cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1710570
title: Materials Data on Tm12Fe2Pb3 by Materials Project

description: Tm12Fe2Pb3 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. there are two inequivalent Tm sites. In the first Tm site, Tm is bonded in a 3-coordinate geometry to one Fe and three Pb atoms. The Tm–Fe bond length is 2.92 Å. There are a spread of Tm–Pb bond distances ranging from 3.15–3.79 Å. In the second Tm site, Tm is bonded in a 4-coordinate geometry to two equivalent Fe and two equivalent Pb atoms. Both Tm–Fe bond lengths are 2.82 Å. Both Tm–Pb bond lengths are 3.50 Å. Fe is bonded in a 9-coordinate geometry to eight Tm and one Fe atom. The Fe–Fe bond length is 2.42 Å. There are two inequivalent Pb sites. In the first Pb site, Pb is bonded to twelve Tm atoms to form a mixture of distorted corner and face-sharing PbTm12 cuboctahedra. In the second Pb site, Pb is bonded in a body-centered cubic geometry to eight equivalent Tm atoms.
DOI: 10.17188/1710571
title: Materials Data on Mg(H3Cl)2 by Materials Project

description: Mg(H2)2(HCl)2 crystallizes in the monoclinic C2/m space group. The structure is zero-dimensional and consists of four hydrochloric acid molecules, four hydrogen molecules, and two magnesium molecules.
DOI: 10.17188/1710572
title: Materials Data on LiCa2HC3 by Materials Project

description: LiCa2C3H crystallizes in the tetragonal P4/mbm space group. The structure is three-dimensional. Li1+ is bonded in a distorted linear geometry to four equivalent C2- and two equivalent H1+ atoms. All Li–C bond lengths are 2.64 Å. Both Li–H bond lengths are 1.89 Å. Ca2+ is bonded in a 6-coordinate geometry to four C2- and two equivalent H1+ atoms. There are two shorter (2.57 Å) and two longer (2.58 Å) Ca–C bond lengths. Both Ca–H bond lengths are 2.50 Å. There are two inequivalent C2- sites. In the first C2- site, C2- is bonded in a 5-coordinate geometry to two equivalent Li1+, two equivalent Ca2+, and one C2- atom. The C–C bond length is 1.33 Å. In the second C2- site, C2- is bonded to four equivalent Ca2+ and two equivalent C2- atoms to form CCa4C2 octahedra that share corners with eight equivalent HLi2Ca4 octahedra and edges with two equivalent CCa4C2 octahedra. The corner-sharing octahedral tilt angles are 80°. H1+ is bonded to two equivalent Li1+ and four equivalent Ca2+ atoms to form HLi2Ca4 octahedra that share corners with six equivalent HLi2Ca4 octahedra and corners with eight equivalent CCa4C2 octahedra. The corner-sharing octahedra tilt angles range from 0–80°.
DOI: 10.17188/1710573
title: Materials Data on TmCO4 by Materials Project

description: TmCO4 crystallizes in the orthorhombic P2_12_12_1 space group. The structure is three-dimensional. Tm is bonded in a 9-coordinate geometry to nine O atoms. There are a spread of Tm–O bond distances ranging from 2.17–2.85 Å. C is bonded in a trigonal planar geometry to three O atoms. There are a spread of C–O bond distances ranging from 1.27–1.32 Å. There are four inequivalent O sites. In the first O site, O is bonded in a bent 120 degrees geometry to two equivalent Tm atoms. In the second O site, O is bonded in a distorted single-bond geometry to two equivalent Tm and one C atom. In the third O site, O is bonded in a distorted single-bond geometry to three equivalent Tm and one C atom. In the fourth O site, O is bonded in a distorted single-bond geometry to two equivalent Tm and one C atom.
DOI: 10.17188/1710574
title: Materials Data on Pb3O by Materials Project

description: OPb3 is alpha bismuth trifluoride structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of four water molecules and one Pb framework. In the Pb framework, there are two inequivalent Pb sites. In the first Pb site, Pb is bonded in a 4-coordinate geometry to four equivalent Pb atoms. All Pb–Pb bond lengths are 3.19 Å. In the second Pb site, Pb is bonded in a body-centered cubic geometry to eight equivalent Pb atoms.
DOI: 10.17188/1710577
title: Materials Data on Ca2Co(AsO5)2 by Materials Project

description: Ca2Co(AsO5)2 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. Ca is bonded in a 6-coordinate geometry to six O atoms. There are a spread of Ca–O bond distances ranging from 2.30–2.57 Å. Co is bonded to six O atoms to form CoO6 octahedra that share corners with four equivalent AsO4 tetrahedra. There are a spread of Co–O bond distances ranging from 1.69–2.22 Å. As is bonded to four O atoms to form AsO4 tetrahedra that share corners with two equivalent CoO6 octahedra. The corner-sharing octahedra tilt angles range from 57–65°. There are a spread of As–O bond distances ranging from 1.68–1.78 Å. There are five inequivalent O sites. In the first O site, O is bonded in a 3-coordinate geometry to one Ca, one Co, and one As atom. In the second O site, O is bonded in a distorted trigonal planar geometry to one Ca, one Co, and one As atom. In the third O site, O is bonded in a distorted trigonal planar geometry to two equivalent Ca and one As atom. In the fourth O site, O is bonded in a bent 120 degrees geometry to one Ca and one As atom. In the fifth O site, O is bonded in a bent 120 degrees geometry to one Ca and one Co atom.
DOI: 10.17188/1710578
title: Materials Data on Cr2Pt2C by Materials Project

description: (PtCr)2C crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional and consists of one methane molecule and one PtCr framework. In the PtCr framework, Cr3+ is bonded in a linear geometry to two equivalent Pt2- atoms. Both Cr–Pt bond lengths are 2.40 Å. There are two inequivalent Pt2- sites. In the first Pt2- site, Pt2- is bonded to four equivalent Cr3+ and two equivalent Pt2- atoms to form distorted corner-sharing PtCr4Pt2 octahedra. The corner-sharing octahedral tilt angles are 0°. Both Pt–Pt bond lengths are 2.46 Å. In the second Pt2- site, Pt2- is bonded in a linear geometry to two equivalent Pt2- atoms.
DOI: 10.17188/1710579
title: Materials Data on Cu2SeS3 by Materials Project

description: Cu2SeS3 crystallizes in the monoclinic Cc space group. The structure is three-dimensional. there are two inequivalent Cu1+ sites. In the first Cu1+ site, Cu1+ is bonded to four S2- atoms to form corner-sharing CuS4 tetrahedra. There are a spread of Cu–S bond distances ranging from 2.25–2.35 Å. In the second Cu1+ site, Cu1+ is bonded to four S2- atoms to form corner-sharing CuS4 tetrahedra. There are a spread of Cu–S bond distances ranging from 2.31–2.36 Å. Se4+ is bonded in a trigonal non-coplanar geometry to three S2- atoms. There are a spread of Se–S bond distances ranging from 2.22–2.33 Å. There are three inequivalent S2- sites. In the first S2- site, S2- is bonded in a 3-coordinate geometry to two Cu1+ and one Se4+ atom. In the second S2- site, S2- is bonded in a 4-coordinate geometry to three Cu1+ and one Se4+ atom. In the third S2- site, S2- is bonded in a 4-coordinate geometry to three Cu1+ and one Se4+ atom.
DOI: 10.17188/1710580
title: Materials Data on Li3MnF5 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: 10.17188/1710581
title: Materials Data on Ba2Na(SnAs)6 by Materials Project

description: NaBa2(SnAs)6 crystallizes in the monoclinic C2/m space group. The structure is two-dimensional and consists of one NaBa2(SnAs)6 sheet oriented in the (0, 0, 1) direction. Na1+ is bonded to six As3- atoms to form NaAs6 octahedra that share edges with six equivalent BaAs6 octahedra. All Na–As bond lengths are 3.25 Å. Ba2+ is bonded to six As3- atoms to form BaAs6 octahedra that share edges with three equivalent NaAs6 octahedra and edges with three equivalent BaAs6 octahedra. All Ba–As bond lengths are 3.29 Å. There are two inequivalent Sn+2.17+ sites. In the first Sn+2.17+ site, Sn+2.17+ is bonded in a distorted trigonal non-coplanar geometry to three As3- atoms. There are a spread of Sn–As bond distances ranging from 2.78–2.82 Å. In the second Sn+2.17+ site, Sn+2.17+ is bonded in a distorted trigonal non-coplanar geometry to three As3- atoms. There are two shorter (2.78 Å) and one longer (2.82 Å) Sn–As bond lengths. There are two inequivalent As3- sites. In the first As3- site, As3- is bonded to one Na1+, two equivalent Ba2+, and three Sn+2.17+ atoms to form a mixture of edge and corner-sharing AsBa2NaSn3 octahedra. The corner-sharing octahedra tilt angles range from 0–1°. In the second As3- site, As3- is bonded to one Na1+, two equivalent Ba2+, and three Sn+2.17+ atoms to form a mixture of edge and corner-sharing AsBa2NaSn3 octahedra. The corner-sharing octahedra tilt angles range from 0–1°.
DOI: 10.17188/1710582
title: Materials Data on BaLi2Sn by Materials Project

description: Li2BaSn crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Li2BaSn ribbons oriented in the (1, 0, 0) direction. Li is bonded in a distorted linear geometry to one Ba and one Sn atom. The Li–Ba bond length is 3.67 Å. The Li–Sn bond length is 2.67 Å. Ba is bonded in a linear geometry to two equivalent Li atoms. Sn is bonded in a linear geometry to two equivalent Li atoms.
DOI: 10.17188/1710584
title: Materials Data on U3Ag6Mo5O27 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: 10.17188/1710585
title: Materials Data on NaAl(SO4)2 by Materials Project

description: NaAl(SO4)2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. Na1+ is bonded in a 6-coordinate geometry to six O2- atoms. There are two shorter (2.54 Å) and four longer (2.63 Å) Na–O bond lengths. Al3+ is bonded to six O2- atoms to form AlO6 octahedra that share corners with six equivalent SO4 tetrahedra. There is two shorter (1.86 Å) and four longer (1.92 Å) Al–O bond length. S6+ is bonded to four O2- atoms to form SO4 tetrahedra that share corners with three equivalent AlO6 octahedra. The corner-sharing octahedra tilt angles range from 34–44°. There are a spread of S–O bond distances ranging from 1.45–1.51 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a 1-coordinate geometry to one Na1+ and one S6+ atom. In the second O2- site, O2- is bonded in a 3-coordinate geometry to one Na1+, one Al3+, and one S6+ atom. In the third O2- site, O2- is bonded in a bent 150 degrees geometry to one Al3+ and one S6+ atom.
DOI: 10.17188/1710586
title: Materials Data on Al(V4Ge)3 by Materials Project

description: Al(V4Ge)3 crystallizes in the orthorhombic Pmmm space group. The structure is three-dimensional. there are five inequivalent V sites. In the first V site, V is bonded in a 6-coordinate geometry to ten V, two equivalent Al, and two equivalent Ge atoms. There are a spread of V–V bond distances ranging from 2.39–2.93 Å. Both V–Al bond lengths are 2.67 Å. Both V–Ge bond lengths are 2.67 Å. In the second V site, V is bonded in a 6-coordinate geometry to six V and four Ge atoms. There are one shorter (2.39 Å) and four longer (2.92 Å) V–V bond lengths. All V–Ge bond lengths are 2.67 Å. In the third V site, V is bonded in a 6-coordinate geometry to ten V, one Al, and three Ge atoms. There are a spread of V–V bond distances ranging from 2.38–2.93 Å. The V–Al bond length is 2.67 Å. All V–Ge bond lengths are 2.67 Å. In the fourth V site, V is bonded in a 6-coordinate geometry to ten V, two equivalent Al, and two equivalent Ge atoms. There are one shorter (2.38 Å) and one longer (2.39 Å) V–V bond lengths. Both V–Al bond lengths are 2.67 Å. Both V–Ge bond lengths are 2.67 Å. In the fifth V site, V is bonded in a 6-coordinate geometry to six V and four Ge atoms. Both V–V bond lengths are 2.39 Å. All V–Ge bond lengths are 2.67 Å. Al is bonded to twelve V atoms to form AlV12 cuboctahedra that share edges with two equivalent GeV12 cuboctahedra, edges with four equivalent AlV12 cuboctahedra, and faces with eight equivalent GeV12 cuboctahedra. There are two inequivalent Ge sites. In the first Ge site, Ge is bonded to twelve V atoms to form GeV12 cuboctahedra that share edges with two equivalent AlV12 cuboctahedra, edges with four equivalent GeV12 cuboctahedra, and faces with eight equivalent GeV12 cuboctahedra. In the second Ge site, Ge is bonded to twelve V atoms to form GeV12 cuboctahedra that share edges with six equivalent GeV12 cuboctahedra, faces with four equivalent AlV12 cuboctahedra, and faces with four equivalent GeV12 cuboctahedra.
DOI: 10.17188/1710587
title: Materials Data on NaNdFeWO6 by Materials Project

description: NaNdWFeO6 is Orthorhombic Perovskite-derived structured and crystallizes in the monoclinic P2_1 space group. The structure is three-dimensional. Na1+ is bonded in a 4-coordinate geometry to six O2- atoms. There are a spread of Na–O bond distances ranging from 2.37–2.91 Å. Nd3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Nd–O bond distances ranging from 2.38–2.69 Å. W6+ is bonded to six O2- atoms to form WO6 octahedra that share corners with six equivalent FeO6 octahedra. The corner-sharing octahedra tilt angles range from 23–35°. There are a spread of W–O bond distances ranging from 1.86–2.09 Å. Fe2+ is bonded to six O2- atoms to form FeO6 octahedra that share corners with six equivalent WO6 octahedra. The corner-sharing octahedra tilt angles range from 23–35°. There are a spread of Fe–O bond distances ranging from 2.11–2.25 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Nd3+, one W6+, and one Fe2+ atom. In the second O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Nd3+, one W6+, and one Fe2+ atom. In the third O2- site, O2- is bonded in a 5-coordinate geometry to two equivalent Na1+, one Nd3+, one W6+, and one Fe2+ atom. In the fourth O2- site, O2- is bonded in a 5-coordinate geometry to two equivalent Na1+, one Nd3+, one W6+, and one Fe2+ atom. In the fifth O2- site, O2- is bonded to two equivalent Nd3+, one W6+, and one Fe2+ atom to form distorted corner-sharing ONd2FeW tetrahedra. In the sixth O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Na1+, one W6+, and one Fe2+ atom.
DOI: 10.17188/1710588
title: Materials Data on CeLuS3 by Materials Project

description: LuCeS3 is Ilmenite-like structured and crystallizes in the orthorhombic C222_1 space group. The structure is three-dimensional. Lu3+ is bonded to six S2- atoms to form distorted LuS6 pentagonal pyramids that share corners with eight equivalent CeS6 octahedra, edges with two equivalent CeS6 octahedra, and faces with two equivalent LuS6 pentagonal pyramids. The corner-sharing octahedra tilt angles range from 22–70°. There are a spread of Lu–S bond distances ranging from 2.70–2.79 Å. Ce3+ is bonded to six S2- atoms to form CeS6 octahedra that share corners with two equivalent CeS6 octahedra, corners with eight equivalent LuS6 pentagonal pyramids, edges with two equivalent CeS6 octahedra, and edges with two equivalent LuS6 pentagonal pyramids. The corner-sharing octahedral tilt angles are 57°. There are four shorter (2.80 Å) and two longer (2.83 Å) Ce–S bond lengths. There are two inequivalent S2- sites. In the first S2- site, S2- is bonded in a distorted rectangular see-saw-like geometry to two equivalent Lu3+ and two equivalent Ce3+ atoms. In the second S2- site, S2- is bonded to two equivalent Lu3+ and two equivalent Ce3+ atoms to form corner-sharing SCe2Lu2 tetrahedra.
DOI: 10.17188/1710589
title: Materials Data on Li2VF6 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: 10.23670/irj.2024.140.9.6
title: Результаты тестовых исследований режимов микросварки

description: Международный научно-исследовательский журнал, Выпуск 2 (140) 2024
DOI: 10.25625/rbjibu/daylwm
title: 4Yangge-Ruine.mp4

description: Yangge in der Ruine einer alten Grundschule im Dorf Wangqiao, Musik: Kinderlied „Zeitungverkaufen“, Traditionelle chinesische Musikinstrumente, aufgenommen am 16.02.2013.
DOI: 10.25625/rbjibu/yagle0
title: 1Dachang-Yangge.mp4

description: „Yangge auf dem großen Platz“ vor dem Haus des Dorfkomitees Wangqiao, Yangge-Melodie „Eine schwingende Truppe“ (Da Baidui), Traditionelle chinesische Musikinstrumente, aufgenommen am 16.02.2013.
DOI: 10.6084/m9.figshare.14471492
title: Additional file 1 of Genome-wide association and transcriptome studies identify candidate genes and pathways for feed conversion ratio in pigs

description: Additional file 1: Table S1. Description of quantitative trait loci (QTL) in the regions significantly associated with FCR.
DOI: 10.5281/zenodo.10669993
title: Microstructured large-area photoconductive terahertz emitters driven at high average power

description: This dataset accompanies the paper "Microstructured large-area photoconductive terahertz emitters driven at high average power"

General data acquisition:

THz is generated with the Microstructured large-area photoconductive terahertz emitters at room temperature. The excitation pump power is controlled by a motorized lambda/2-waveplate  in connection with a thin-film polarizer. The bias voltage is generated with a waveforgenerator (keysight 33500B) in combination with a voltage amplifier (Falco WMA-300). The probe beam for electro-optic sampling (EOS) is guided over an oscillating delay line, having a delay range of approximately 15 ps and a shaking frequency of 1 Hz, leading to 155 THz traces in over 78 s measurement time.

THz traces obtained with EOS and a lock-in amplifier for low noise detection. THz average power is measured with a pyroelectric thin-film detector (THz 20, SLT GmbH) calibrated by the German Metrology Institute (PTB) and recorded with a lock-in amplifier for low noise detection. The recorded data via lock-in amplifier are saved as HDF-5 format.

HDF-5 is an efficient (binary), cross-platform data format and can be read easily by i.e. Python or Matlab. The graphical user interface “HDFView” can be downloaded for free (after registration) from https://www.hdfgroup.org/downloads/hdfview/. It allows to explore the folder structure of an HDF-5 file but is not necessary when using Python or Matlab.

The structure of a single HDF-5 from the uploaded raw data is



A folder called "AI", standing for analog input



The dataset "AI 1" stands for the first analog channel, containing the position of the scanning delay line. The voltage can be converted to “THz time” with a conversion factor, where 20 V corresponds to a 15 ps delay.

The dataset “AI 2”, is a voltage signal from the transimpedance amplifier and is proportional to the THz electric field.




There are additional attributes in the root-folder of the HDF-5 file.

The processed data (used in the figures) can be found in the files labeled Fig. X in each folder there is a text file "read me" that explains about recording and reading the data.
description: The research work presented in this paper was funded by the German Research Foundation (“Deutsche Forschungsgemeinschaft”) (DFG) under Project-ID 287022738 TRR 196 for Project M01. Funded by the Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) under Germany's Excellence Strategy – EXC-2033 – Projektnummer 390677874 - Resolv. The project "terahertz.NRW" receives funding from the programme "Netzwerke 2021", an initiative of the Ministry of Culture and Science of the State of Northrhine Westphalia. The sole responsibility for the content of this publication lies with the authors.
DOI: 10.5281/zenodo.10669994
title: Microstructured large-area photoconductive terahertz emitters driven at high average power

description: This dataset accompanies the paper "Microstructured large-area photoconductive terahertz emitters driven at high average power"

General data acquisition:

THz is generated with the Microstructured large-area photoconductive terahertz emitters at room temperature. The excitation pump power is controlled by a motorized lambda/2-waveplate  in connection with a thin-film polarizer. The bias voltage is generated with a waveforgenerator (keysight 33500B) in combination with a voltage amplifier (Falco WMA-300). The probe beam for electro-optic sampling (EOS) is guided over an oscillating delay line, having a delay range of approximately 15 ps and a shaking frequency of 1 Hz, leading to 155 THz traces in over 78 s measurement time.

THz traces obtained with EOS and a lock-in amplifier for low noise detection. THz average power is measured with a pyroelectric thin-film detector (THz 20, SLT GmbH) calibrated by the German Metrology Institute (PTB) and recorded with a lock-in amplifier for low noise detection. The recorded data via lock-in amplifier are saved as HDF-5 format.

HDF-5 is an efficient (binary), cross-platform data format and can be read easily by i.e. Python or Matlab. The graphical user interface “HDFView” can be downloaded for free (after registration) from https://www.hdfgroup.org/downloads/hdfview/. It allows to explore the folder structure of an HDF-5 file but is not necessary when using Python or Matlab.

The structure of a single HDF-5 from the uploaded raw data is



A folder called "AI", standing for analog input



The dataset "AI 1" stands for the first analog channel, containing the position of the scanning delay line. The voltage can be converted to “THz time” with a conversion factor, where 20 V corresponds to a 15 ps delay.

The dataset “AI 2”, is a voltage signal from the transimpedance amplifier and is proportional to the THz electric field.




There are additional attributes in the root-folder of the HDF-5 file.

The processed data (used in the figures) can be found in the files labeled Fig. X in each folder there is a text file "read me" that explains about recording and reading the data.
description: The research work presented in this paper was funded by the German Research Foundation (“Deutsche Forschungsgemeinschaft”) (DFG) under Project-ID 287022738 TRR 196 for Project M01. Funded by the Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) under Germany's Excellence Strategy – EXC-2033 – Projektnummer 390677874 - Resolv. The project "terahertz.NRW" receives funding from the programme "Netzwerke 2021", an initiative of the Ministry of Culture and Science of the State of Northrhine Westphalia. The sole responsibility for the content of this publication lies with the authors.
DOI: 10.25625/rbjibu/6ilodc
title: 6Bootstanz-Theater.mp4

description: Bootstanz-Theater auf dem Privatgrundstück der Familie Hao, Musik: Yangge-Melodie „Da Yangge“ usw., Traditionelle chinesische Musikinstrumente， aufgenommen am 24.02.2013.
DOI: 10.6084/m9.figshare.14471507.v1
title: Additional file 5 of Genome-wide association and transcriptome studies identify candidate genes and pathways for feed conversion ratio in pigs

description: Additional file 5: Table S5. List of hypothalamus DEGs between Yorkshire pigs with high and low FCR.
DOI: 10.6084/m9.figshare.14471681
title: Additional file 8 of Isolation and genomic characterization of five novel strains of Erysipelotrichaceae from commercial pigs

description: Additional file 8: Table S1. Accession numbers, genome coverage and size, and the pathway of GalNAc of the strains downloaded from NCBI.
DOI: 10.6084/m9.figshare.14471547
title: Additional file 4 of Optimization of SPME–GC–MS and characterization of floral scents from Aquilegia japonica and A. amurensis flowers

description: Additional file 4: Table S3. The correlation between the six replicates in A. japonica.