cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1739708
title: Materials Data on Ca2BiN3 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: 10.17188/1739709
title: Materials Data on Zn11(CN5)2 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1739710
title: Materials Data on LaGa2Pt3 by Materials Project

description: LaPt3Ga2 crystallizes in the hexagonal P6/mmm space group. The structure is three-dimensional. La2+ is bonded to twelve equivalent Pt2- atoms to form a mixture of edge, face, and corner-sharing LaPt12 cuboctahedra. All La–Pt bond lengths are 3.48 Å. Pt2- is bonded in a 12-coordinate geometry to four equivalent La2+ and four equivalent Ga2+ atoms. All Pt–Ga bond lengths are 2.61 Å. Ga2+ is bonded in a 6-coordinate geometry to six equivalent Pt2- atoms.
DOI: 10.6084/m9.figshare.13335758
title: PS C (Chapter II, Evans Dissertation)

description: This is drone product set C from Chapter II of Alexandra's dissertation.<br>The orthomosaic and DSM show East Branch Piscataqua River in Falmouth, ME, USA. The imagery was collected on October 16, 2017 using a DJI Phantom 3 Professional drone. Ground control points were used for georeferencing the imagery during SfM processing, but note that the elevation values in the DSM are only useful for relative topography across the site. The Topcon Hiper Lite+ recorded inaccurately negative elevation values which limits the dataset's compatibility with other datasets and the DSM will likely need to be corrected for relative compatibility. The XY locations are more reliable based on checks against alignment with base maps in ArcGIS. The drone PS' relative accuracy was deemed acceptable for the purposes in Chapter II. Automated drone flight paths were used to collect nadir and angled aerial images with sufficient image overlap for SfM processing in Agisoft PhotoScan Professional. The PhotoScan-generated report includes additional details on the SfM processing workflow and on the drone products.<br>Please see Alexandra's dissertation (University of New Hampshire) for more information on the drone products and project.<br>These materials were made using resources from an NSF EPSCoR funded project “RII Track-2 FEC: Strengthening the scientific basis for decision-making about dams: Multi-scale, coupled-systems research on ecological, social, and economic trade-offs” (a.k.a. "Future of Dams"). Support for this project is provided by the National Science Foundation’s Research Infrastructure Improvement NSF #IIA-1539071. Any opinions, findings, and conclusions or recommendations expressed in this material are those of the author(s) and do not necessarily reflect the views of the National Science Foundation.
DOI: 10.6084/m9.figshare.13704559.v2
title: Supplemental tables and figure

description: Supplemental tables and figure
DOI: 10.6084/m9.figshare.13668803
title: Cyclomatic or Cognitive? Which Complexity Metric represents better Code Understandability

description: Raw data for the replicability
DOI: 10.6084/m9.figshare.13668803.v1
title: Cyclomatic or Cognitive? Which Complexity Metric represents better Code Understandability

description: Raw data for the replicability
DOI: 10.17188/1739711
title: Materials Data on Sr3Ru3N5 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: 10.6084/m9.figshare.13697490
title: NGS Dataset: A multiplexed, automated evolution pipeline enables scalable discovery and characterization of biosensors

description: Next Generation Sequencing (NGS) data was used to measure the self-cleavage of libraries of ribozyme using the CleaveSeq method as described in reference. This repository contains the raw data for these sequencing runs. Each experiment is represented by the following data:• Raw sequencing fastq files; each of these may contain data for multiple experiments identified by embedded barcode prefixes and suffixes.• Counts files. Each raw sequence file was reduced to a counts file that list all of the unique full sequences contained in the fastq file along with counts of how many times that exact sequence occurred.• Metadata that lists, for each individual experiment, the raw fastq and count file containing data for the experiment along with prefixes and suffixes that identify which reads in the file correspond to cleaved and to uncleaved molecules in the experiment. <br>Notes:• We typically use data which matches the specified prefixes and suffixes with up to one error in each.• The same experiment may have multiple entries – this indicates that an analysis used data from multiple independent experiments.• Since the counts files compactly represent the relevant information from the fastq files, we are only uploading one set of raw fastq files for reference purposes. <br>
DOI: 10.6084/m9.figshare.13335758.v1
title: PS C (Chapter II, Evans Dissertation)

description: This is drone product set C from Chapter II of Alexandra's dissertation.<br>The orthomosaic and DSM show East Branch Piscataqua River in Falmouth, ME, USA. The imagery was collected on October 16, 2017 using a DJI Phantom 3 Professional drone. Ground control points were used for georeferencing the imagery during SfM processing, but note that the elevation values in the DSM are only useful for relative topography across the site. The Topcon Hiper Lite+ recorded inaccurately negative elevation values which limits the dataset's compatibility with other datasets and the DSM will likely need to be corrected for relative compatibility. The XY locations are more reliable based on checks against alignment with base maps in ArcGIS. The drone PS' relative accuracy was deemed acceptable for the purposes in Chapter II. Automated drone flight paths were used to collect nadir and angled aerial images with sufficient image overlap for SfM processing in Agisoft PhotoScan Professional. The PhotoScan-generated report includes additional details on the SfM processing workflow and on the drone products.<br>Please see Alexandra's dissertation (University of New Hampshire) for more information on the drone products and project.<br>These materials were made using resources from an NSF EPSCoR funded project “RII Track-2 FEC: Strengthening the scientific basis for decision-making about dams: Multi-scale, coupled-systems research on ecological, social, and economic trade-offs” (a.k.a. "Future of Dams"). Support for this project is provided by the National Science Foundation’s Research Infrastructure Improvement NSF #IIA-1539071. Any opinions, findings, and conclusions or recommendations expressed in this material are those of the author(s) and do not necessarily reflect the views of the National Science Foundation.
DOI: 10.17188/1739712
title: Materials Data on Ba2GdGaTe5 by Materials Project

description: Ba2GdGaTe5 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are two inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded in a 8-coordinate geometry to eight Te2- atoms. There are a spread of Ba–Te bond distances ranging from 3.51–3.92 Å. In the second Ba2+ site, Ba2+ is bonded in a 8-coordinate geometry to eight Te2- atoms. There are a spread of Ba–Te bond distances ranging from 3.51–3.93 Å. Gd3+ is bonded to six Te2- atoms to form GdTe6 octahedra that share edges with two equivalent GdTe6 octahedra and edges with two equivalent GaTe4 tetrahedra. There are a spread of Gd–Te bond distances ranging from 3.08–3.26 Å. Ga3+ is bonded to four Te2- atoms to form GaTe4 tetrahedra that share edges with two equivalent GdTe6 octahedra. There are a spread of Ga–Te bond distances ranging from 2.60–2.74 Å. There are five inequivalent Te2- sites. In the first Te2- site, Te2- is bonded to four Ba2+ and one Ga3+ atom to form distorted edge-sharing TeBa4Ga square pyramids. In the second Te2- site, Te2- is bonded in a 5-coordinate geometry to three Ba2+, one Gd3+, and one Ga3+ atom. In the third Te2- site, Te2- is bonded in a 5-coordinate geometry to three Ba2+, one Gd3+, and one Ga3+ atom. In the fourth Te2- site, Te2- is bonded in a 5-coordinate geometry to three Ba2+ and two equivalent Gd3+ atoms. In the fifth Te2- site, Te2- is bonded in a 6-coordinate geometry to three Ba2+, two equivalent Gd3+, and one Ga3+ atom.
DOI: 10.17633/rd.brunel.13372589.v1
title: Historical Documents of the Irish Avant-Garde

description: Historical Documents of the Irish Avant-Garde, January 2015<br>The purpose of the research was to open up an imaginative space where an Irish Avant-garde could have happened and to conduct an exercise in ‘what if?’ The work offers a fictional survey of avant-garde composition in Ireland from the late 19th to early 21st centuries. <br>Dr Walshe conducted research into the structures and establishments of Irish artistic history to investigate how histories of music are created, but found that there was no real data. She subsequently began bending history and explored a potential tradition of experimentalism in Ireland. Following this methodology, the research project opened up into a history of the imaginary which operates in parallel to the Irish cultural mainstream.<br>Dr Walshe's research showed that linear narratives in music are often fictional anyway due to the editing they tend to undergo. She unearthed parallels to Irish culture as a whole, which tends to expel its artists first before welcoming them back into their realm once they’re dead. The creation of an imaginative space in this work showed that an Irish avant-garde with revolutionaries, female, queer and other artists, who may have existed and subsequently been written out of history, could have happened. <br>The full recordings are available here: Historical Documents of the Irish Avant Garde | Various Artists | Migro Records (bandcamp.com)<br>
DOI: 10.6084/m9.figshare.13697490.v1
title: NGS Dataset: A multiplexed, automated evolution pipeline enables scalable discovery and characterization of biosensors

description: Next Generation Sequencing (NGS) data was used to measure the self-cleavage of libraries of ribozyme using the CleaveSeq method as described in reference. This repository contains the raw data for these sequencing runs. Each experiment is represented by the following data:• Raw sequencing fastq files; each of these may contain data for multiple experiments identified by embedded barcode prefixes and suffixes.• Counts files. Each raw sequence file was reduced to a counts file that list all of the unique full sequences contained in the fastq file along with counts of how many times that exact sequence occurred.• Metadata that lists, for each individual experiment, the raw fastq and count file containing data for the experiment along with prefixes and suffixes that identify which reads in the file correspond to cleaved and to uncleaved molecules in the experiment. <br>Notes:• We typically use data which matches the specified prefixes and suffixes with up to one error in each.• The same experiment may have multiple entries – this indicates that an analysis used data from multiple independent experiments.• Since the counts files compactly represent the relevant information from the fastq files, we are only uploading one set of raw fastq files for reference purposes. <br>
DOI: 10.17188/1739713
title: Materials Data on FePHO5 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: 10.6084/m9.figshare.13611215.v2
title: The end-Cretaceous and the origin of modern Neotropical rainforests data

description: This folder contains the raw data and files required for replicating the analysis used in the manuscript "Extinction at the end-Cretaceous and the origin of modern Neotropical rainforests".
DOI: 10.17188/1739714
title: Materials Data on Cr2Pb3N4 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: 10.6084/m9.figshare.13611215.v1
title: The end-Cretaceous and the origin of modern Neotropical rainforests data

description: This folder contains the raw data and files required for replicating the analysis used in the manuscript "Extinction at the end-Cretaceous and the origin of modern Neotropical rainforests".
DOI: 10.17188/1739715
title: Materials Data on Ca2Mn2O5 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: 10.6084/m9.figshare.13611215
title: The end-Cretaceous and the origin of modern Neotropical rainforests data

description: This folder contains the raw data and files required for replicating the analysis used in the manuscript "Extinction at the end-Cretaceous and the origin of modern Neotropical rainforests".
DOI: 10.6084/m9.figshare.13705774.v1
title: Observations of Ion Gyroharmonic Structuring in Second Harmonic Generation Stimulated Electromagnetic Emissions during Ionospheric Heating

description: This data contains .wave files collected during an ionosphere heating experiment conducted at the High Frequency Active Auroral Research Program (HAARP) facility conducted to investigate second harmonic generation in stimulated electromagnetic emissions
DOI: 10.17188/1739717
title: Materials Data on KGaFe(CN)6 by Materials Project

description: KFeGa(CN)6 is half-Heusler structured and crystallizes in the cubic F-43m space group. The structure is zero-dimensional and consists of four ferrum molecules, four kalium molecules, and four Ga(CN)6 clusters. In each Ga(CN)6 cluster, Ga3+ is bonded in an octahedral geometry to six equivalent N3- atoms. All Ga–N bond lengths are 2.04 Å. C+1.83+ is bonded in a distorted single-bond geometry to one N3- atom. The C–N bond length is 1.18 Å. N3- is bonded in a linear geometry to one Ga3+ and one C+1.83+ atom.
DOI: 10.17188/1739718
title: Materials Data on K2La4O7 by Materials Project

description: K2La4O7 crystallizes in the trigonal P-31m space group. The structure is three-dimensional. K1+ is bonded in a distorted hexagonal planar geometry to six equivalent O2- atoms. All K–O bond lengths are 3.29 Å. There are two inequivalent La3+ sites. In the first La3+ site, La3+ is bonded to four O2- atoms to form LaO4 trigonal pyramids that share corners with six equivalent LaO6 octahedra and a cornercorner with one LaO4 trigonal pyramid. The corner-sharing octahedral tilt angles are 63°. There are one shorter (2.15 Å) and three longer (2.33 Å) La–O bond lengths. In the second La3+ site, La3+ is bonded to six equivalent O2- atoms to form LaO6 octahedra that share corners with six equivalent LaO4 trigonal pyramids and edges with three equivalent LaO6 octahedra. All La–O bond lengths are 2.45 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a 3-coordinate geometry to two equivalent K1+ and three La3+ atoms. In the second O2- site, O2- is bonded in a linear geometry to two equivalent La3+ atoms.
DOI: 10.6084/m9.figshare.13704559.v3
title: Supplemental materials

description: Supplemental tables and figures
DOI: 10.17188/1739719
title: Materials Data on Ca2Mg by Materials Project

description: Ca2Mg crystallizes in the monoclinic C2/m space group. The structure is two-dimensional and consists of one Ca2Mg sheet oriented in the (0, 0, 1) direction. there are two inequivalent Ca sites. In the first Ca site, Ca is bonded to three equivalent Mg atoms to form a mixture of distorted edge and corner-sharing CaMg3 cuboctahedra. There are one shorter (3.41 Å) and two longer (3.49 Å) Ca–Mg bond lengths. In the second Ca site, Ca is bonded in a 4-coordinate geometry to four equivalent Mg atoms. There are two shorter (3.50 Å) and two longer (3.54 Å) Ca–Mg bond lengths. Mg is bonded in a 9-coordinate geometry to seven Ca and two equivalent Mg atoms. Both Mg–Mg bond lengths are 3.40 Å.
DOI: 10.17188/1739720
title: Materials Data on La3Pd4 by Materials Project

description: La3Pd4 crystallizes in the trigonal R-3 space group. The structure is three-dimensional. La is bonded in a 9-coordinate geometry to nine Pd atoms. There are a spread of La–Pd bond distances ranging from 2.97–3.46 Å. There are three inequivalent Pd sites. In the first Pd site, Pd is bonded in a 6-coordinate geometry to six equivalent La and two equivalent Pd atoms. Both Pd–Pd bond lengths are 2.94 Å. In the second Pd site, Pd is bonded in a 6-coordinate geometry to six equivalent La and two equivalent Pd atoms. In the third Pd site, Pd is bonded in a 10-coordinate geometry to seven equivalent La and three equivalent Pd atoms. There are one shorter (2.99 Å) and two longer (3.09 Å) Pd–Pd bond lengths.
DOI: 10.17188/1739721
title: Materials Data on Yb5(Ge5Rh2)2 by Materials Project

description: Yb5Rh4Ge10 crystallizes in the tetragonal P4/mbm space group. The structure is three-dimensional. there are three inequivalent Yb sites. In the first Yb site, Yb is bonded in a 8-coordinate geometry to four equivalent Rh and twelve Ge atoms. All Yb–Rh bond lengths are 3.24 Å. There are eight shorter (2.98 Å) and four longer (3.31 Å) Yb–Ge bond lengths. In the second Yb site, Yb is bonded to four equivalent Rh and eight Ge atoms to form face-sharing YbGe8Rh4 cuboctahedra. All Yb–Rh bond lengths are 3.09 Å. There are a spread of Yb–Ge bond distances ranging from 2.98–3.14 Å. In the third Yb site, Yb is bonded in a 8-coordinate geometry to four equivalent Rh and ten Ge atoms. All Yb–Rh bond lengths are 3.37 Å. There are a spread of Yb–Ge bond distances ranging from 3.23–3.37 Å. Rh is bonded in a 10-coordinate geometry to five Yb and five Ge atoms. There are a spread of Rh–Ge bond distances ranging from 2.45–2.56 Å. There are three inequivalent Ge sites. In the first Ge site, Ge is bonded in a 9-coordinate geometry to six Yb, two equivalent Rh, and one Ge atom. The Ge–Ge bond length is 2.41 Å. In the second Ge site, Ge is bonded in a 2-coordinate geometry to five Yb, two equivalent Rh, and one Ge atom. The Ge–Ge bond length is 2.63 Å. In the third Ge site, Ge is bonded in a 2-coordinate geometry to four Yb, two equivalent Rh, and two equivalent Ge atoms. Both Ge–Ge bond lengths are 2.87 Å.
DOI: 10.17188/1739723
title: Materials Data on PrSmSeS by Materials Project

description: SmPrSeS is Halite, Rock Salt-derived structured and crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. Sm is bonded to two equivalent Se and four equivalent S atoms to form SmSe2S4 octahedra that share corners with six equivalent SmSe2S4 octahedra, edges with four equivalent SmSe2S4 octahedra, and edges with eight equivalent PrSe4S2 octahedra. The corner-sharing octahedral tilt angles are 0°. Both Sm–Se bond lengths are 2.93 Å. All Sm–S bond lengths are 2.93 Å. Pr is bonded to four equivalent Se and two equivalent S atoms to form PrSe4S2 octahedra that share corners with six equivalent PrSe4S2 octahedra, edges with four equivalent PrSe4S2 octahedra, and edges with eight equivalent SmSe2S4 octahedra. The corner-sharing octahedral tilt angles are 0°. All Pr–Se bond lengths are 2.93 Å. Both Pr–S bond lengths are 2.93 Å. Se is bonded to two equivalent Sm and four equivalent Pr atoms to form SePr4Sm2 octahedra that share corners with six equivalent SePr4Sm2 octahedra, edges with four equivalent SePr4Sm2 octahedra, and edges with eight equivalent SPr2Sm4 octahedra. The corner-sharing octahedral tilt angles are 0°. S is bonded to four equivalent Sm and two equivalent Pr atoms to form SPr2Sm4 octahedra that share corners with six equivalent SPr2Sm4 octahedra, edges with four equivalent SPr2Sm4 octahedra, and edges with eight equivalent SePr4Sm2 octahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1739724
title: Materials Data on Li2MnV3O8 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: 10.17188/1739725
title: Materials Data on K10Tl7 by Materials Project

description: K10Tl7 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are ten inequivalent K sites. In the first K site, K is bonded in a 3-coordinate geometry to three Tl atoms. There are a spread of K–Tl bond distances ranging from 3.77–3.95 Å. In the second K site, K is bonded in a 2-coordinate geometry to four Tl atoms. There are a spread of K–Tl bond distances ranging from 3.54–3.92 Å. In the third K site, K is bonded in a 5-coordinate geometry to five Tl atoms. There are a spread of K–Tl bond distances ranging from 3.60–4.05 Å. In the fourth K site, K is bonded in a 4-coordinate geometry to four Tl atoms. There are a spread of K–Tl bond distances ranging from 3.66–3.91 Å. In the fifth K site, K is bonded in a 5-coordinate geometry to five Tl atoms. There are a spread of K–Tl bond distances ranging from 3.66–4.05 Å. In the sixth K site, K is bonded in a 4-coordinate geometry to four Tl atoms. There are a spread of K–Tl bond distances ranging from 3.72–3.81 Å. In the seventh K site, K is bonded in a 3-coordinate geometry to three Tl atoms. There are a spread of K–Tl bond distances ranging from 3.59–4.00 Å. In the eighth K site, K is bonded in a 5-coordinate geometry to six Tl atoms. There are a spread of K–Tl bond distances ranging from 3.74–4.09 Å. In the ninth K site, K is bonded in a 4-coordinate geometry to four Tl atoms. There are a spread of K–Tl bond distances ranging from 3.75–4.07 Å. In the tenth K site, K is bonded in a 3-coordinate geometry to three Tl atoms. There are a spread of K–Tl bond distances ranging from 3.73–4.01 Å. There are seven inequivalent Tl sites. In the first Tl site, Tl is bonded in a 10-coordinate geometry to six K and four Tl atoms. There are a spread of Tl–Tl bond distances ranging from 3.28–3.33 Å. In the second Tl site, Tl is bonded in a 10-coordinate geometry to six K and four Tl atoms. There are two shorter (3.33 Å) and one longer (3.34 Å) Tl–Tl bond lengths. In the third Tl site, Tl is bonded in a 10-coordinate geometry to six K and four Tl atoms. There are a spread of Tl–Tl bond distances ranging from 3.27–3.40 Å. In the fourth Tl site, Tl is bonded in a 12-coordinate geometry to six K and six Tl atoms. There are a spread of Tl–Tl bond distances ranging from 3.30–3.54 Å. In the fifth Tl site, Tl is bonded in a 10-coordinate geometry to six K and four Tl atoms. There are one shorter (3.32 Å) and one longer (3.37 Å) Tl–Tl bond lengths. In the sixth Tl site, Tl is bonded in a 10-coordinate geometry to six K and four Tl atoms. The Tl–Tl bond length is 3.32 Å. In the seventh Tl site, Tl is bonded in a 11-coordinate geometry to five K and six Tl atoms.