cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1733909
title: Materials Data on Nd4Fe4Co12B3C by Materials Project

description: Nd4Fe4Co12B3C crystallizes in the hexagonal P-6m2 space group. The structure is three-dimensional. there are three inequivalent Nd sites. In the first Nd site, Nd is bonded in a 6-coordinate geometry to six Fe atoms. All Nd–Fe bond lengths are 2.95 Å. In the second Nd site, Nd is bonded in a 12-coordinate geometry to twelve equivalent Co, three equivalent B, and three equivalent C atoms. All Nd–Co bond lengths are 2.90 Å. All Nd–B bond lengths are 2.95 Å. All Nd–C bond lengths are 2.95 Å. In the third Nd site, Nd is bonded in a 12-coordinate geometry to twelve equivalent Co and six B atoms. All Nd–Co bond lengths are 2.93 Å. All Nd–B bond lengths are 2.95 Å. There are two inequivalent Fe sites. In the first Fe site, Fe is bonded in a 12-coordinate geometry to three equivalent Nd and six Co atoms. There are three shorter (2.44 Å) and three longer (2.48 Å) Fe–Co bond lengths. In the second Fe site, Fe is bonded in a 12-coordinate geometry to three equivalent Nd and six Co atoms. There are three shorter (2.46 Å) and three longer (2.48 Å) Fe–Co bond lengths. There are two inequivalent Co sites. In the first Co site, Co is bonded in a 2-coordinate geometry to two equivalent Nd, two Fe, one B, and one C atom. The Co–B bond length is 2.03 Å. The Co–C bond length is 1.99 Å. In the second Co site, Co is bonded in a 2-coordinate geometry to two equivalent Nd, two Fe, and two B atoms. Both Co–B bond lengths are 2.05 Å. There are three inequivalent B sites. In the first B site, B is bonded in a 6-coordinate geometry to three equivalent Nd and six equivalent Co atoms. In the second B site, B is bonded in a 6-coordinate geometry to three equivalent Nd and six equivalent Co atoms. In the third B site, B is bonded in a 6-coordinate geometry to three equivalent Nd and six equivalent Co atoms. C is bonded in a 6-coordinate geometry to three equivalent Nd and six equivalent Co atoms.
DOI: 10.17188/1733910
title: Materials Data on Ba2MgTl by Materials Project

description: Ba2MgTl is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ba is bonded in a body-centered cubic geometry to four equivalent Mg and four equivalent Tl atoms. All Ba–Mg bond lengths are 3.74 Å. All Ba–Tl bond lengths are 3.74 Å. Mg is bonded in a body-centered cubic geometry to eight equivalent Ba atoms. Tl is bonded in a body-centered cubic geometry to eight equivalent Ba atoms.
DOI: 10.17188/1733911
title: Materials Data on Fe2O2F5 by Materials Project

description: Fe2O2F5 crystallizes in the orthorhombic Imma space group. The structure is three-dimensional. there are two inequivalent Fe sites. In the first Fe site, Fe is bonded to two equivalent O and four equivalent F atoms to form corner-sharing FeO2F4 octahedra. The corner-sharing octahedral tilt angles are 42°. Both Fe–O bond lengths are 2.36 Å. All Fe–F bond lengths are 2.00 Å. In the second Fe site, Fe is bonded to six F atoms to form corner-sharing FeF6 octahedra. The corner-sharing octahedra tilt angles range from 36–42°. There is four shorter (1.96 Å) and two longer (2.01 Å) Fe–F bond length. O is bonded in a bent 120 degrees geometry to one Fe and one O atom. The O–O bond length is 1.25 Å. There are two inequivalent F sites. In the first F site, F is bonded in a bent 150 degrees geometry to two Fe atoms. In the second F site, F is bonded in a bent 150 degrees geometry to two equivalent Fe atoms.
DOI: 10.17188/1733912
title: Materials Data on Cu3PO7 by Materials Project

description: Cu3PO7 crystallizes in the orthorhombic Pbca space group. The structure is three-dimensional. there are three inequivalent Cu3+ sites. In the first Cu3+ site, Cu3+ is bonded in a distorted rectangular see-saw-like geometry to four O2- atoms. There are a spread of Cu–O bond distances ranging from 1.81–1.89 Å. In the second Cu3+ site, Cu3+ is bonded in a square co-planar geometry to four O2- atoms. There are a spread of Cu–O bond distances ranging from 1.86–1.89 Å. In the third Cu3+ site, Cu3+ is bonded to five O2- atoms to form CuO5 square pyramids that share corners with three equivalent PO4 tetrahedra and an edgeedge with one CuO5 square pyramid. There are a spread of Cu–O bond distances ranging from 1.82–2.23 Å. P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with three equivalent CuO5 square pyramids. There are a spread of P–O bond distances ranging from 1.54–1.58 Å. There are seven inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Cu3+ and one P5+ atom. In the second O2- site, O2- is bonded in a trigonal non-coplanar geometry to three Cu3+ atoms. In the third O2- site, O2- is bonded in a 3-coordinate geometry to two equivalent Cu3+ and one P5+ atom. In the fourth O2- site, O2- is bonded in a distorted trigonal planar geometry to three Cu3+ atoms. In the fifth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Cu3+ and one P5+ atom. In the sixth O2- site, O2- is bonded in a bent 120 degrees geometry to two Cu3+ atoms. In the seventh O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Cu3+ and one P5+ atom.
DOI: 10.17188/1733913
title: Materials Data on Tb5Si4 by Materials Project

description: Tb5Si4 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. there are three inequivalent Tb+3.20+ sites. In the first Tb+3.20+ site, Tb+3.20+ is bonded to six Si4- atoms to form a mixture of distorted edge, face, and corner-sharing TbSi6 pentagonal pyramids. The corner-sharing octahedra tilt angles range from 39–40°. There are a spread of Tb–Si bond distances ranging from 2.87–3.04 Å. In the second Tb+3.20+ site, Tb+3.20+ is bonded in a 7-coordinate geometry to seven Si4- atoms. There are a spread of Tb–Si bond distances ranging from 3.05–3.69 Å. In the third Tb+3.20+ site, Tb+3.20+ is bonded to six Si4- atoms to form a mixture of face and corner-sharing TbSi6 octahedra. The corner-sharing octahedral tilt angles are 56°. There are a spread of Tb–Si bond distances ranging from 2.92–3.31 Å. There are three inequivalent Si4- sites. In the first Si4- site, Si4- is bonded in a 9-coordinate geometry to eight Tb+3.20+ and one Si4- atom. The Si–Si bond length is 2.52 Å. In the second Si4- site, Si4- is bonded in a 9-coordinate geometry to eight Tb+3.20+ and one Si4- atom. The Si–Si bond length is 2.52 Å. In the third Si4- site, Si4- is bonded in a 9-coordinate geometry to eight Tb+3.20+ and one Si4- atom.
DOI: 10.17188/1733914
title: Materials Data on Li2Cr3O6 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: 10.17188/1733915
title: Materials Data on CsU2(PO4)4 by Materials Project

description: CsU2(PO4)4 crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. Cs1+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Cs–O bond distances ranging from 3.08–3.54 Å. U+5.50+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of U–O bond distances ranging from 2.04–2.68 Å. There are two inequivalent P5+ sites. In the first P5+ site, P5+ is bonded in a tetrahedral geometry to four O2- atoms. There are a spread of P–O bond distances ranging from 1.54–1.57 Å. In the second P5+ site, P5+ is bonded in a tetrahedral geometry to four O2- atoms. There are a spread of P–O bond distances ranging from 1.49–1.66 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one U+5.50+ and one P5+ atom. In the second O2- site, O2- is bonded in a distorted single-bond geometry to two equivalent U+5.50+ and one P5+ atom. In the third O2- site, O2- is bonded in a distorted single-bond geometry to two equivalent U+5.50+ and one P5+ atom. In the fourth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one U+5.50+ and one P5+ atom. In the fifth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one U+5.50+ and one P5+ atom. In the sixth O2- site, O2- is bonded in a distorted single-bond geometry to two equivalent Cs1+ and one P5+ atom. In the seventh O2- site, O2- is bonded in a single-bond geometry to two equivalent Cs1+ and one P5+ atom. In the eighth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one U+5.50+ and one P5+ atom.
DOI: 10.17188/1733916
title: Materials Data on CsEr10(C2I9)2 by Materials Project

description: CsEr10(C2I9)2 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. Cs1+ is bonded to twelve I1- atoms to form CsI12 cuboctahedra that share corners with six ErCI5 octahedra and faces with two equivalent ErCI5 octahedra. The corner-sharing octahedra tilt angles range from 41–46°. There are a spread of Cs–I bond distances ranging from 4.07–4.49 Å. There are five inequivalent Er3+ sites. In the first Er3+ site, Er3+ is bonded to one C+3.25- and five I1- atoms to form distorted ErCI5 octahedra that share a cornercorner with one CsI12 cuboctahedra, edges with two ErCI5 octahedra, and a faceface with one CsI12 cuboctahedra. The Er–C bond length is 2.18 Å. There are a spread of Er–I bond distances ranging from 3.03–3.41 Å. In the second Er3+ site, Er3+ is bonded in a 7-coordinate geometry to two C+3.25- and five I1- atoms. There are one shorter (2.46 Å) and one longer (2.47 Å) Er–C bond lengths. There are a spread of Er–I bond distances ranging from 2.92–3.65 Å. In the third Er3+ site, Er3+ is bonded in a 8-coordinate geometry to four C+3.25- and four I1- atoms. There are a spread of Er–C bond distances ranging from 2.60–2.63 Å. There are a spread of Er–I bond distances ranging from 3.12–3.26 Å. In the fourth Er3+ site, Er3+ is bonded to one C+3.25- and five I1- atoms to form distorted ErCI5 octahedra that share corners with two equivalent CsI12 cuboctahedra and edges with two ErCI5 octahedra. The Er–C bond length is 2.19 Å. There are a spread of Er–I bond distances ranging from 3.00–3.40 Å. In the fifth Er3+ site, Er3+ is bonded in a 6-coordinate geometry to two C+3.25- and four I1- atoms. Both Er–C bond lengths are 2.44 Å. There are a spread of Er–I bond distances ranging from 2.91–3.20 Å. There are two inequivalent C+3.25- sites. In the first C+3.25- site, C+3.25- is bonded in a 6-coordinate geometry to five Er3+ and one C+3.25- atom. The C–C bond length is 1.44 Å. In the second C+3.25- site, C+3.25- is bonded in a 6-coordinate geometry to five Er3+ and one C+3.25- atom. There are nine inequivalent I1- sites. In the first I1- site, I1- is bonded in a 3-coordinate geometry to three Er3+ atoms. In the second I1- site, I1- is bonded in a 4-coordinate geometry to one Cs1+ and three Er3+ atoms. In the third I1- site, I1- is bonded in a 2-coordinate geometry to two Er3+ atoms. In the fourth I1- site, I1- is bonded in a 4-coordinate geometry to one Cs1+ and three Er3+ atoms. In the fifth I1- site, I1- is bonded in a 3-coordinate geometry to one Cs1+ and two Er3+ atoms. In the sixth I1- site, I1- is bonded in a 4-coordinate geometry to one Cs1+ and three Er3+ atoms. In the seventh I1- site, I1- is bonded in a 4-coordinate geometry to one Cs1+ and two Er3+ atoms. In the eighth I1- site, I1- is bonded in a 1-coordinate geometry to one Cs1+ and two Er3+ atoms. In the ninth I1- site, I1- is bonded in a distorted T-shaped geometry to three Er3+ atoms.
DOI: 10.17188/1733917
title: Materials Data on LiMg2 by Materials Project

description: LiMg2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. Li is bonded to three equivalent Li and nine Mg atoms to form distorted LiLi3Mg9 cuboctahedra that share corners with six equivalent LiLi3Mg9 cuboctahedra, corners with twelve MgLi5Mg7 cuboctahedra, edges with four equivalent LiLi3Mg9 cuboctahedra, edges with fourteen MgLi5Mg7 cuboctahedra, faces with six equivalent LiLi3Mg9 cuboctahedra, and faces with fourteen MgLi5Mg7 cuboctahedra. There are one shorter (3.11 Å) and two longer (3.20 Å) Li–Li bond lengths. There are a spread of Li–Mg bond distances ranging from 3.08–3.12 Å. There are two inequivalent Mg sites. In the first Mg site, Mg is bonded to five equivalent Li and seven Mg atoms to form distorted MgLi5Mg7 cuboctahedra that share corners with six equivalent LiLi3Mg9 cuboctahedra, corners with twelve MgLi5Mg7 cuboctahedra, edges with five equivalent LiLi3Mg9 cuboctahedra, edges with thirteen MgLi5Mg7 cuboctahedra, faces with eight equivalent LiLi3Mg9 cuboctahedra, and faces with twelve MgLi5Mg7 cuboctahedra. There are a spread of Mg–Mg bond distances ranging from 3.11–3.20 Å. In the second Mg site, Mg is bonded to four equivalent Li and eight Mg atoms to form distorted MgLi4Mg8 cuboctahedra that share corners with six equivalent LiLi3Mg9 cuboctahedra, corners with twelve MgLi5Mg7 cuboctahedra, edges with nine equivalent LiLi3Mg9 cuboctahedra, edges with nine MgLi5Mg7 cuboctahedra, faces with six equivalent LiLi3Mg9 cuboctahedra, and faces with fourteen MgLi5Mg7 cuboctahedra. There are a spread of Mg–Mg bond distances ranging from 3.06–3.20 Å.
DOI: 10.17188/1733918
title: Materials Data on Rb2NdCuCl6 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: 10.17188/1733919
title: Materials Data on Co3BiO8 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: 10.17188/1733920
title: Materials Data on Tb2NiGe4 by Materials Project

description: Tb2NiGe4 crystallizes in the orthorhombic Amm2 space group. The structure is three-dimensional. there are two inequivalent Tb sites. In the first Tb site, Tb is bonded in a 10-coordinate geometry to ten Ge atoms. There are a spread of Tb–Ge bond distances ranging from 3.02–3.23 Å. In the second Tb site, Tb is bonded in a 4-coordinate geometry to four equivalent Ni and ten Ge atoms. All Tb–Ni bond lengths are 3.19 Å. There are a spread of Tb–Ge bond distances ranging from 3.05–3.26 Å. Ni is bonded in a 9-coordinate geometry to four equivalent Tb and five Ge atoms. There are a spread of Ni–Ge bond distances ranging from 2.32–2.38 Å. There are four inequivalent Ge sites. In the first Ge site, Ge is bonded in a 9-coordinate geometry to six Tb, one Ni, and two equivalent Ge atoms. Both Ge–Ge bond lengths are 2.57 Å. In the second Ge site, Ge is bonded in a 8-coordinate geometry to six Tb and two equivalent Ge atoms. In the third Ge site, Ge is bonded in a 4-coordinate geometry to four Tb, two equivalent Ni, and four equivalent Ge atoms. All Ge–Ge bond lengths are 2.89 Å. In the fourth Ge site, Ge is bonded in a 4-coordinate geometry to four Tb, two equivalent Ni, and four equivalent Ge atoms.
DOI: 10.17188/1733921
title: Materials Data on DyNi3Sn2 by Materials Project

description: DyNi3Sn2 crystallizes in the hexagonal P6/mmm space group. The structure is three-dimensional. there are two inequivalent Dy sites. In the first Dy site, Dy is bonded in a hexagonal planar geometry to six equivalent Ni atoms. All Dy–Ni bond lengths are 3.01 Å. In the second Dy site, Dy is bonded in a 12-coordinate geometry to twelve Ni and six equivalent Sn atoms. There are six shorter (3.21 Å) and six longer (3.42 Å) Dy–Ni bond lengths. All Dy–Sn bond lengths are 3.22 Å. There are two inequivalent Ni sites. In the first Ni site, Ni is bonded in a 9-coordinate geometry to three Dy, two equivalent Ni, and four equivalent Sn atoms. Both Ni–Ni bond lengths are 2.62 Å. All Ni–Sn bond lengths are 2.58 Å. In the second Ni site, Ni is bonded to four equivalent Dy, four equivalent Ni, and four equivalent Sn atoms to form a mixture of face and corner-sharing NiDy4Ni4Sn4 cuboctahedra. All Ni–Sn bond lengths are 2.65 Å. Sn is bonded in a 12-coordinate geometry to two equivalent Dy and six Ni atoms.
DOI: 10.17188/1733923
title: Materials Data on LiNdO2 by Materials Project

description: LiNdO2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Li1+ is bonded to four O2- atoms to form distorted LiO4 trigonal pyramids that share corners with five equivalent NdO7 pentagonal bipyramids, corners with four equivalent LiO4 trigonal pyramids, edges with three equivalent NdO7 pentagonal bipyramids, and a faceface with one NdO7 pentagonal bipyramid. There are a spread of Li–O bond distances ranging from 1.92–2.14 Å. Nd3+ is bonded to seven O2- atoms to form distorted NdO7 pentagonal bipyramids that share corners with four equivalent NdO7 pentagonal bipyramids, corners with five equivalent LiO4 trigonal pyramids, edges with seven equivalent NdO7 pentagonal bipyramids, edges with three equivalent LiO4 trigonal pyramids, and a faceface with one LiO4 trigonal pyramid. There are a spread of Nd–O bond distances ranging from 2.39–2.54 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded to two equivalent Li1+ and four equivalent Nd3+ atoms to form a mixture of distorted edge, face, and corner-sharing OLi2Nd4 octahedra. The corner-sharing octahedra tilt angles range from 58–60°. In the second O2- site, O2- is bonded in a 2-coordinate geometry to two equivalent Li1+ and three equivalent Nd3+ atoms.
DOI: 10.17188/1733924
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: 10.17188/1733925
title: Materials Data on Cs2KAlI6 by Materials Project

description: Cs2KAlI6 is (Cubic) Perovskite-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Cs1+ is bonded to twelve equivalent I1- atoms to form CsI12 cuboctahedra that share corners with twelve equivalent CsI12 cuboctahedra, faces with six equivalent CsI12 cuboctahedra, faces with four equivalent KI6 octahedra, and faces with four equivalent AlI6 octahedra. All Cs–I bond lengths are 4.39 Å. K1+ is bonded to six equivalent I1- atoms to form KI6 octahedra that share corners with six equivalent AlI6 octahedra and faces with eight equivalent CsI12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All K–I bond lengths are 3.41 Å. Al3+ is bonded to six equivalent I1- atoms to form AlI6 octahedra that share corners with six equivalent KI6 octahedra and faces with eight equivalent CsI12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Al–I bond lengths are 2.78 Å. I1- is bonded in a distorted linear geometry to four equivalent Cs1+, one K1+, and one Al3+ atom.
DOI: 10.17188/1733926
title: Materials Data on CuH2(NCl2)2 by Materials Project

description: CuCl2N2(HCl)2 is Protactinium-derived structured and crystallizes in the tetragonal P4_2/mnm space group. The structure is zero-dimensional and consists of four ammonia molecules, two copper chloride molecules, and two HCl clusters. In each HCl cluster, H1+ is bonded in a bent 120 degrees geometry to two equivalent Cl1- atoms. Both H–Cl bond lengths are 1.59 Å. Cl1- is bonded in a 6-coordinate geometry to two equivalent H1+ atoms.
DOI: 10.17188/1733927
title: Materials Data on Mg(ClO4)2 by Materials Project

description: Mg(ClO4)2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Mg is bonded to six O atoms to form MgO6 octahedra that share corners with six equivalent ClO4 tetrahedra. There are a spread of Mg–O bond distances ranging from 2.10–2.13 Å. There are four inequivalent O sites. In the first O site, O is bonded in a bent 150 degrees geometry to one Mg and one Cl atom. The O–Cl bond length is 1.46 Å. In the second O site, O is bonded in a bent 150 degrees geometry to one Mg and one Cl atom. The O–Cl bond length is 1.46 Å. In the third O site, O is bonded in a bent 150 degrees geometry to one Mg and one Cl atom. The O–Cl bond length is 1.48 Å. In the fourth O site, O is bonded in a single-bond geometry to one Cl atom. The O–Cl bond length is 1.42 Å. Cl is bonded to four O atoms to form ClO4 tetrahedra that share corners with three equivalent MgO6 octahedra. The corner-sharing octahedra tilt angles range from 37–44°.
DOI: 10.5281/zenodo.4495033
title: Entwicklung eines taktilen Mikrotaster-Messsystems für Hochgeschwindigkeitsmessung von Form, Rauheit und mechanischen Eigenschaften (Data)

description: Raw data, scripts and figures used for the article "Entwicklung eines taktilen Mikrotaster-Messsystems für Hochgeschwindigkeitsmessung von Form, Rauheit und mechanischen Eigenschaften", published in the proceedings of 20. GMA/ITG-Fachtagung Sensoren und Messsysteme 2019; 2019-06-25 - 2019-06-26; Nürnberg, Germany. The data/scripts can be opened/executed by the software "Matlab"
description: This project has received funding from the EMPIR program co-financed by the Participating States and from the European Union's Horizon 2020 research and innovation program under no. 17IND05 MicroProbes.
DOI: 10.17188/1733928
title: Materials Data on K2NbTlF6 by Materials Project

description: K2NbTlF6 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. K1+ is bonded to twelve equivalent F1- atoms to form KF12 cuboctahedra that share corners with twelve equivalent KF12 cuboctahedra, faces with six equivalent KF12 cuboctahedra, faces with four equivalent NbF6 octahedra, and faces with four equivalent TlF6 octahedra. All K–F bond lengths are 3.36 Å. Nb3+ is bonded to six equivalent F1- atoms to form NbF6 octahedra that share corners with six equivalent TlF6 octahedra and faces with eight equivalent KF12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Nb–F bond lengths are 2.10 Å. Tl1+ is bonded to six equivalent F1- atoms to form TlF6 octahedra that share corners with six equivalent NbF6 octahedra and faces with eight equivalent KF12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Tl–F bond lengths are 2.64 Å. F1- is bonded in a distorted linear geometry to four equivalent K1+, one Nb3+, and one Tl1+ atom.
DOI: 10.5281/zenodo.4495032
title: Entwicklung eines taktilen Mikrotaster-Messsystems für Hochgeschwindigkeitsmessung von Form, Rauheit und mechanischen Eigenschaften (Data)

description: Raw data, scripts and figures used for the article "Entwicklung eines taktilen Mikrotaster-Messsystems für Hochgeschwindigkeitsmessung von Form, Rauheit und mechanischen Eigenschaften", published in the proceedings of 20. GMA/ITG-Fachtagung Sensoren und Messsysteme 2019; 2019-06-25 - 2019-06-26; Nürnberg, Germany. The data/scripts can be opened/executed by the software "Matlab"
description: This project has received funding from the EMPIR program co-financed by the Participating States and from the European Union's Horizon 2020 research and innovation program under no. 17IND05 MicroProbes.
DOI: 10.17188/1733930
title: Materials Data on Li5Mn3O5F3 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