er atoms to form HEr4 tetrahedra that share corners with three equivalent ClLi3Er3 octahedra, corners with six equivalent HEr4 tetrahedra, and edges with three equivalent HEr4 tetrahedra. The corner-sharing octahedral tilt angles are 48°. In the second H site, H is bonded to four Er atoms to form HEr4 tetrahedra that share corners with three equivalent ClLi3Er3 octahedra, corners with six equivalent HEr4 tetrahedra, edges with three equivalent ClLi3Er3 octahedra, and edges with three equivalent HEr4 tetrahedra. The corner-sharing octahedral tilt angles are 29°. There are two inequivalent Cl sites. In the first Cl site, Cl is bonded in a distorted T-shaped geometry to three equivalent Er atoms. In the second Cl site, Cl is bonded to three equivalent Li and three equivalent Er atoms to form ClLi3Er3 octahedra that share corners with three equivalent ClLi3Er3 octahedra, corners with six HEr4 tetrahedra, edges with nine equivalent ClLi3Er3 octahedra, and edges with three equivalent HEr4 tetrahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1745463
title: Materials Data on KAl3(SO7)2 by Materials Project

description: KAl3(SO7)2 crystallizes in the trigonal R-3m space group. The structure is three-dimensional. K is bonded to twelve O atoms to form KO12 cuboctahedra that share corners with six equivalent SO4 tetrahedra and faces with six equivalent AlO6 octahedra. There are six shorter (2.89 Å) and six longer (2.98 Å) K–O bond lengths. Al is bonded to six O atoms to form AlO6 octahedra that share corners with four equivalent AlO6 octahedra, corners with two equivalent SO4 tetrahedra, and faces with two equivalent KO12 cuboctahedra. The corner-sharing octahedral tilt angles are 38°. There is four shorter (1.85 Å) and two longer (2.01 Å) Al–O bond length. S is bonded to four O atoms to form SO4 tetrahedra that share corners with three equivalent KO12 cuboctahedra and corners with three equivalent AlO6 octahedra. The corner-sharing octahedral tilt angles are 51°. There is one shorter (1.43 Å) and three longer (1.51 Å) S–O bond length. There are three inequivalent O sites. In the first O site, O is bonded in a single-bond geometry to one S atom. In the second O site, O is bonded in a 2-coordinate geometry to one K, one Al, and one S atom. In the third O site, O is bonded in a distorted bent 150 degrees geometry to one K and two equivalent Al atoms.
DOI: 10.17188/1745465
title: Materials Data on CrN2 by Materials Project

description: CrN2 crystallizes in the monoclinic C2 space group. The structure is three-dimensional. there are two inequivalent Cr6+ sites. In the first 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 1.72–1.75 Å. In the second 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 1.73–1.75 Å. There are five 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 bent 150 degrees geometry to two Cr6+ atoms. In the fourth N3- site, N3- is bonded in a bent 120 degrees geometry to two Cr6+ atoms. In the fifth N3- site, N3- is bonded in a bent 120 degrees geometry to two Cr6+ atoms.
DOI: 10.17188/1745466
title: Materials Data on LiFeSiO4 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: 10.17188/1745467
title: Materials Data on Li2VN2 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: 10.17188/1745468
title: Materials Data on SrMg2 by Materials Project

description: Mg2Sr crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. Sr is bonded to two equivalent Sr and ten equivalent Mg atoms to form a mixture of distorted edge and face-sharing SrSr2Mg10 cuboctahedra. Both Sr–Sr bond lengths are 3.67 Å. There are a spread of Sr–Mg bond distances ranging from 3.44–3.75 Å. Mg is bonded in a 5-coordinate geometry to five equivalent Sr atoms.
DOI: 10.17188/1745469
title: Materials Data on ScSiRu2 by Materials Project

description: ScRu2Si crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two ScRu2Si ribbons oriented in the (1, 0, 0) direction. Sc is bonded in a linear geometry to two equivalent Ru atoms. Both Sc–Ru bond lengths are 2.28 Å. Ru is bonded in a linear geometry to one Sc and one Si atom. The Ru–Si bond length is 2.21 Å. Si is bonded in a linear geometry to two equivalent Ru atoms.
DOI: 10.6073/pasta/898af1b0756d57a5e069d2cf36215cee
title: North Temperate Lakes LTER: Crayfish Abundance 1981 - current

description: Crayfish data include crayfish catch in cylindrical minnow traps baited with beef liver and occasional occurrence in other gear used to sample fish. Traps are placed at fyke net locations in nine study lakes (Allequash, Big Muskellunge, Crystal, Sparkling, Trout, Mendota, Monona, Wingra and Fish). Crayfish traps have been eliminated as gear in the Madison area lakes (Mendota, Monona, Wingra, and Fish) after 2003. Individuals are identified to species and counted. In Trout and Sparkling Lake more detailed surveys have been conducted during the summer on an ad hoc basis to track distribution and abundance of the invading species Orconectes rusticus. Additional data sets consist of pre-LTER sets (initiated in late June 1972) gathered by Capelli (Ph.D. dissertation) and Lorman (Ph.D. dissertation). Most of pre-LTER data is detailed distribution in Trout Lake, and community composition in other area lakes. Sampling Frequency: annually Number of sites: 9 Note that 2020 data does not exist due to insufficient sampling.
DOI: 10.17188/1745473
title: Materials Data on CeMg(BO2)5 by Materials Project

description: MgCe(BO2)5 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Mg2+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Mg–O bond distances ranging from 2.08–2.37 Å. Ce3+ is bonded in a 10-coordinate geometry to ten O2- atoms. There are a spread of Ce–O bond distances ranging from 2.34–2.98 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 1.47–1.50 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 1.48–1.50 Å. In the third B3+ site, B3+ is bonded in a trigonal planar geometry to three O2- atoms. All B–O bond lengths are 1.38 Å. In the fourth 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 1.46–1.52 Å. In the fifth 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 1.36–1.39 Å. There are ten inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 120 degrees geometry to one Ce3+ and two B3+ atoms. In the second O2- site, O2- is bonded in a 2-coordinate geometry to one Mg2+, one Ce3+, and two B3+ atoms. In the third O2- site, O2- is bonded in a distorted bent 120 degrees geometry to two equivalent Ce3+ and two B3+ atoms. In the fourth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Mg2+, one Ce3+, and two B3+ atoms. In the fifth O2- site, O2- is bonded in a 1-coordinate geometry to two equivalent Mg2+, one Ce3+, and one B3+ atom. In the sixth O2- site, O2- is bonded in a distorted single-bond geometry to two equivalent Ce3+ and one B3+ atom. In the seventh O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Ce3+ and two B3+ atoms. In the eighth O2- site, O2- is bonded in a 3-coordinate geometry to one Mg2+ and two B3+ atoms. In the ninth O2- site, O2- is bonded in a distorted trigonal planar geometry to one Mg2+ and two B3+ atoms. In the tenth O2- site, O2- is bonded in a bent 120 degrees geometry to one Ce3+ and two B3+ atoms.
DOI: 10.17188/1745475
title: Materials Data on Cr4B by Materials Project

description: Cr4B crystallizes in the orthorhombic F222 space group. The structure is three-dimensional. there are four inequivalent Cr sites. In the first Cr site, Cr is bonded in a distorted bent 150 degrees geometry to two equivalent B atoms. Both Cr–B bond lengths are 2.14 Å. In the second Cr site, Cr is bonded in a distorted bent 150 degrees geometry to two equivalent B atoms. Both Cr–B bond lengths are 2.18 Å. In the third Cr site, Cr is bonded in a distorted water-like geometry to two equivalent B atoms. Both Cr–B bond lengths are 2.17 Å. In the fourth Cr site, Cr is bonded in a 2-coordinate geometry to two equivalent B atoms. Both Cr–B bond lengths are 2.17 Å. B is bonded in a 8-coordinate geometry to eight Cr atoms.
DOI: 10.17188/1745476
title: Materials Data on SmSnIr by Materials Project

description: SmIrSn crystallizes in the hexagonal P-62m space group. The structure is three-dimensional. Sm is bonded in a 11-coordinate geometry to five Ir and six equivalent Sn atoms. There are one shorter (3.05 Å) and four longer (3.07 Å) Sm–Ir bond lengths. There are two shorter (3.27 Å) and four longer (3.37 Å) Sm–Sn bond lengths. There are two inequivalent Ir sites. In the first Ir site, Ir is bonded in a 9-coordinate geometry to three equivalent Sm and six equivalent Sn atoms. All Ir–Sn bond lengths are 2.80 Å. In the second Ir site, Ir is bonded in a 9-coordinate geometry to six equivalent Sm and three equivalent Sn atoms. All Ir–Sn bond lengths are 2.84 Å. Sn is bonded in a 12-coordinate geometry to six equivalent Sm and four Ir atoms.
DOI: 10.17188/1745477
title: Materials Data on Li3V3P8O29 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: 10.17188/1745478
title: Materials Data on CrNi3(PO4)4 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: 10.17188/1745479
title: Materials Data on TmCuPbS3 by Materials Project

description: TmCuPbS3 crystallizes in the orthorhombic Cmc2_1 space group. The structure is three-dimensional. Tm3+ is bonded to six S2- atoms to form TmS6 octahedra that share corners with two equivalent TmS6 octahedra, edges with two equivalent TmS6 octahedra, and edges with four equivalent CuS4 tetrahedra. The corner-sharing octahedral tilt angles are 41°. There are a spread of Tm–S bond distances ranging from 2.70–2.75 Å. Cu1+ is bonded to four S2- atoms to form CuS4 tetrahedra that share corners with two equivalent CuS4 tetrahedra and edges with four equivalent TmS6 octahedra. There are a spread of Cu–S bond distances ranging from 2.32–2.40 Å. Pb2+ is bonded in a 7-coordinate geometry to seven S2- atoms. There are a spread of Pb–S bond distances ranging from 2.96–3.31 Å. There are three inequivalent S2- sites. In the first S2- site, S2- is bonded in a 6-coordinate geometry to two equivalent Tm3+, two equivalent Cu1+, and two equivalent Pb2+ atoms. In the second S2- site, S2- is bonded in a 3-coordinate geometry to two equivalent Tm3+, one Cu1+, and three equivalent Pb2+ atoms. In the third S2- site, S2- is bonded in a 5-coordinate geometry to two equivalent Tm3+, one Cu1+, and two equivalent Pb2+ atoms.
DOI: 10.17188/1745480
title: Materials Data on LiCo2N3 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: 10.17188/1745481
title: Materials Data on RuF6 by Materials Project

description: RuF6 is beta Np structured and crystallizes in the orthorhombic Pnma space group. The structure is zero-dimensional and consists of four 13693-08-8 molecules. Ru6+ is bonded in an octahedral geometry to six F1- atoms. All Ru–F bond lengths are 1.86 Å. There are four inequivalent F1- sites. In the first F1- site, F1- is bonded in a single-bond geometry to one Ru6+ atom. In the second F1- site, F1- is bonded in a single-bond geometry to one Ru6+ atom. In the third F1- site, F1- is bonded in a single-bond geometry to one Ru6+ atom. In the fourth F1- site, F1- is bonded in a single-bond geometry to one Ru6+ atom.
DOI: 10.17188/1745482
title: Materials Data on Na2LiScF6 by Materials Project

description: Na2LiScF6 is (Cubic) Perovskite-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Na1+ is bonded to twelve equivalent F1- atoms to form NaF12 cuboctahedra that share corners with twelve equivalent NaF12 cuboctahedra, faces with six equivalent NaF12 cuboctahedra, faces with four equivalent LiF6 octahedra, and faces with four equivalent ScF6 octahedra. All Na–F bond lengths are 2.84 Å. Li1+ is bonded to six equivalent F1- atoms to form LiF6 octahedra that share corners with six equivalent ScF6 octahedra and faces with eight equivalent NaF12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Li–F bond lengths are 2.01 Å. Sc3+ is bonded to six equivalent F1- atoms to form ScF6 octahedra that share corners with six equivalent LiF6 octahedra and faces with eight equivalent NaF12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Sc–F bond lengths are 2.01 Å. F1- is bonded in a distorted linear geometry to four equivalent Na1+, one Li1+, and one Sc3+ atom.
DOI: 10.17188/1745483
title: Materials Data on Pm2MgGe by Materials Project

description: MgPm2Ge is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Mg is bonded in a body-centered cubic geometry to eight equivalent Pm atoms. All Mg–Pm bond lengths are 3.22 Å. Pm is bonded in a body-centered cubic geometry to four equivalent Mg and four equivalent Ge atoms. All Pm–Ge bond lengths are 3.22 Å. Ge is bonded in a body-centered cubic geometry to eight equivalent Pm atoms.
DOI: 10.17188/1745485
title: Materials Data on Dy5Co19P12 by Materials Project

description: Dy5Co19P12 crystallizes in the trigonal P31m space group. The structure is three-dimensional. there are two inequivalent Dy3+ sites. In the first Dy3+ site, Dy3+ is bonded to six equivalent P3- atoms to form distorted DyP6 pentagonal pyramids that share corners with twelve CoP4 tetrahedra, edges with nine CoP4 tetrahedra, and faces with two equivalent DyP6 pentagonal pyramids. All Dy–P bond lengths are 2.81 Å. In the second Dy3+ site, Dy3+ is bonded to six P3- atoms to form distorted DyP6 pentagonal pyramids that share corners with four equivalent DyP6 pentagonal pyramids, corners with twelve CoP4 tetrahedra, edges with two equivalent DyP6 pentagonal pyramids, edges with eight CoP4 tetrahedra, and faces with two equivalent DyP6 pentagonal pyramids. There are a spread of Dy–P bond distances ranging from 2.83–2.87 Å. There are five inequivalent Co+1.11+ sites. In the first Co+1.11+ site, Co+1.11+ is bonded in a 1-coordinate geometry to five P3- atoms. There are one shorter (2.20 Å) and four longer (2.58 Å) Co–P bond lengths. In the second Co+1.11+ site, Co+1.11+ is bonded to four P3- atoms to form CoP4 tetrahedra that share corners with four DyP6 pentagonal pyramids, corners with eight CoP4 tetrahedra, edges with three DyP6 pentagonal pyramids, and edges with four CoP4 tetrahedra. There are three shorter (2.25 Å) and one longer (2.34 Å) Co–P bond lengths. In the third Co+1.11+ site, Co+1.11+ is bonded to four P3- atoms to form CoP4 tetrahedra that share corners with two equivalent DyP6 pentagonal pyramids, corners with twelve CoP4 tetrahedra, edges with three DyP6 pentagonal pyramids, and edges with three CoP4 tetrahedra. There are a spread of Co–P bond distances ranging from 2.22–2.34 Å. In the fourth Co+1.11+ site, Co+1.11+ is bonded to four P3- atoms to form CoP4 tetrahedra that share corners with eight DyP6 pentagonal pyramids, corners with six CoP4 tetrahedra, edges with two equivalent DyP6 pentagonal pyramids, and edges with four equivalent CoP4 tetrahedra. There are two shorter (2.18 Å) and two longer (2.22 Å) Co–P bond lengths. In the fifth Co+1.11+ site, Co+1.11+ is bonded in a trigonal planar geometry to three equivalent P3- atoms. All Co–P bond lengths are 2.16 Å. There are three inequivalent P3- sites. In the first P3- site, P3- is bonded in a 9-coordinate geometry to four equivalent Dy3+ and five Co+1.11+ atoms. In the second P3- site, P3- is bonded in a 9-coordinate geometry to two equivalent Dy3+ and seven Co+1.11+ atoms. In the third P3- site, P3- is bonded in a 9-coordinate geometry to two equivalent Dy3+ and seven Co+1.11+ atoms.
DOI: 10.17188/1745486
title: Materials Data on KNa2LiTi2Fe2(SiO3)8 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: 10.17188/1745487
title: Materials Data on Li2MnV2(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: 10.17188/1745488
title: Materials Data on Sr3Pm by Materials Project

description: Sr3Pm is beta Cu3Ti-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Sr is bonded to eight equivalent Sr and four equivalent Pm atoms to form distorted SrSr8Pm4 cuboctahedra that share corners with four equivalent PmSr12 cuboctahedra, corners with fourteen equivalent SrSr8Pm4 cuboctahedra, edges with six equivalent PmSr12 cuboctahedra, edges with twelve equivalent SrSr8Pm4 cuboctahedra, faces with four equivalent PmSr12 cuboctahedra, and faces with sixteen equivalent SrSr8Pm4 cuboctahedra. There are a spread of Sr–Sr bond distances ranging from 3.97–4.21 Å. There are two shorter (4.00 Å) and two longer (4.09 Å) Sr–Pm bond lengths. Pm is bonded to twelve equivalent Sr atoms to form PmSr12 cuboctahedra that share corners with six equivalent PmSr12 cuboctahedra, corners with twelve equivalent SrSr8Pm4 cuboctahedra, edges with eighteen equivalent SrSr8Pm4 cuboctahedra, faces with eight equivalent PmSr12 cuboctahedra, and faces with twelve equivalent SrSr8Pm4 cuboctahedra.
DOI: 10.17188/1745489
title: Materials Data on Zr2CrTc by Materials Project

description: Zr2CrTc crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Zr2CrTc ribbons oriented in the (1, 0, 0) direction. Zr is bonded in a linear geometry to one Cr and one Tc atom. The Zr–Cr bond length is 2.97 Å. The Zr–Tc bond length is 2.25 Å. Cr is bonded in a linear geometry to two equivalent Zr atoms. Tc is bonded in a linear geometry to two equivalent Zr atoms.
DOI: 10.17188/1745490
title: Materials Data on Mn3FeO8 by Materials Project

description: Mn3FeO8 is trigonal omega-derived structured and crystallizes in the trigonal R-3m space group. The structure is two-dimensional and consists of three Mn3FeO8 sheets oriented in the (0, 0, 1) direction. Mn+4.33+ is bonded to six O2- atoms to form MnO6 octahedra that share edges with two equivalent FeO6 octahedra and edges with four equivalent MnO6 octahedra. There is four shorter (1.94 Å) and two longer (1.95 Å) Mn–O bond length. Fe3+ is bonded to six equivalent O2- atoms to form FeO6 octahedra that share edges with six equivalent MnO6 octahedra. All Fe–O bond lengths are 1.99 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three equivalent Mn+4.33+ atoms. In the second O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to two equivalent Mn+4.33+ and one Fe3+ atom.
DOI: 10.17188/1745491
title: Materials Data on BiTe by Materials Project

description: BiTe crystallizes in the orthorhombic Cmmm space group. The structure is two-dimensional and consists of two BiTe sheets oriented in the (0, 1, 0) direction. Bi2+ is bonded in a distorted square co-planar geometry to four equivalent Te2- atoms. All Bi–Te bond lengths are 3.21 Å. Te2- is bonded in a 4-coordinate geometry to four equivalent Bi2+ atoms.
DOI: 10.17188/1745492
title: Materials Data on Mn2O3F 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: 10.17188/1745494
title: Materials Data on In by Materials Project

description: In is Tungsten structured and crystallizes in the cubic Im-3m space group. The structure is three-dimensional. In is bonded in a body-centered cubic geometry to eight equivalent In atoms. All In–In bond lengths are 3.32 Å.
DOI: 10.17188/1745496
title: Materials Data on CsSbWO6 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: 10.17188/1745497
title: Materials Data on Li2ZnAg by Materials Project

description: Li2AgZn crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Li2AgZn ribbons oriented in the (1, 0, 0) direction. Li is bonded in a linear geometry to one Ag and one Zn atom. The Li–Ag bond length is 2.58 Å. The Li–Zn bond length is 2.75 Å. Ag is bonded in a linear geometry to two equivalent Li atoms. Zn is bonded in a linear geometry to two equivalent Li atoms.