cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.6084/m9.figshare.14987379.v1
title: Supplementary Material for: Association between Latent Trajectories of Fluid Balance and Clinical Outcomes in Critically Ill Patients with Acute Kidney Injury: A Prospective Multicenter Observational Study

description: <b><i>Introduction:</i></b> We aimed to identify different trajectories of fluid balance (FB) and investigate the effect of FB trajectories on clinical outcomes in intensive care unit (ICU) patients with acute kidney injury (AKI) and the dose-response association between fluid overload (FO) and mortality. <b><i>Methods:</i></b> We derived data from the Beijing Acute Kidney Injury Trial (BAKIT). A total of 1,529 critically ill patients with AKI were included. The primary outcome was 28-day mortality, and hospital mortality, ICU mortality and AKI stage were the secondary outcomes. A group-based trajectory model was used to identify the trajectory of FB during the first 7 days. Multivariable logistic regression was performed to examine the relationship between FB trajectories and clinical outcomes. A logistic regression model with restricted cubic splines was used to examine the dose relationship between FO and 28-day mortality. <b><i>Results:</i></b> Three distinct trajectories of FB were identified: low FB (1,316, 86.1%), decreasing FB (120, 7.8%), and high FB (93, 6.1%). Compared with low FB, high FB was associated with increased 28-day mortality (odds ratio [OR] 1.94, 95% confidence interval [CI] 1.17–3.19) and AKI stage (OR 2.04, 95% CI 1.23–3.37), whereas decreasing FB was associated with a reduction in 28-day mortality by approximately half (OR 0.53, 95% CI 0.32–0.87). Similar results were found for the outcomes of ICU mortality and hospital mortality. We observed a J-shaped relationship between maximum FO and 28-day mortality, with the lowest risk at a maximum FO of 2.8% L/kg. <b><i>Conclusion:</i></b> Different trajectories of FB in critically ill patients with AKI were associated with clinical outcomes. An FB above or below a certain range was associated with an increased risk of mortality. Further studies should explore this relationship and search for the optimal fluid management strategies for critically ill patients with AKI.
DOI: 10.25345/c51n8d
title: MassIVE MSV000087828 - Caracterisation chimique du houblon de Corse
title: Samples: MeOH extracts of Corsican Humulus lupulus cones. 2021.
DOI: 10.5281/zenodo.5101077
title: Data files for 'From Cooper pair splitting to the non-local spectroscopy of a Shiba state'

description: Data files for 'From Cooper pair splitting to the non-local spectroscopy of a Shiba state'
DOI: 10.5285/bbaf922a-e46e-7e94-e053-6c86abc0089a
title: Physical and modelled interactions between coral growth and water hydrodynamics using <em>Lophelia pertusa</em> as a model organism.

description: This dataset contains data regarding how branching cold-water corals (<em>Lophelia pertusa</em>) modify flow velocity. The data are generated in two ways; through Particle Imaging Velocimetry (PIV) on <em>Lophelia pertusa</em> nubbins, and through modelled simulations of how growing <em>L. pertusa</em> will impact resultant flow around them. Coral colonies for experimental PIV analysis in flumes were collected at 107 metres depth from the Central Tisler Reef in 2014. Flow patterns in the areas behind <em>L. pertusa</em> colonies and around coral nubbins were studied at a range of average free stream velocities using PIV to match a variety of field ranges. Velocity values representing water speeds at locations on coral nubbins as well as images from PIV as resulting vectors and streamline vectors under a variety of scenarios are all included in this dataset. This work was done between March and October 2014. For the modelling data, a Smoothed Particle Hydrodynamics (SPH) model was created to simulate coral growth with simple rules, that coral would 'grow' where flow velocity was optimal for feeding. A fully Lagrangian numerical SPH approach was employed to model and capture the dynamic and complex hydrodynamic fluid-solid interactions of coral growth. The model code and images generated by the code were produced between August 2016 and January 2021 and are included in this dataset. The generation of these data were funded by NERC grants NE/K009028/1, NE/K009028/2, NE/L002558/1, NE/H010025, European Commission ASSEMBLE Project (Grant Agreement No. 227799), Royal Society of Edinburgh 48701/1, FORMAS Grant No. 215-2012-1134, EU Horizon 2020 Research and Innovation Program Grant Agreement No. 678760 and No. 818123, and UKRI GCRF One Ocean Hub NE/S008950/1.
DOI: 10.11571/upei-roblib-data/researchdata:679
title: DAIRY PRODUCER SATISFACTION AND KNOWLEDGE TRANSFER WITH THE VETERINARY-ADMINISTERED RISK ASSESSMENT AND MANAGEMENT PLAN IN A VOLUNTARY JOHNE’S DISEASE CONTROL PROGRAM - SUPPLEMENTAL FILE
DOI: 10.34740/kaggle/dsv/2427960
title: YouTube Trending Video Dataset (updated daily)
DOI: 10.34808/qm00-z683
title: Reduction of the strontium titanate doped by Ytrium ceramics observed by X-ray photoemission spectroscopy method

description: 


Ytrium-doped strontium titanate (YSTF) ceramics materials were manufactured by three various methods: 1) standard solid-state reaction method from Y2O3 (Sigma Aldrich, 99,9%), TiO2 (Sigma Aldrich, 99%) and SrCO3 (Sigma Aldrich,98%), 2) Pechini method, 3) wet method.
Both kind of samples were measured, after and before reduction process (in a hydrogen). Reduction of samples carried out at 750 Celsius degree. To observe results of the reduction process, valence states of elements of manufactured samples was measured by XPS method. The Analyses were carried out with X-ray photoelectron spectrometer (Omicron NanoTechnology) with 128-channel collector. XPS measurements were performed at room temperature in a ultra-high vacuum conditions, below 1.1 x10-8 mBar. The photoelectrons were excited by an Mg-Ka X-Ray source. The X-ray anode was operated at 15 keV and 300 W. Omicron Argus hemispherical electron analyser with round aperture of 4 mm was used for analysing of emitted photoelectrons. The binding energies were corrected using the background C1s line (285.0 eV). XPS spectra were analysed with Casa-XPS software using a Shirley background subtraction and Gaussian–Lorentzian curve as a fitting algorithm.
DOI: 10.34808/7crn-wp11
title: Chemical composition of La-Sr-Ce-Ni-Ti ceramics material measured by XPS method

description: La-Sr-Ce-Ni-Ti (LSCNT) based ceramics sample was manufactured by standard solid state reaction.Prepared powder was pressed into pilled and sintered in a furnace in air atmosphere for 10h. Annealing temperature was 1200 Celsius degree. To calculate chemical composition and determine valence states of the elements, X-Ray photoemission spectroscopy (XPS) analysis were performed. Measurements were conducted at room temperature under a pressure below 1.1 × 10−9 mBar. The photoelectrons were excited by an Mg-Kα X-Ray anode operated at 15 keV and 300 W. Omicron Argus hemispherical electron analyser with a round aperture of 4 mm was used for the analysis of energy of the emitted photoelectrons. Th high resolution scans were performed for each element (La3d, Ni2p, Ti2p, Sr3d and Ce3d).
DOI: 10.34808/as4r-1t33
title: Valence state of Manganium in a MnCoO ceramics

description: Manganium -cobalt based ceramics materials were produced by solid state reaction and sintred in a furnance in air atmosphere for 20h. Annealing temperature was 600 Celsius degree. For investigations a series of samples, with a various composition was chosen: MnCoO, Mn, Co2O and Mn2CoO. In order to determine valence states of the Mn, X-Ray photoemission spectroscopy (XPS) analysis were performed at room temperature under a pressure below 1.1 × 10−9 mBar. The photoelectrons were excited by an Mg-Kα X-Ray anode operated at 15 keV and 300 W. Omicron Argus hemispherical electron analyser with a round aperture of 4 mm was used for the analysis of emitted photoelectrons. Measurements were carried out in a constant analyser energy (CAE) mode with pass energy equal 50 eV. To remove contaminations and oxides, the surface was etched before the measurement. Argon ion gun with energy up to 5 keV was used for 5 min. etching. Two regions were measured: Mn2p and Mn3s. Measurements shoved domination of Mn3+ in a materials.
DOI: 10.34808/qm6g-cp76
title: Investigations of the valence state of Co in a MnCoO ceramics

description: McCoO ceramics materials were produced by solid state reaction and sintred in a furnance in air atmosphere for 20h. Annealing temperature was 600 Celsius degree. For investigations a series of samples, with a various composition was chosen: MnCoO, Mn, Co2O and Mn2CoO. Chemical behaviour of the Cobaltium was measured by XPS method.  The analyses were carried out with X-ray photoelectron spectrometer (Omicron NanoTechnology) with 128-channel collector. XPS measurements were performed at room temperature in a ultra-high vacuum conditions, below 1.1 x10-8 mBar. The photoelectrons were excited by an Mg-Ka X-Ray source. The X-ray anode was operated at 15 keV and 300 W. Omicron Argus hemispherical electron analyser with round aperture of 4 mm was used for analysing of emitted photoelectrons. The binding energies were corrected using the background C1s line (285.0 eV). XPS spectra were analysed with Casa-XPS software using a Shirley background subtraction and Gaussian–Lorentzian curve as a fitting algorithm. Measurements shoved more or less equal content of Co3+ and Co4+ in each samples.
DOI: 10.17632/tvn32z4rbd.1
title: LINF_150020700

description: mitochondrial DNA topoisomerase II | TOP2 Leishmania infantum (strain JPCM5)
DOI: 10.17632/ckrbcfmmbw.1
title: National Strategic Reference Framework (N.S.R.F.) 2007-2013, Greece Data for R&D projects: Indicators of absorption, evaluation and effectiveness

description: National Strategic Reference Framework (N.S.R.F.) 2007-2013, Greece Data for R&D projects: Indicators of absorption, evaluation and effectiveness Primary Research Data for all R&D projects Public expenditure by R.T.D.I. sector and beneficiary, by Sector and subsector R.T.D.I, by Region and Beneficiary, by Operational Program, by Regional Operational Program, public expenditure by beneficiary Descriptive data of result indicators for the implemented research projects of the programming period 2007-2013
DOI: 10.34808/rjrf-mg17
title: Cytotoxicity of C-2028, QDgreen, QDred, QDgreen-FA, QDred-FA, QDgreen-FA-C-2028 and QDred-FA-C-2028 aginst LNCaP cancer cells

description: This study presents absorbance values of formazan product (converted from MTT) which corresponds the cytotoxicity of C-2028, QDgreen, QDred, QDgreen-FA, QDred-FA, QDgreen-FA-C-2028 and QDred-FA-C-2028 aginst LNCaP cancer cells.  FA (folic acid) was used as a linker between quantum dots (QDs) and compound (C-2028) at different concentration (50-200 µM).
DOI: 10.34808/3nxy-s931
title: Cytotoxicity of C-2028, QDgreen, QDred, QDgreen-FA, QDred-FA, QDgreen-FA-C-2028 and QDred-FA-C-2028 aginst Du-145 cancer cells

description: This study presents absorbance values of formazan product (converted from MTT) which corresponds the cytotoxicity of C-2028, QDgreen, QDred, QDgreen-FA, QDred-FA, QDgreen-FA-C-2028 and QDred-FA-C-2028 aginst H460 cancer cells.  FA (folic acid) was used as a linker between quantum dots (QDs) and compound (C-2028) at different concentration (50-200 µM).
DOI: 10.25919/3gag-mc88
title: Parkes observations for project P1005 semester 2021APRS_06

description: We propose to conduct observations of PSR J1812-15, a 1-s pulsar in a 20.3-hr circular orbit around a light companion which also exhibits variable emission (turning `on’ and `off’). Binary pulsars are valuable objects of scientific study, allowing for a wide range of applications, including tests of gravity, probes of the neutron star equation of state and fossil records of stellar evolution. Long spin-period pulsars in binary systems are generally much rarer than faster-spinning recycled pulsars, and represent an under-explored region of pulsar binary evolution. We propose a two-pronged campaign designed to address individual aspects of PSR J1812-15’s behaviour. Firstly, although we have developed a binary solution as a consequence of previous P1005 observations, we are still unable to develop a phase-connected timing solution, a key step in understanding this pulsar and its binary formation process. We therefore propose a 6-month monitoring campaign intended to provide the additional constraint required to determine a unique solution. Secondly, we have identified a correlation between the pulsar’s detectability and its orbital phase, suggesting that an eclipse or other complex interaction between the pulsar and its binary companion is at least partially responsible for its variable emission. We propose to monitor a series of consecutive orbits so as to fully cover the pulsar’s orbital phase, exploiting the wide bandwidth of the UWL receiver to distinguish between variability due to the binary companion or other sources (e.g. intrinsic pulse nulling).
DOI: 10.34808/2xm8-nc36
title: Nonlinear impedance of Bi2VO5.5 ceramic of thickness 2.52 mm (after second heat-treatment at 913 K) was measured at high temperature range with impedance spectroscopy method

description: The nonlinear electrical properties of Bi2VO5.5 ceramic of thickness 2.52 mm (after second heat-treatment at 913 K) was measured by impedance spectroscopy method. 
The polycrystalline Bi2VO5.5 ceramic was synthesised via a conventional solid state reaction route. The stoichiometric mixture of initial powders of Bi2O3 and V2O5 were ball-milled in pure acetone for 6 h. The milling was performed in steps of 1 h with rest intervals of 10 min. The mixture was initially heated up to 770 K and then to 1020 K in air. It was kept at this temperature for 24 h and grinded next. The calcined powder was mixed with a small amount of ethyl alcohol binder and cold-pressed into pellets (12 mm in diameter and 2–3 mmin thickness) under a compacting pressure of 26 kNcm−2. The obtained pellets were sintered at 1070 K for 24 h with heating and cooling rates of 50 Kh−1. The sample thickness was 2.52 mm. Sample was two times heat-treated at 913 K before electrical measurements.
For the electrical measurements gold electrodes were evaporated at the preheated samples. Impedance measurements were carried out in the temperature range from 473 K to 913 K, frequency range between 10 mHz to 1 MHz, with the ac voltage of 1 Vrms with Concept 40 broadband dielectric spectrometer. The higher harmonic components (harmonic 1 and 2) were measured up to frequency of 1000 Hz. Measurements were conducted during heating and cooling. Here the impedance for harmonic components was defined as the ratio of the voltage base wave to the n-th harmonic current component: Zn∗= U0∗/In∗, where Zn⁎ including the base wave generally depend on the sample voltage U1⁎ base wave amplitude. From Zn⁎ allother independent variables are calculated. The dependence of current density on the cosinusoidal electric field E(t)= E0cos(ωt) leads to the following expression:
j´ = σ´0hE0 cos (ωt) + σ´1hE0 cos (2ωt) + σ´2hE0 cos (3ωt) + …Where σ´0h denotes base conductivity, while σ´1h, σ´2h etc. are higher harmonics conductivity. The admittivity for harmonic components with n ≥1, is calculated from relation σ⁎n = i2πfε0ε⁎n.
DOI: 10.34808/62z9-7r55
title: Nonlinear impedance as a function of A.C. voltage of Bi2VO5.5 ceramic of thickness 2.88 mm was measured at 693 K with impedance spectroscopy method

description: The nonlinear electrical properties of Bi2VO5.5 ceramic of thickness 2.88 mm was measured by impedance spectroscopy method. 
The polycrystalline Bi2VO5.5 ceramic was synthesised via a conventional solid state reaction route. The stoichiometric mixture of initial powders of Bi2O3 and V2O5 were ball-milled in pure acetone for 6 h. The milling was performed in steps of 1 h with rest intervals of 10 min. The mixture was initially heated up to 770 K and then to 1020 K in air. It was kept at this temperature for 24 h and grinded next. The calcined powder was mixed with a small amount of ethyl alcohol binder and cold-pressed into pellets (12 mm in diameter and 2–3 mmin thickness) under a compacting pressure of 26 kNcm−2. The obtained pellets were sintered at 1070 K for 24 h with heating and cooling rates of 50 Kh−1. The sample thickness was 2.88 mm.
For the electrical measurements gold electrodes were evaporated at the preheated samples. Impedance measurements were carried out at temperature of 693 K, frequency range: 0.1, 1, 10 and 100 Hz, with the ac voltage range between 0.01 to 3 Vrms with Concept 40 broadband dielectric spectrometer. The higher harmonic components (harmonic 2) were measured. Measurements were conducted during heating and cooling. Here the impedance for harmonic components was defined as the ratio of the voltage base wave to the n-th harmonic current component: Zn∗= U0∗/In∗, where Zn⁎ including the base wave generally depend on the sample voltage U1⁎ base wave amplitude. From Zn⁎ allother independent variables are calculated. The dependence of current density on the cosinusoidal electric field E(t)= E0cos(ωt) leads to the following expression:
j´ = σ´0hE0 cos (ωt) + σ´1hE0 cos (2ωt) + σ´2hE0 cos (3ωt) + …Where σ´0h denotes base conductivity, while σ´1h, σ´2h etc. are higher harmonics conductivity. The admittivity for harmonic components with n ≥1, is calculated from relation σ⁎n = i2πfε0ε⁎n.
DOI: 10.34808/6w72-cr12
title: Nonlinear impedance as a function of temperature and frequency for Bi2VO5.5 ceramic of thickness 2.52 mm was measured at different A.C. voltage with impedance spectroscopy method

description: The nonlinear electrical properties of Bi2VO5.5 ceramic of thickness 2.52 mm was measured by impedance spectroscopy method. 
The polycrystalline Bi2VO5.5 ceramic was synthesised via a conventional solid state reaction route. The stoichiometric mixture of initial powders of Bi2O3 and V2O5 were ball-milled in pure acetone for 6 h. The milling was performed in steps of 1 h with rest intervals of 10 min. The mixture was initially heated up to 770 K and then to 1020 K in air. It was kept at this temperature for 24 h and grinded next. The calcined powder was mixed with a small amount of ethyl alcohol binder and cold-pressed into pellets (12 mm in diameter and 2–3 mmin thickness) under a compacting pressure of 26 kNcm−2. The obtained pellets were sintered at 1070 K for 24 h with heating and cooling rates of 50 Kh−1. The sample thickness was 2.52 mm.
For the electrical measurements gold electrodes were evaporated at the preheated samples. Impedance measurements were carried out at temperature range from 473 K to 913 K, frequency range from 0.1 Hz to 1 MHz, with the ac voltage: 0.01, 0.1, 1 and 2 Vrms with Concept 40 broadband dielectric spectrometer. The higher harmonic components (harmonic 2) were measured up to frequency of 1000 Hz. Measurements were conducted during heating and cooling. Here the impedance for harmonic components was defined as the ratio of the voltage base wave to the n-th harmonic current component: Zn∗= U0∗/In∗, where Zn⁎ including the base wave generally depend on the sample voltage U1⁎ base wave amplitude. From Zn⁎ allother independent variables are calculated. The dependence of current density on the cosinusoidal electric field E(t)= E0cos(ωt) leads to the following expression:
j´ = σ´0hE0 cos (ωt) + σ´1hE0 cos (2ωt) + σ´2hE0 cos (3ωt) + …Where σ´0h denotes base conductivity, while σ´1h, σ´2h etc. are higher harmonics conductivity. The admittivity for harmonic components with n ≥1, is calculated from relation σ⁎n = i2πfε0ε⁎n.
DOI: 10.34808/2r87-8h97
title: Nonlinear impedance as a function of A.C. voltage and temperature for Bi2VO5.5 ceramic of thickness 2.52 mm (after first heat-treatment at 913 K) was measured at different frequencies with impedance spectroscopy method

description: The nonlinear electrical properties of Bi2VO5.5 ceramic of thickness 2.52 mm was measured by impedance spectroscopy method. 
The polycrystalline Bi2VO5.5 ceramic was synthesised via a conventional solid state reaction route. The stoichiometric mixture of initial powders of Bi2O3 and V2O5 were ball-milled in pure acetone for 6 h. The milling was performed in steps of 1 h with rest intervals of 10 min. The mixture was initially heated up to 770 K and then to 1020 K in air. It was kept at this temperature for 24 h and grinded next. The calcined powder was mixed with a small amount of ethyl alcohol binder and cold-pressed into pellets (12 mm in diameter and 2–3 mmin thickness) under a compacting pressure of 26 kNcm−2. The obtained pellets were sintered at 1070 K for 24 h with heating and cooling rates of 50 Kh−1. The sample thickness was 2.52 mm.
For the electrical measurements gold electrodes were evaporated at the preheated samples. Impedance measurements were carried out at temperature range from 423 K to 813 K, frequency of 0.01, 0.1, 1 and 10 Hz, with the ac voltage range between 0.01 and 3 Vrms with Concept 40 broadband dielectric spectrometer. The higher harmonic components (harmonic 1 and 2) were measured. Measurements were conducted during heating and cooling. Here the impedance for harmonic components was defined as the ratio of the voltage base wave to the n-th harmonic current component: Zn∗= U0∗/In∗, where Zn⁎ including the base wave generally depend on the sample voltage U1⁎ base wave amplitude. From Zn⁎ allother independent variables are calculated. The dependence of current density on the cosinusoidal electric field E(t)= E0cos(ωt) leads to the following expression:
j´ = σ´0hE0 cos (ωt) + σ´1hE0 cos (2ωt) + σ´2hE0 cos (3ωt) + …Where σ´0h denotes base conductivity, while σ´1h, σ´2h etc. are higher harmonics conductivity. The admittivity for harmonic components with n ≥1, is calculated from relation σ⁎n = i2πfε0ε⁎n.
DOI: 10.34808/3jvv-hr22
title: Linear impedance of  25Na2O–20CaO–5P2O5–50SiO2 glass measured with impedance spectroscopy method at low temperature region

description: The linear electrical properties of  25Na2O–20CaO–5P2O5–50SiO2 glass was measured by impedance spectroscopy method. 
The glass 25Na2O–20CaO–5P2O5–50SiO2 (in mol%) was melted from reagents: NaH2PO3 (C 99.5% SIGMAALDRICH), Na2CO3 (99.9 % ChemPur GmbH), CaCO3 (99.9 % ChemPur GmbH) and SiO2 (99.99% ChemPur GmbH). Alumina crucibles were used for melting at temperatures of 1350 degC, under air atmosphere. The melts were quenched onto brass plate. The exact composition of melted samples was studied with the use of SEM-EDS  and was found to be Na18.3Ca6.5P3.6Si16.1O55.5 (in at%).
For the electrical measurements gold electrodes were evaporated at the preheated and grinded samples. Impedance measurements were carried out in the temperature range from 153 K to 423 K, in the frequency range from 10mHz to 1 MHz and with the ac voltage of 1 Vrms with Concept 40 broadband dielectric spectrometer.
DOI: 10.34808/tw5v-kq58
title: Luminescence properties of TeOx-Tb thin films

description: The DataSet contains the emission and excitation spectra of TeOx-Tb thin films. The material was obtained by the sol-gel method.  The starting solution was prepared by mixing telluric acid (precursor) with thetraetylene glycol, water, and ethanol. Next, the 5% mol of terbium ions were added, the nitrates were used as a source of rare-earth ions. The sol was obtained by vigorously stirring precursor solution at 50°C for 2h, then the temperature was raised to 75°C for the next 2h.  Next, the sol was used to prepared thin films by a spin coating method. The corning glass with 8 nm alumina oxide was used as a substrate.  After deposition, the thin films were dried at 200°C under an argon atmosphere.
Luminescence emission and excitation spectra of gel were collected in a Horiba Yvon spectrofluorometer (Fluorolog 3).