cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1195977
title: Materials Data on FeB by Materials Project

description: FeB crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Fe3+ is bonded in a 7-coordinate geometry to seven equivalent B3- atoms. There are five shorter (2.14 Å) and two longer (2.15 Å) Fe–B bond lengths. B3- is bonded in a 9-coordinate geometry to seven equivalent Fe3+ and two equivalent B3- atoms. Both B–B bond lengths are 1.79 Å.
DOI: 10.17188/1195978
title: Materials Data on SmInRh by Materials Project

description: SmRhIn crystallizes in the hexagonal P-62m space group. The structure is three-dimensional. Sm is bonded in a 11-coordinate geometry to five Rh and six equivalent In atoms. There are four shorter (3.05 Å) and one longer (3.11 Å) Sm–Rh bond lengths. There are two shorter (3.26 Å) and four longer (3.38 Å) Sm–In bond lengths. There are two inequivalent Rh sites. In the first Rh site, Rh is bonded in a 9-coordinate geometry to six equivalent Sm and three equivalent In atoms. All Rh–In bond lengths are 2.88 Å. In the second Rh site, Rh is bonded in a 9-coordinate geometry to three equivalent Sm and six equivalent In atoms. All Rh–In bond lengths are 2.78 Å. In is bonded in a 4-coordinate geometry to six equivalent Sm and four Rh atoms.
DOI: 10.17188/1195979
title: Materials Data on Rb2P3 by Materials Project

description: Rb2P3 crystallizes in the orthorhombic Fmmm space group. The structure is three-dimensional. there are two inequivalent Rb1+ sites. In the first Rb1+ site, Rb1+ is bonded in a 8-coordinate geometry to eight P+0.67- atoms. There are four shorter (3.62 Å) and four longer (3.68 Å) Rb–P bond lengths. In the second Rb1+ site, Rb1+ is bonded in a 10-coordinate geometry to ten P+0.67- atoms. There are a spread of Rb–P bond distances ranging from 3.47–3.62 Å. There are two inequivalent P+0.67- sites. In the first P+0.67- site, P+0.67- is bonded in a 2-coordinate geometry to six Rb1+ and two equivalent P+0.67- atoms. Both P–P bond lengths are 2.17 Å. In the second P+0.67- site, P+0.67- is bonded in a 8-coordinate geometry to six Rb1+ and two P+0.67- atoms. The P–P bond length is 2.17 Å.
DOI: 10.17188/1195980
title: Materials Data on InPS4 by Materials Project

description: InPS4 crystallizes in the tetragonal I-4 space group. The structure is three-dimensional. In3+ is bonded to four equivalent S2- atoms to form InS4 tetrahedra that share corners with four equivalent PS4 tetrahedra. All In–S bond lengths are 2.53 Å. P5+ is bonded to four equivalent S2- atoms to form PS4 tetrahedra that share corners with four equivalent InS4 tetrahedra. All P–S bond lengths are 2.06 Å. S2- is bonded in a water-like geometry to one In3+ and one P5+ atom.
DOI: 10.17188/1195981
title: Materials Data on MnVAs by Materials Project

description: VMnAs is Matlockite structured and crystallizes in the tetragonal P4/nmm space group. The structure is three-dimensional. V is bonded to four equivalent V, four equivalent Mn, and four equivalent As atoms to form distorted VMn4V4As4 cuboctahedra that share corners with four equivalent VMn4V4As4 cuboctahedra, corners with four equivalent MnV4As5 square pyramids, edges with eight equivalent MnV4As5 square pyramids, faces with eight equivalent VMn4V4As4 cuboctahedra, and faces with four equivalent MnV4As5 square pyramids. All V–V bond lengths are 2.59 Å. All V–Mn bond lengths are 2.86 Å. All V–As bond lengths are 2.57 Å. Mn is bonded to four equivalent V and five equivalent As atoms to form distorted MnV4As5 square pyramids that share corners with four equivalent VMn4V4As4 cuboctahedra, corners with four equivalent MnV4As5 square pyramids, edges with eight equivalent VMn4V4As4 cuboctahedra, edges with eight equivalent MnV4As5 square pyramids, faces with four equivalent VMn4V4As4 cuboctahedra, and faces with four equivalent MnV4As5 square pyramids. There are one shorter (2.48 Å) and four longer (2.62 Å) Mn–As bond lengths. As is bonded in a 9-coordinate geometry to four equivalent V and five equivalent Mn atoms.
DOI: 10.17188/1195982
title: Materials Data on Ca2InPd2 by Materials Project

description: Ca2Pd2In crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. Ca is bonded in a 7-coordinate geometry to six equivalent Pd and four equivalent In atoms. There are a spread of Ca–Pd bond distances ranging from 3.08–3.26 Å. There are a spread of Ca–In bond distances ranging from 3.43–3.50 Å. Pd is bonded in a 9-coordinate geometry to six equivalent Ca, one Pd, and two equivalent In atoms. The Pd–Pd bond length is 2.72 Å. There are one shorter (2.73 Å) and one longer (2.75 Å) Pd–In bond lengths. In is bonded in a 12-coordinate geometry to eight equivalent Ca and four equivalent Pd atoms.
DOI: 10.17188/1195983
title: Materials Data on Ga2FeS4 by Materials Project

description: FeGa2S4 crystallizes in the trigonal P-3m1 space group. The structure is two-dimensional and consists of one FeGa2S4 sheet oriented in the (0, 0, 1) direction. Fe2+ is bonded to six equivalent S2- atoms to form FeS6 octahedra that share corners with six equivalent GaS4 tetrahedra and edges with six equivalent FeS6 octahedra. All Fe–S bond lengths are 2.48 Å. Ga3+ is bonded to four S2- atoms to form GaS4 tetrahedra that share corners with three equivalent FeS6 octahedra and corners with six equivalent GaS4 tetrahedra. The corner-sharing octahedral tilt angles are 58°. There are one shorter (2.22 Å) and three longer (2.35 Å) Ga–S bond lengths. There are two inequivalent S2- sites. In the first S2- site, S2- is bonded to three equivalent Fe2+ and one Ga3+ atom to form a mixture of distorted edge and corner-sharing SGaFe3 trigonal pyramids. In the second S2- site, S2- is bonded in a trigonal non-coplanar geometry to three equivalent Ga3+ atoms.
DOI: 10.17188/1195984
title: Materials Data on InPt3C by Materials Project

description: Pt3InC is (Cubic) Perovskite structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Pt2- is bonded in a distorted linear geometry to four equivalent In2+ and two equivalent C4+ atoms. All Pt–In bond lengths are 3.01 Å. Both Pt–C bond lengths are 2.13 Å. In2+ is bonded to twelve equivalent Pt2- atoms to form InPt12 cuboctahedra that share corners with twelve equivalent InPt12 cuboctahedra, faces with six equivalent InPt12 cuboctahedra, and faces with eight equivalent CPt6 octahedra. C4+ is bonded to six equivalent Pt2- atoms to form CPt6 octahedra that share corners with six equivalent CPt6 octahedra and faces with eight equivalent InPt12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1195985
title: Materials Data on Yb(NdS2)2 by Materials Project

description: Yb(NdS2)2 crystallizes in the orthorhombic C222_1 space group. The structure is three-dimensional. Yb2+ is bonded in a distorted rectangular see-saw-like geometry to four S2- atoms. There are two shorter (2.68 Å) and two longer (2.75 Å) Yb–S bond lengths. Nd3+ is bonded to five S2- atoms to form edge-sharing NdS5 square pyramids. There are a spread of Nd–S bond distances ranging from 2.71–2.95 Å. There are two inequivalent S2- sites. In the first S2- site, S2- is bonded in a rectangular see-saw-like geometry to one Yb2+ and three equivalent Nd3+ atoms. In the second S2- site, S2- is bonded in a distorted T-shaped geometry to one Yb2+ and two equivalent Nd3+ atoms.
DOI: 10.17188/1196003
title: Materials Data on Er2ReC2 by Materials Project

description: Er2ReC2 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. there are two inequivalent Er sites. In the first Er site, Er is bonded in a distorted rectangular see-saw-like geometry to four C atoms. There are a spread of Er–C bond distances ranging from 2.50–2.64 Å. In the second Er site, Er is bonded to five C atoms to form a mixture of edge and corner-sharing ErC5 square pyramids. There are a spread of Er–C bond distances ranging from 2.48–2.55 Å. Re is bonded in a distorted trigonal planar geometry to three C atoms. There are a spread of Re–C bond distances ranging from 1.93–2.04 Å. There are two inequivalent C sites. In the first C site, C is bonded to five Er and one Re atom to form a mixture of edge and corner-sharing CEr5Re octahedra. The corner-sharing octahedra tilt angles range from 2–37°. In the second C site, C is bonded to four Er and two equivalent Re atoms to form a mixture of edge and corner-sharing CEr4Re2 octahedra. The corner-sharing octahedra tilt angles range from 11–37°.
DOI: 10.17188/1196004
title: Materials Data on GeIr by Materials Project

description: IrGe is Modderite structured and crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Ir is bonded to six equivalent Ge atoms to form a mixture of distorted face, edge, and corner-sharing IrGe6 octahedra. The corner-sharing octahedra tilt angles range from 46–56°. There are a spread of Ir–Ge bond distances ranging from 2.51–2.62 Å. Ge is bonded in a 6-coordinate geometry to six equivalent Ir atoms.
DOI: 10.17188/1196005
title: Materials Data on SrBe13 by Materials Project

description: SrBe13 crystallizes in the cubic Fm-3c space group. The structure is three-dimensional. Sr is bonded in a 1-coordinate geometry to twenty-four equivalent Be atoms. All Sr–Be bond lengths are 3.07 Å. There are two inequivalent Be sites. In the first Be site, Be is bonded to twelve equivalent Be atoms to form a mixture of corner and face-sharing BeBe12 cuboctahedra. All Be–Be bond lengths are 2.16 Å. In the second Be site, Be is bonded to two equivalent Sr and ten Be atoms to form BeSr2Be10 cuboctahedra that share corners with twenty-eight BeBe12 cuboctahedra, edges with eight equivalent BeSr2Be10 cuboctahedra, and faces with twenty-five BeBe12 cuboctahedra. There are a spread of Be–Be bond distances ranging from 2.24–2.32 Å.
DOI: 10.5281/zenodo.4477407
title: The Influence of the Extremely Low Frequency Electromagnetic Field on Clear Cell Renal Carcinoma

description: Abstract: The development of new technologies and industry is conducive to the increase in the number and variety of electromagnetic field (EMF) sources in our environment. The main sources of EMF are high-voltage lines, household appliances, audio/video devices, mobile phones, radio stations, and radar devices. In the growing use of electronic devices, scientists are increasingly interested in the effects of EMF on human health. Even though many studies on the effects of EMF have already been carried out, none of them has shown a significant effect on mammals, including humans. Moreover, it is not entirely clear how EMF influences cell behavior. The International Agency for Research on Cancer on May 31, 2011, classified PEM as a possible carcinogenic factor. This study aimed to investigate the effect of the electromagnetic field on morphological and functional changes in clear cell renal carcinoma. The research was carried out on in vitro cultures of four cell lines: HEK293, 786-O 769-P, and Caki1. The results of the research showed that the EMF of low frequency had a slight effect on the viability of cells. EMF, which induced cell arrest in the G1 phase, increased the number of early apoptotic cells and decreased the number of viable cells in the 786-O line. EMF did not affect the proliferation and viability of HEK293 cells. Extreme low-frequency EMF (ELF-EMF) also showed an inhibitory effect on the migration and metastatic properties of clear cell kidney cancer cells. Moreover, shortly after the end of ELF-EMF exposure, significant increases in ROS levels were observed in all tested cell lines. As part of the work, it was shown that low-frequency EMF shows an inhibitory effect on the proliferation of primary cancer cells, diminishing their migratory, invasive, and metastatic abilities. It also increases the apoptosis of cancer cells and the amount of reactive oxygen species. Based on the results of our research, we want to point up that the effect of ELF-EMF depends on a specific metabolic state or at a specific stage in the cell cycle of the cells under study.
description: Raw data
DOI: 10.5281/zenodo.4477406
title: The Influence of the Extremely Low Frequency Electromagnetic Field on Clear Cell Renal Carcinoma

description: Abstract: The development of new technologies and industry is conducive to the increase in the number and variety of electromagnetic field (EMF) sources in our environment. The main sources of EMF are high-voltage lines, household appliances, audio/video devices, mobile phones, radio stations, and radar devices. In the growing use of electronic devices, scientists are increasingly interested in the effects of EMF on human health. Even though many studies on the effects of EMF have already been carried out, none of them has shown a significant effect on mammals, including humans. Moreover, it is not entirely clear how EMF influences cell behavior. The International Agency for Research on Cancer on May 31, 2011, classified PEM as a possible carcinogenic factor. This study aimed to investigate the effect of the electromagnetic field on morphological and functional changes in clear cell renal carcinoma. The research was carried out on in vitro cultures of four cell lines: HEK293, 786-O 769-P, and Caki1. The results of the research showed that the EMF of low frequency had a slight effect on the viability of cells. EMF, which induced cell arrest in the G1 phase, increased the number of early apoptotic cells and decreased the number of viable cells in the 786-O line. EMF did not affect the proliferation and viability of HEK293 cells. Extreme low-frequency EMF (ELF-EMF) also showed an inhibitory effect on the migration and metastatic properties of clear cell kidney cancer cells. Moreover, shortly after the end of ELF-EMF exposure, significant increases in ROS levels were observed in all tested cell lines. As part of the work, it was shown that low-frequency EMF shows an inhibitory effect on the proliferation of primary cancer cells, diminishing their migratory, invasive, and metastatic abilities. It also increases the apoptosis of cancer cells and the amount of reactive oxygen species. Based on the results of our research, we want to point up that the effect of ELF-EMF depends on a specific metabolic state or at a specific stage in the cell cycle of the cells under study.
description: Raw data
DOI: 10.17188/1196006
title: Materials Data on ZrIn2 by Materials Project

description: ZrIn2 crystallizes in the tetragonal I4_1/amd space group. The structure is three-dimensional. Zr is bonded in a 12-coordinate geometry to ten In atoms. There are a spread of Zr–In bond distances ranging from 3.07–3.22 Å. There are two inequivalent In sites. In the first In site, In is bonded in a distorted square co-planar geometry to four equivalent Zr and four equivalent In atoms. There are two shorter (3.28 Å) and two longer (3.30 Å) In–In bond lengths. In the second In site, In is bonded to six equivalent Zr and six In atoms to form a mixture of distorted corner, edge, and face-sharing InZr6In6 cuboctahedra. Both In–In bond lengths are 3.02 Å.
DOI: 10.17188/1196007
title: Materials Data on LiIn2Pd by Materials Project

description: LiPdIn2 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 In atoms. All Li–In bond lengths are 2.88 Å. Pd is bonded in a distorted body-centered cubic geometry to eight equivalent In atoms. All Pd–In bond lengths are 2.88 Å. In is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Pd atoms.
DOI: 10.17188/1196008
title: Materials Data on Eu(POs)2 by Materials Project

description: Eu(OsP)2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Eu2+ is bonded in a 8-coordinate geometry to eight equivalent Os2- atoms. All Eu–Os bond lengths are 3.38 Å. Os2- is bonded in a 12-coordinate geometry to four equivalent Eu2+ and four equivalent P1+ atoms. All Os–P bond lengths are 2.34 Å. P1+ is bonded in a 4-coordinate geometry to four equivalent Os2- atoms.
DOI: 10.17188/1196009
title: Materials Data on USbAs by Materials Project

description: UAsSb is Matlockite structured and crystallizes in the tetragonal P4/nmm space group. The structure is three-dimensional. U6+ is bonded in a 5-coordinate geometry to four equivalent Sb3- and five equivalent As3- atoms. All U–Sb bond lengths are 3.27 Å. There are one shorter (2.86 Å) and four longer (2.96 Å) U–As bond lengths. Sb3- is bonded to four equivalent U6+ and four equivalent Sb3- atoms to form distorted SbU4Sb4 hexagonal bipyramids that share corners with four equivalent SbU4Sb4 hexagonal bipyramids, corners with twelve equivalent AsU5 square pyramids, edges with four equivalent SbU4Sb4 hexagonal bipyramids, edges with four equivalent AsU5 square pyramids, and faces with four equivalent SbU4Sb4 hexagonal bipyramids. All Sb–Sb bond lengths are 2.93 Å. As3- is bonded to five equivalent U6+ atoms to form AsU5 square pyramids that share corners with twelve equivalent SbU4Sb4 hexagonal bipyramids, corners with four equivalent AsU5 square pyramids, edges with four equivalent SbU4Sb4 hexagonal bipyramids, and edges with eight equivalent AsU5 square pyramids.
DOI: 10.17188/1196010
title: Materials Data on Rb(InAu2)2 by Materials Project

description: Rb(Au2In)2 crystallizes in the tetragonal I4/mcm space group. The structure is three-dimensional. Rb1+ is bonded in a 8-coordinate geometry to eight equivalent Au1- atoms. All Rb–Au bond lengths are 3.51 Å. Au1- is bonded in a 10-coordinate geometry to two equivalent Rb1+, four equivalent Au1-, and four equivalent In+1.50+ atoms. There are a spread of Au–Au bond distances ranging from 2.79–3.11 Å. There are a spread of Au–In bond distances ranging from 2.83–3.01 Å. In+1.50+ is bonded in a 8-coordinate geometry to eight equivalent Au1- atoms.
DOI: 10.17188/1196011
title: Materials Data on PdPbF4 by Materials Project

description: PdPbF4 crystallizes in the tetragonal I4/mcm space group. The structure is three-dimensional. Pd2+ is bonded in a square co-planar geometry to four equivalent F1- atoms. All Pd–F bond lengths are 2.02 Å. Pb2+ is bonded in a 8-coordinate geometry to eight equivalent F1- atoms. All Pb–F bond lengths are 2.58 Å. F1- is bonded in a distorted trigonal planar geometry to one Pd2+ and two equivalent Pb2+ atoms.
DOI: 10.17188/1196012
title: Materials Data on Gd(CuGe)2 by Materials Project

description: GdCu2Ge2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. Gd is bonded in a 4-coordinate geometry to eight equivalent Cu and eight equivalent Ge atoms. There are a spread of Gd–Cu bond distances ranging from 3.23–3.36 Å. There are four shorter (3.12 Å) and four longer (3.20 Å) Gd–Ge bond lengths. Cu is bonded in a 4-coordinate geometry to four equivalent Gd and four equivalent Ge atoms. There are three shorter (2.45 Å) and one longer (2.46 Å) Cu–Ge bond lengths. Ge is bonded in a 9-coordinate geometry to four equivalent Gd, four equivalent Cu, and one Ge atom. The Ge–Ge bond length is 2.49 Å.
DOI: 10.17188/1196013
title: Materials Data on Nd3PbC by Materials Project

description: Nd3PbC is (Cubic) Perovskite structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional and consists of one methane molecule and one Nd3Pb framework. In the Nd3Pb framework, Nd is bonded in a linear geometry to two equivalent Pb atoms. Both Nd–Pb bond lengths are 2.94 Å. Pb is bonded to six equivalent Nd atoms to form corner-sharing PbNd6 octahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1196014
title: Materials Data on Cr4InCuSe8 by Materials Project

description: Cr4CuInSe8 is Spinel-derived structured and crystallizes in the cubic F-43m space group. The structure is three-dimensional. Cr3+ is bonded to six Se2- atoms to form CrSe6 octahedra that share corners with three equivalent CuSe4 tetrahedra, corners with three equivalent InSe4 tetrahedra, and edges with six equivalent CrSe6 octahedra. There are three shorter (2.53 Å) and three longer (2.58 Å) Cr–Se bond lengths. Cu1+ is bonded to four equivalent Se2- atoms to form CuSe4 tetrahedra that share corners with twelve equivalent CrSe6 octahedra. The corner-sharing octahedral tilt angles are 56°. All Cu–Se bond lengths are 2.48 Å. In3+ is bonded to four equivalent Se2- atoms to form InSe4 tetrahedra that share corners with twelve equivalent CrSe6 octahedra. The corner-sharing octahedral tilt angles are 61°. All In–Se bond lengths are 2.60 Å. There are two inequivalent Se2- sites. In the first Se2- site, Se2- is bonded in a distorted rectangular see-saw-like geometry to three equivalent Cr3+ and one Cu1+ atom. In the second Se2- site, Se2- is bonded to three equivalent Cr3+ and one In3+ atom to form a mixture of distorted edge and corner-sharing SeCr3In tetrahedra.
DOI: 10.17188/1196015
title: Materials Data on TlTe by Materials Project

description: TlTe crystallizes in the tetragonal I4/mcm space group. The structure is three-dimensional. Tl1+ is bonded in a 7-coordinate geometry to three equivalent Tl1+ and seven Te1- atoms. There are one shorter (3.58 Å) and two longer (3.79 Å) Tl–Tl bond lengths. There are a spread of Tl–Te bond distances ranging from 3.49–3.72 Å. There are three inequivalent Te1- sites. In the first Te1- site, Te1- is bonded in a 10-coordinate geometry to eight equivalent Tl1+ and two equivalent Te1- atoms. Both Te–Te bond lengths are 3.16 Å. In the second Te1- site, Te1- is bonded to four equivalent Tl1+ and four Te1- atoms to form corner-sharing TeTl4Te4 hexagonal bipyramids. There are two shorter (3.02 Å) and two longer (3.16 Å) Te–Te bond lengths. In the third Te1- site, Te1- is bonded in a 9-coordinate geometry to eight equivalent Tl1+ and one Te1- atom.
DOI: 10.17188/1196016
title: Materials Data on UCoSi by Materials Project

description: UCoSi crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. U3+ is bonded to six equivalent Si4- atoms to form a mixture of corner, edge, and face-sharing USi6 octahedra. The corner-sharing octahedra tilt angles range from 45–50°. There are a spread of U–Si bond distances ranging from 2.91–2.93 Å. Co1+ is bonded in a trigonal planar geometry to three equivalent Si4- atoms. There are one shorter (2.33 Å) and two longer (2.34 Å) Co–Si bond lengths. Si4- is bonded in a 9-coordinate geometry to six equivalent U3+ and three equivalent Co1+ atoms.
DOI: 10.17188/1196017
title: Materials Data on InN by Materials Project

description: InN is Halite, Rock Salt structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. In3+ is bonded to six equivalent N3- atoms to form a mixture of corner and edge-sharing InN6 octahedra. The corner-sharing octahedral tilt angles are 0°. All In–N bond lengths are 2.35 Å. N3- is bonded to six equivalent In3+ atoms to form a mixture of corner and edge-sharing NIn6 octahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1196018
title: Materials Data on Dy(BC)2 by Materials Project

description: DyB2C2 crystallizes in the tetragonal P4_2/mmc space group. The structure is three-dimensional. Dy is bonded in a 8-coordinate geometry to eight equivalent B and eight equivalent C atoms. All Dy–B bond lengths are 2.74 Å. All Dy–C bond lengths are 2.71 Å. B is bonded in a 2-coordinate geometry to four equivalent Dy and two equivalent C atoms. Both B–C bond lengths are 1.61 Å. C is bonded in a 2-coordinate geometry to four equivalent Dy, two equivalent B, and one C atom. The C–C bond length is 1.42 Å.