cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.6084/m9.figshare.13674136.v1
title: Supplementary Material for: Detection of Major Cardioembolic Sources in Real-World Patients with Ischemic Stroke or Transient Ischemic Attack of Undetermined Cause

description: <b><i>Background/Aim:</i></b> Current guidelines recommend transthoracic echocardiography (TTE) and ambulatory rhythm monitoring following ischemic stroke or transient ischemic attack (TIA) of undetermined cause for identifying cardioembolic sources (CES). Due to ongoing controversies about this routine strategy, we evaluated its yield in a real-world setting. <b><i>Methods:</i></b> In a tertiary medical center, we retrospectively evaluated consecutive patients with ischemic stroke or TIA of undetermined cause, who (after standard work-up) underwent TTE, ambulatory rhythm monitoring, or both. CES were classified as major if probably related to ischemic events and warranting a change of therapy. <b><i>Results:</i></b> Between January 2014 and December 2017, 674 patients had ischemic stroke or TIA of undetermined cause. Of all 484 patients (71.8%) who underwent TTE, 9 (1.9%) had a major CES. However, 7 of them had already been identified for cardiac evaluation due to new major electrocardiographic abnormalities or cardiac symptoms. Thus, only 2 patients (0.4%) truly benefitted from unselected TTE screening. Ambulatory rhythm monitoring was performed in 411 patients (61.0%) and revealed AF in 10 patients (2.4%). <b><i>Conclusion:</i></b> Detecting a major CES is essential because appropriate treatment lowers the risk of recurrent stroke. Nonetheless, in this real-world study that aimed at routine use of TTE and ambulatory rhythm monitoring in patients with ischemic stroke or TIA of undetermined cause, the prevalence of major CES was low. Most patients with major CES on TTE already had an indication for referral to a cardiologist, suggesting that major CES might also have been identified with a much more selective use of TTE.
DOI: 10.17188/1683883
title: Materials Data on SrSi3Ni by Materials Project

description: SrNiSi3 crystallizes in the tetragonal I4mm space group. The structure is three-dimensional. Sr2+ is bonded to twelve Si+1.33- atoms to form a mixture of face, edge, and corner-sharing SrSi12 cuboctahedra. There are a spread of Sr–Si bond distances ranging from 3.11–3.26 Å. Ni2+ is bonded in a 5-coordinate geometry to five Si+1.33- atoms. There are four shorter (2.34 Å) and one longer (2.40 Å) Ni–Si bond lengths. There are two inequivalent Si+1.33- sites. In the first Si+1.33- site, Si+1.33- is bonded in a 9-coordinate geometry to four equivalent Sr2+, one Ni2+, and four equivalent Si+1.33- atoms. All Si–Si bond lengths are 2.59 Å. In the second Si+1.33- site, Si+1.33- is bonded in a 8-coordinate geometry to four equivalent Sr2+, two equivalent Ni2+, and two equivalent Si+1.33- atoms.
DOI: 10.17632/7bjhtwpfg3.1
title: COVID-19 Dental Journals

description: This dataset contains information of output of dental journals on COVID-19.
DOI: 10.17188/1683884
title: Materials Data on Hf6BCl14 by Materials Project

description: Hf6BCl14 crystallizes in the orthorhombic Cmce space group. The structure is three-dimensional. there are two inequivalent Hf sites. In the first Hf site, Hf is bonded to one B and five Cl atoms to form a mixture of corner and edge-sharing HfBCl5 octahedra. The corner-sharing octahedra tilt angles range from 0–46°. The Hf–B bond length is 2.32 Å. There are a spread of Hf–Cl bond distances ranging from 2.49–2.64 Å. In the second Hf site, Hf is bonded to one B and five Cl atoms to form a mixture of distorted corner and edge-sharing HfBCl5 octahedra. The corner-sharing octahedra tilt angles range from 0–46°. The Hf–B bond length is 2.25 Å. There are a spread of Hf–Cl bond distances ranging from 2.50–3.05 Å. B is bonded in an octahedral geometry to six Hf atoms. There are five inequivalent Cl sites. In the first Cl site, Cl is bonded in an L-shaped geometry to two Hf atoms. In the second Cl site, Cl is bonded in a bent 150 degrees geometry to two equivalent Hf atoms. In the third Cl site, Cl is bonded in an L-shaped geometry to two equivalent Hf atoms. In the fourth Cl site, Cl is bonded in a 3-coordinate geometry to three Hf atoms. In the fifth Cl site, Cl is bonded in an L-shaped geometry to two Hf atoms.
DOI: 10.17188/1683885
title: Materials Data on KNi4(PO4)3 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17632/xczzcyjd69.1
title: Datasets supporting fruit components biomass and carbon stocks derivation of Strychnos madagascariensis and S. spinosa

description: These datasets are associated with a research article currently under review in a Journal. They support findings of an original manuscript which aimed to determine biomass allocation between fruit components of Strychnos madagascariensis and Strychnos spinosa and to investigate the carbon stocks sequestrated by fruits. They also contain scripts/codes of data analyses carried out using the R-software (R DEVELOPMENT CORE TEAM: a language and environment for statistical computing). The research was conducted with the intention of assessing the relevance of allometric (regression) techniques in the quantification of biomass and carbon stocks sequestrated by fruits in response to the growing need to evaluate the wild fruit biomass production of savannah ecosystems for both commercial and ecological purposes. Details of the findings are to be found in the article that will be available in coming days. Raw data-tables were obtained from a harvest of 400 ripe fruits of both plant species. Biomass measurements were done on individual fruits and laboratory work was made with grouped fruits. Further details have to be found in the article.
DOI: 10.17188/1683886
title: Materials Data on HoCrO3 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: 10.17188/1683887
title: Materials Data on Zn9Fe4 by Materials Project

description: Fe4Zn9 is Bergman Structure: Mg32(Al,Zn)49 Bergman-derived structured and crystallizes in the cubic I-43m space group. The structure is three-dimensional. there are two inequivalent Fe sites. In the first Fe site, Fe is bonded to three equivalent Fe and nine Zn atoms to form a mixture of face and corner-sharing FeZn9Fe3 cuboctahedra. All Fe–Fe bond lengths are 2.45 Å. There are a spread of Fe–Zn bond distances ranging from 2.63–2.68 Å. In the second Fe site, Fe is bonded in a 12-coordinate geometry to six Fe and six Zn atoms. All Fe–Fe bond lengths are 2.62 Å. There are three shorter (2.57 Å) and three longer (2.62 Å) Fe–Zn bond lengths. There are two inequivalent Zn sites. In the first Zn site, Zn is bonded in a 3-coordinate geometry to three Fe and four equivalent Zn atoms. There are a spread of Zn–Zn bond distances ranging from 2.63–3.07 Å. In the second Zn site, Zn is bonded in a 11-coordinate geometry to four Fe and nine Zn atoms. The Zn–Zn bond length is 2.58 Å.
DOI: 10.17188/1683889
title: Materials Data on CaLuMn2O6 by Materials Project

description: CaLuMn2O6 is Orthorhombic Perovskite-derived structured and crystallizes in the monoclinic Pm space group. The structure is three-dimensional. there are two inequivalent Ca2+ sites. In the first Ca2+ site, Ca2+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Ca–O bond distances ranging from 2.31–2.62 Å. In the second Ca2+ site, Ca2+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Ca–O bond distances ranging from 2.31–2.63 Å. There are two inequivalent Lu3+ sites. In the first Lu3+ site, Lu3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Lu–O bond distances ranging from 2.22–2.66 Å. In the second Lu3+ site, Lu3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Lu–O bond distances ranging from 2.21–2.66 Å. There are two inequivalent Mn+3.50+ sites. In the first Mn+3.50+ site, Mn+3.50+ is bonded to six O2- atoms to form corner-sharing MnO6 octahedra. The corner-sharing octahedra tilt angles range from 28–38°. There are a spread of Mn–O bond distances ranging from 1.96–2.00 Å. In the second Mn+3.50+ site, Mn+3.50+ is bonded to six O2- atoms to form corner-sharing MnO6 octahedra. The corner-sharing octahedra tilt angles range from 28–37°. There are a spread of Mn–O bond distances ranging from 1.95–2.04 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a 5-coordinate geometry to one Ca2+, two Lu3+, and two Mn+3.50+ atoms. In the second O2- site, O2- is bonded in a 5-coordinate geometry to two Ca2+, one Lu3+, and two Mn+3.50+ atoms. In the third O2- site, O2- is bonded in a 5-coordinate geometry to one Ca2+, two Lu3+, and two Mn+3.50+ atoms. In the fourth O2- site, O2- is bonded in a 5-coordinate geometry to two Ca2+, one Lu3+, and two Mn+3.50+ atoms. In the fifth O2- site, O2- is bonded to one Ca2+, one Lu3+, and two equivalent Mn+3.50+ atoms to form distorted corner-sharing OCaLuMn2 trigonal pyramids. In the sixth O2- site, O2- is bonded to one Ca2+, one Lu3+, and two equivalent Mn+3.50+ atoms to form distorted corner-sharing OCaLuMn2 tetrahedra. In the seventh O2- site, O2- is bonded to one Ca2+, one Lu3+, and two equivalent Mn+3.50+ atoms to form distorted corner-sharing OCaLuMn2 tetrahedra. In the eighth O2- site, O2- is bonded to one Ca2+, one Lu3+, and two equivalent Mn+3.50+ atoms to form distorted corner-sharing OCaLuMn2 tetrahedra.
DOI: 10.17632/ft7r4wrnt3.1
title: PREOPERATIVE WALKING RECOMMENDATION FOR NON-CARDIAC SURGERY PATIENTS TO REDUCE THE LENGTH OF HOSPITAL STAY: A RANDOMIZED CONTROL TRIAL

description: Background: Even though the importance of preparing patients for a surgical event is recognized, there are still gaps about the benefit of improving functional capacity by walking during the waiting time among patients scheduled for non-cardiac surgery. This study aimed to evaluate the impact of pre-surgical walking in-hospital length of stay, early ambulation, and the appearance of complications after surgery among patients scheduled for non-cardiac surgery. Methods: A two-arm, single-blinded randomized controlled trial was developed from May 2016 to August 2017. Eligible outpatients scheduled for non-cardiac surgery, capable of walking, were randomized (2:1 ratio) to receive a prescription of walking 150 minutes/week during the whole pre-surgical waiting time (n = 249) or conventional care (n = 119). The primary outcome was the difference in hospital length of stay. Secondary results were time to the first ambulation during hospitalization, description of ischemic events during hospitalization, six months of hospital discharge, and the walking continuation. We performed an intention to treat analysis and compared length of stay between both groups by Kaplan-Meier estimator (log-rank test). Results: There were no significant differences in the length of hospital stay between both groups (log-rank test p = 0.367) and no differences in the first ambulation time during hospitalization (log-rank test p=0.299). Similar rates of postoperative complications were observed in both groups, but the intervention group patients continued to practice walking six months after discharge (p&lt;0.001). Conclusion: Our study is the first clinical trial evaluating the impact of walking before non-cardiac surgery in the length of stay, early ambulation, and complications after surgery. Prescription of walking for patients before non-cardiac surgery had no significant effect in reducing the length of stay, early ambulation, and complications but promoted the walking up six months after discharge. The results become a crucial element for further investigation.
DOI: 10.17188/1683891
title: Materials Data on EuPbAu2 by Materials Project

description: EuAu2Pb is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Eu is bonded in a body-centered cubic geometry to eight equivalent Au and six equivalent Pb atoms. All Eu–Au bond lengths are 3.16 Å. All Eu–Pb bond lengths are 3.64 Å. Au is bonded in a body-centered cubic geometry to four equivalent Eu and four equivalent Pb atoms. All Au–Pb bond lengths are 3.16 Å. Pb is bonded in a 8-coordinate geometry to six equivalent Eu and eight equivalent Au atoms.
DOI: 10.17188/1683892
title: Materials Data on Fe2Cu(PO5)2 by Materials Project

description: Fe2Cu(PO5)2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Fe is bonded to six O atoms to form FeO6 octahedra that share corners with two equivalent FeO6 octahedra and corners with four equivalent PO4 tetrahedra. The corner-sharing octahedral tilt angles are 55°. There are a spread of Fe–O bond distances ranging from 1.95–2.14 Å. Cu is bonded in a distorted square co-planar geometry to six O atoms. There are a spread of Cu–O bond distances ranging from 1.85–2.51 Å. P is bonded to four O atoms to form PO4 tetrahedra that share corners with four equivalent FeO6 octahedra. The corner-sharing octahedra tilt angles range from 37–47°. There are a spread of P–O bond distances ranging from 1.52–1.59 Å. There are five inequivalent O sites. In the first O site, O is bonded in a distorted bent 150 degrees geometry to one Fe and one P atom. In the second O site, O is bonded in a bent 150 degrees geometry to one Fe and one P atom. In the third O site, O is bonded in a 3-coordinate geometry to one Fe, one Cu, and one P atom. In the fourth O site, O is bonded in a 2-coordinate geometry to one Fe, one Cu, and one P atom. In the fifth O site, O is bonded in a distorted trigonal planar geometry to two equivalent Fe and one Cu atom.
DOI: 10.17632/wxb8tf74p7.1
title: The effect of zinc concentration upon electronic structure, optical and dielectric properties of Cd1− xZnxTe alloy: TB-mBJ investigation
DOI: 10.17188/1683893
title: Materials Data on InC4Br7N4 by Materials Project

description: InBr6C4N4Br crystallizes in the monoclinic P2/c space group. The structure is zero-dimensional and consists of four C4N4Br clusters and four InBr6 clusters. In each C4N4Br cluster, there are two inequivalent C4+ sites. In the first C4+ site, C4+ is bonded in a single-bond geometry to one N3- atom. The C–N bond length is 1.18 Å. In the second C4+ site, C4+ is bonded in a single-bond geometry to one N3- atom. The C–N bond length is 1.18 Å. There are two inequivalent N3- sites. In the first N3- site, N3- is bonded in a single-bond geometry to one C4+ and one Br1- atom. The N–Br bond length is 3.32 Å. In the second N3- site, N3- is bonded in a single-bond geometry to one C4+ and one Br1- atom. The N–Br bond length is 3.40 Å. Br1- is bonded in a distorted rectangular see-saw-like geometry to four N3- atoms. In each InBr6 cluster, In3+ is bonded in an octahedral geometry to six Br1- atoms. There are two shorter (2.67 Å) and four longer (2.68 Å) In–Br bond lengths. There are three inequivalent Br1- sites. In the first Br1- site, Br1- is bonded in a single-bond geometry to one In3+ atom. In the second Br1- site, Br1- is bonded in a single-bond geometry to one In3+ atom. In the third Br1- site, Br1- is bonded in a single-bond geometry to one In3+ atom.
DOI: 10.17188/1683894
title: Materials Data on FeOF 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: 10.17632/htdkz4539r.1
title: Screening for common mental disorders using the SRQ-20 in medical students from Porto Velho-RO - Dataset

description: Database (raw and analyzed) and metadata concerning the analysis of prevalence for common mental disorders using the SRQ-20 in medical students from Porto Velho, Brazil. [Base de dados (bruta e analisada) e metadados relativos à análise da prevalência de TMC utilizando o SRQ-20 em estudantes de medicina de Porto Velho-RO.]
DOI: 10.17188/1683895
title: Materials Data on Li5CoOF5 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: 10.17188/1683897
title: Materials Data on AlIn2N3 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: 10.17188/1683898
title: Materials Data on Sr4CaYGa2(Cu2O7)2 by Materials Project

description: Sr4CaYGa2(Cu2O7)2 crystallizes in the monoclinic C2 space group. The structure is three-dimensional. there are two inequivalent Sr2+ sites. In the first Sr2+ site, Sr2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Sr–O bond distances ranging from 2.48–3.13 Å. In the second Sr2+ site, Sr2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Sr–O bond distances ranging from 2.48–3.12 Å. Ca2+ is bonded in a body-centered cubic geometry to eight O2- atoms. There are a spread of Ca–O bond distances ranging from 2.44–2.51 Å. Y3+ is bonded in a body-centered cubic geometry to eight O2- atoms. There are four shorter (2.39 Å) and four longer (2.44 Å) Y–O bond lengths. There are two inequivalent Cu+2.25+ sites. In the first Cu+2.25+ site, Cu+2.25+ is bonded to five O2- atoms to form CuO5 square pyramids that share corners with four equivalent CuO5 square pyramids and a cornercorner with one GaO4 tetrahedra. There are a spread of Cu–O bond distances ranging from 1.93–2.41 Å. In the second Cu+2.25+ site, Cu+2.25+ is bonded to five O2- atoms to form CuO5 square pyramids that share corners with four equivalent CuO5 square pyramids and a cornercorner with one GaO4 tetrahedra. There are a spread of Cu–O bond distances ranging from 1.93–2.40 Å. Ga3+ is bonded to four O2- atoms to form GaO4 tetrahedra that share corners with two CuO5 square pyramids and corners with two equivalent GaO4 tetrahedra. There are a spread of Ga–O bond distances ranging from 1.85–1.92 Å. There are seven inequivalent O2- sites. In the first O2- site, O2- is bonded in a 1-coordinate geometry to four Sr2+, one Cu+2.25+, and one Ga3+ atom. In the second O2- site, O2- is bonded to two Sr2+, one Ca2+, one Y3+, and two Cu+2.25+ atoms to form distorted OSr2CaYCu2 octahedra that share corners with two equivalent OSr2CaYCu2 octahedra and corners with two equivalent OSr2Ga2 tetrahedra. The corner-sharing octahedra tilt angles range from 65–67°. In the third O2- site, O2- is bonded in a 6-coordinate geometry to two Sr2+, one Ca2+, one Y3+, and two Cu+2.25+ atoms. In the fourth O2- site, O2- is bonded to two Sr2+ and two equivalent Ga3+ atoms to form distorted OSr2Ga2 tetrahedra that share corners with two equivalent OSr2CaYCu2 octahedra and corners with two equivalent OSr2Ga2 tetrahedra. The corner-sharing octahedra tilt angles range from 53–66°. In the fifth O2- site, O2- is bonded in a 6-coordinate geometry to two Sr2+, one Ca2+, one Y3+, and two Cu+2.25+ atoms. In the sixth O2- site, O2- is bonded in a 6-coordinate geometry to two Sr2+, one Ca2+, one Y3+, and two Cu+2.25+ atoms. In the seventh O2- site, O2- is bonded in a 1-coordinate geometry to four Sr2+, one Cu+2.25+, and one Ga3+ atom.
DOI: 10.17632/zpfm55nr33.2
title: Scales and scalarity: processing scalar inferences

description: This repository contains the data files that are reported in the manuscript "Scales and scalarity: processing scalar inferences".
DOI: 10.17188/1683899
title: Materials Data on NaCrCSO7 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: 10.17188/1683900
title: Materials Data on H4S(NO)2 by Materials Project

description: (NH4)2H4S3(N2O3)2 crystallizes in the monoclinic P2_1/c space group. The structure is zero-dimensional and consists of eight ammonium molecules and four H4S3(N2O3)2 clusters. In each H4S3(N2O3)2 cluster, there are four inequivalent N1+ sites. In the first N1+ site, N1+ is bonded in a distorted bent 120 degrees geometry to two S2- atoms. Both N–S bond lengths are 1.64 Å. In the second N1+ site, N1+ is bonded in a bent 120 degrees geometry to two S2- atoms. There is one shorter (1.59 Å) and one longer (1.63 Å) N–S bond length. In the third N1+ site, N1+ is bonded in a tetrahedral geometry to four H1+ atoms. There are a spread of N–H bond distances ranging from 1.02–1.05 Å. In the fourth N1+ site, N1+ is bonded in a bent 120 degrees geometry to two S2- atoms. There is one shorter (1.58 Å) and one longer (1.63 Å) N–S bond length. There are four inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a single-bond geometry to one N1+ and one O2- atom. The H–O bond length is 1.71 Å. In the second H1+ site, H1+ is bonded in a single-bond geometry to one N1+ atom. In the third H1+ site, H1+ is bonded in a single-bond geometry to one N1+ atom. In the fourth H1+ site, H1+ is bonded in a single-bond geometry to one N1+ atom. There are three inequivalent S2- sites. In the first S2- site, S2- is bonded to two N1+ and two O2- atoms to form corner-sharing SN2O2 tetrahedra. Both S–O bond lengths are 1.46 Å. In the second S2- site, S2- is bonded to two N1+ and two O2- atoms to form corner-sharing SN2O2 tetrahedra. There is one shorter (1.47 Å) and one longer (1.49 Å) S–O bond length. In the third S2- site, S2- is bonded to two N1+ and two O2- atoms to form corner-sharing SN2O2 tetrahedra. There is one shorter (1.46 Å) and one longer (1.48 Å) S–O bond length. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a single-bond geometry to one S2- atom. In the second O2- site, O2- is bonded in a single-bond geometry to one S2- atom. In the third O2- site, O2- is bonded in a single-bond geometry to one S2- atom. In the fourth O2- site, O2- is bonded in a single-bond geometry to one S2- atom. In the fifth O2- site, O2- is bonded in a single-bond geometry to one S2- atom. In the sixth O2- site, O2- is bonded in a distorted single-bond geometry to one H1+ and one S2- atom.
DOI: 10.17188/1683901
title: Materials Data on CsVN2 by Materials Project

description: CsVN2 crystallizes in the cubic Fd-3m space group. The structure is three-dimensional. Cs1+ is bonded in a 12-coordinate geometry to twelve equivalent N3- atoms. All Cs–N bond lengths are 3.48 Å. V5+ is bonded to four equivalent N3- atoms to form corner-sharing VN4 tetrahedra. All V–N bond lengths are 1.82 Å. N3- is bonded in a linear geometry to six equivalent Cs1+ and two equivalent V5+ atoms.
DOI: 10.17188/1683902
title: Materials Data on YbYAl4 by Materials Project

description: YbYAl4 is Hexagonal Laves-derived structured and crystallizes in the cubic F-43m space group. The structure is three-dimensional. Yb is bonded in a 12-coordinate geometry to four equivalent Y and twelve equivalent Al atoms. All Yb–Y bond lengths are 3.43 Å. All Yb–Al bond lengths are 3.28 Å. Y is bonded in a 12-coordinate geometry to four equivalent Yb and twelve equivalent Al atoms. All Y–Al bond lengths are 3.28 Å. Al is bonded to three equivalent Yb, three equivalent Y, and six equivalent Al atoms to form a mixture of edge, corner, and face-sharing AlYb3Y3Al6 cuboctahedra. All Al–Al bond lengths are 2.80 Å.