cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.34808/5fm2-1g82
title: Nonlinear impedance of 35Bi2VO5.5-65SrB4O7 fully crystallized glass measured with impedance spectroscopy method at high temperature region

description: The nonlinear electrcial properties of 35Bi2VO5.5-65SrB4O7 fully crystallized glass was measured by impedance spectroscopy method. 
In order to prepare glasses two compounds: Bi2VO5.5 and SrB4O7 were synthesized via a solid state reaction route. The Bi2VO5.5 was synthesized from the stoichiometric mixture of initial powders of Bi2O3 and V2O5 which were ball-milled in pure acetone for 6 h at room temperature. The milling was performed in steps of 1 h with rest intervals of 10min. The mixture was heated up to 1020K in air and kept at this temperature for 24 h. The heating and cooling rate was of 50K h-1. The obtained powder was checked by X-ray diffraction method. The SrB4O7 was synthesized from the stoichiometric mixture of analytical grade SrCO3 and H3BO3 which were mashed in a mortar. Next the mixture was heated up to 1073K and kept at this temperature for 12 h. Samples of a composition of 35Bi2VO5.5–65SrB4O7 (in mol%) were prepared by the conventional melt quenching technique. The melting was conducted in alumina crucibles at 1373K for 2 h. The melts were poured onto a preheated (573 K) brass plate and pressed by another plate to obtain flat circular disks of 1–2mm thickness and 20–30mm diameter. Glass was heat treated at 813 K to obtain glass-ceramic.
For the electrical measurements gold electrodes were evaporated at the preheated samples. Impedance measurements were carried out in the temperature range from 373 K to 813 K, with the ac voltage of 1 Vrms with Concept 40 broadband dielectric spectrometer. The higher harmonic components (harmonic 0, harmonic 1 and 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/rgff-1f36
title: Nonlinear impedance of 40Bi2VO5.5-60SrB4O7 annealed glass at 593 K measured with impedance spectroscopy method at high temperature region

description: The nonlinear electrical properties of 40Bi2VO5.5-60SrB4O7 glass annealed at 593 K was measured by impedance spectroscopy method. 
In order to prepare glasses two compounds: Bi2VO5.5 and SrB4O7 were synthesized via a solid state reaction route. The Bi2VO5.5 was synthesized from the stoichiometric mixture of initial powders of Bi2O3 and V2O5 which were ball-milled in pure acetone for 6 h at room temperature. The milling was performed in steps of 1 h with rest intervals of 10min. The mixture was heated up to 1020K in air and kept at this temperature for 24 h. The heating and cooling rate was of 50K h-1. The obtained powder was checked by X-ray diffraction method. The SrB4O7 was synthesized from the stoichiometric mixture of analytical grade SrCO3 and H3BO3 which were mashed in a mortar. Next the mixture was heated up to 1073K and kept at this temperature for 12 h. Samples of a composition of 40Bi2VO5.5–60SrB4O7 (in mol%) were prepared by the conventional melt quenching technique. The melting was conducted in alumina crucibles at 1373K for few min. The melts were poured onto a preheated (573 K) brass plate and pressed by another plate to obtain flat circular disks of 1–2mm thickness and 20–30mm diameter. Glasses were annealed at 593 K.
For the electrical measurements gold electrodes were evaporated at the preheated samples. Impedance measurements were carried out in the temperature range from 373 K to 813 K, with the ac voltage of 1 Vrms with Concept 40 broadband dielectric spectrometer. The higher harmonic components (harmonic 0, harmonic 1 and 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: 10.6084/m9.figshare.14974737
title: Opossum_Density_Data_Revised.zip

description: Includes relevant datasets for <i>Journal of Wildlife Management</i> manuscript "Influence of landscape on Virginia opossum density".
DOI: 10.6084/m9.figshare.14974737.v1
title: Opossum_Density_Data_Revised.zip

description: Includes relevant datasets for <i>Journal of Wildlife Management</i> manuscript "Influence of landscape on Virginia opossum density".
DOI: 10.34808/ca2j-4a66
title: Nonlinear impedance of glass 40Bi2VO5.5-60SrB4O7 annealed at 593 K and next fully crystallized was measured with impedance spectroscopy method at high temperature region

description: The nonlinear electrcial properties of glass 40Bi2VO5.5-60SrB4O7 annealed at 593 K and next fully crystallized was measured by impedance spectroscopy method. 
In order to prepare glasses two compounds: Bi2VO5.5 and SrB4O7 were synthesized via a solid state reaction route. The Bi2VO5.5 was synthesized from the stoichiometric mixture of initial powders of Bi2O3 and V2O5 which were ball-milled in pure acetone for 6 h at room temperature. The milling was performed in steps of 1 h with rest intervals of 10min. The mixture was heated up to 1020K in air and kept at this temperature for 24 h. The heating and cooling rate was of 50K h-1. The obtained powder was checked by X-ray diffraction method. The SrB4O7 was synthesized from the stoichiometric mixture of analytical grade SrCO3 and H3BO3 which were mashed in a mortar. Next the mixture was heated up to 1073K and kept at this temperature for 12 h. Samples of a composition of 40Bi2VO5.5–60SrB4O7 (in mol%) were prepared by the conventional melt quenching technique. The melting was conducted in alumina crucibles at 1373K for few min. The melts were poured onto a preheated (573 K) brass plate and pressed by another plate to obtain flat circular disks of 1–2mm thickness and 20–30mm diameter. Glass was annealed at 593 K and next heat treated at 813 K to obtain glass-ceramic.
For the electrical measurements gold electrodes were evaporated at the preheated samples. Impedance measurements were carried out in the temperature range from 373 K to 813 K, with the ac voltage of 1 Vrms with Concept 40 broadband dielectric spectrometer. The higher harmonic components (harmonic 0, harmonic 1 and 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: 10.34808/46zr-bh88
title: Tax rates for the payroll and profit tax for financial institutions Israel 2002-2015

description: The following dataset presents the historical tax rates for the payroll and profit tax paid by financial institutions (non-VAT taxation) in Israel.  The data presented in the dataset concerns 2002-2015.
DOI: 10.34808/czjp-9618
title: Corporate tax rates (2000-2019) - Greece

description: Over the past twenty years, Greece has changed the statutory corporate tax rate, which in 2000 was 40%. The 2008 tax reform provided for a gradual reduction of the rate by 1% annually over the period 2010-2014 (from 25% to 20%). This dataset contains data on CIT rates in Greece.
DOI: 10.34808/h781-er92
title: Corporate income tax in Mexico (1981-1986)

description: The following dataset contains information about Mexican corporate income tax. The presented data concerns the years 1981-1986.
DOI: 10.34808/k1st-mv84
title: IRAP tax differentiation in Italian Regions

description: The following table presents the widespread differentiation in the standard IRAP rates applied in the particular regions of Italy. The tax rates in the table have been updated to 2019 (Only Regions marked with "*" updated their tax rates to the 2020 tax period as of March 16, 2020).
In addition, the Italian tax system provides a set of IRAP flat-rate deductions for dependent workers with an open-ended contract, dependent workers in disadvantaged regions and smaller taxpayers.
DOI: 10.34808/a276-gh75
title: Structure of the SME sector by economy sectors in Poland and the EU-28

description: Eurostat data show that almost 75% of SMEs in Poland are trade and services, and every seventh enterprise conducts activities related to construction, and every eight - in industry. Comparing the industry structure of Polish companies with the structure of enterprises operating in EU countries, it should be noted that we are characterized by a greater number of commercial companies and a smaller number of service companies.
DOI: 10.34808/s8rx-s607
title: Implied Tax Subsidy Rates for Research and Development Expenditure in European OECD Countries (2019)

description: The implied rate of tax credits, developed by the OECD, is one way to measure the extent of R&D tax credits based on spending in different countries. Tax credit rates are measured as the difference between one R&D investment unit and the pre-tax income required to earn commission from that investment unit, assuming the firm is representative. In other words, it measures the scope for preferential treatment of R&D in a given tax system. The more generous the tax rules on R&D, the higher the implied subsidy rates for R&D. The alleged subsidy rate of zero means that R&D is not eligible for preferential tax treatment.
DOI: 10.34808/zk6q-n053
title: Income tax rates for special activities in Czech Republic

description: The standard corporate income tax rate is 19%. Since 2015, the tax rates for special activities have changed as follows: the tax rate for pension funds is 0% (with some exemption); The tax regulations define a new so-called "Basic investment fund" and only that particular fund can benefit from the lower tax rate of 5%. Other mutual funds that do not meet the conditions for core mutual funds are subject to the standard 19% income tax rate.
DOI: 10.5517/ccpxtky
title: CCDC 653311: Experimental Crystal Structure Determination

description: Related Article: S.Gomez Torres|2007|Thesis|||
DOI: 10.5517/ccpxtv7
title: CCDC 653320: Experimental Crystal Structure Determination

description: Related Article: S.Gomez Torres|2007|Thesis|||
DOI: 10.5517/ccrg6gv
title: CCDC 698847: Experimental Crystal Structure Determination

description: Related Article: P.G.Jones|2008|CSD Communication|||
DOI: 10.5517/ccrg6hw
title: CCDC 698848: Experimental Crystal Structure Determination

description: Related Article: P.G.Jones|2008|CSD Communication|||
DOI: 10.5517/ccdc.csd.cc1pg79p
title: CCDC 1562812: Experimental Crystal Structure Determination

description: Related Article: Sagnik K. Roymuhury, Mrinmay Mandal, Debashis Chakraborty, Venkatachalam Ramkumar|2021|Polym.Chem.|12|3953|doi:10.1039/D1PY00237F
DOI: 10.5517/ccdc.csd.cc1pg7ft
title: CCDC 1562816: Experimental Crystal Structure Determination

description: Related Article: Sagnik K. Roymuhury, Mrinmay Mandal, Debashis Chakraborty, Venkatachalam Ramkumar|2021|Polym.Chem.|12|3953|doi:10.1039/D1PY00237F
DOI: 10.5517/ccdc.csd.cc1pg7gv
title: CCDC 1562817: Experimental Crystal Structure Determination

description: Related Article: Sagnik K. Roymuhury, Mrinmay Mandal, Debashis Chakraborty, Venkatachalam Ramkumar|2021|Polym.Chem.|12|3953|doi:10.1039/D1PY00237F
DOI: 10.5517/ccdc.csd.cc1pg7hw
title: CCDC 1562818: Experimental Crystal Structure Determination

description: Related Article: Sagnik K. Roymuhury, Mrinmay Mandal, Debashis Chakraborty, Venkatachalam Ramkumar|2021|Polym.Chem.|12|3953|doi:10.1039/D1PY00237F
DOI: 10.5517/ccdc.csd.cc1pg7jx
title: CCDC 1562819: Experimental Crystal Structure Determination

description: Related Article: Sagnik K. Roymuhury, Mrinmay Mandal, Debashis Chakraborty, Venkatachalam Ramkumar|2021|Polym.Chem.|12|3953|doi:10.1039/D1PY00237F
DOI: 10.5517/ccdc.csd.cc24lrp6
title: CCDC 1984238: Experimental Crystal Structure Determination

description: Related Article: Huan Xue, Xin-Song Huang, Qi Yin, Xiao-Jing Hu, He-Qi Zheng, Ge Huang, Tian-Fu Liu|2020|Cryst.Growth Des.|20|4861|doi:10.1021/acs.cgd.0c00239
DOI: 10.5517/ccdc.csd.cc24lrq7
title: CCDC 1984239: Experimental Crystal Structure Determination

description: Related Article: Huan Xue, Xin-Song Huang, Qi Yin, Xiao-Jing Hu, He-Qi Zheng, Ge Huang, Tian-Fu Liu|2020|Cryst.Growth Des.|20|4861|doi:10.1021/acs.cgd.0c00239
DOI: 10.5517/ccdc.csd.cc259mmr
title: CCDC 2005254: Experimental Crystal Structure Determination

description: Related Article: Vladimir P. Fedin, Anna A. Lysova, Denis G. Samsonenko, Konstantin A. Kovalenko, Danil N. Dybtsev, Anton S. Nizovtsev|2020|Angew.Chem.,Int.Ed.|59|20561|doi:10.1002/anie.202008132
DOI: 10.5517/ccdc.csd.cc259mns
title: CCDC 2005255: Experimental Crystal Structure Determination

description: Related Article: Vladimir P. Fedin, Anna A. Lysova, Denis G. Samsonenko, Konstantin A. Kovalenko, Danil N. Dybtsev, Anton S. Nizovtsev|2020|Angew.Chem.,Int.Ed.|59|20561|doi:10.1002/anie.202008132
DOI: 10.5517/ccdc.csd.cc259mpt
title: CCDC 2005256: Experimental Crystal Structure Determination

description: Related Article: Vladimir P. Fedin, Anna A. Lysova, Denis G. Samsonenko, Konstantin A. Kovalenko, Danil N. Dybtsev, Anton S. Nizovtsev|2020|Angew.Chem.,Int.Ed.|59|20561|doi:10.1002/anie.202008132
DOI: 10.5517/ccdc.csd.cc259mqv
title: CCDC 2005257: Experimental Crystal Structure Determination

description: Related Article: Vladimir P. Fedin, Anna A. Lysova, Denis G. Samsonenko, Konstantin A. Kovalenko, Danil N. Dybtsev, Anton S. Nizovtsev|2020|Angew.Chem.,Int.Ed.|59|20561|doi:10.1002/anie.202008132
DOI: 10.5517/ccdc.csd.cc259mrw
title: CCDC 2005258: Experimental Crystal Structure Determination

description: Related Article: Vladimir P. Fedin, Anna A. Lysova, Denis G. Samsonenko, Konstantin A. Kovalenko, Danil N. Dybtsev, Anton S. Nizovtsev|2020|Angew.Chem.,Int.Ed.|59|20561|doi:10.1002/anie.202008132
DOI: 10.5517/ccdc.csd.cc259w9p
title: CCDC 2005492: Experimental Crystal Structure Determination

description: Related Article: Stephan K. Pedersen, Kristina Eriksen, Hans Ågren, Boris F. Minaev, Nataliya N. Karaush-Karmazin, Ole Hammerich, Glib V. Baryshnikov, Michael Pittelkow|2020|J.Am.Chem.Soc.|142|14058|doi:10.1021/jacs.0c05898
DOI: 10.5517/ccdc.csd.cc24zqzv
title: CCDC 1995748: Experimental Crystal Structure Determination

description: Related Article: Anton A. Ivanov, Clément Falaise, Alexandra A. Shmakova, Nathalie Leclerc, Stéphane Cordier, Yann Molard, Yuri V. Mironov, Michael A. Shestopalov, Pavel A. Abramov, Maxim N. Sokolov, Mohamed Haouas, Emmanuel Cadot|2020|Inorg.Chem.|59|11396|doi:10.1021/acs.inorgchem.0c01160
DOI: 10.5517/ccdc.csd.cc24zr0x
title: CCDC 1995749: Experimental Crystal Structure Determination

description: Related Article: Anton A. Ivanov, Clément Falaise, Alexandra A. Shmakova, Nathalie Leclerc, Stéphane Cordier, Yann Molard, Yuri V. Mironov, Michael A. Shestopalov, Pavel A. Abramov, Maxim N. Sokolov, Mohamed Haouas, Emmanuel Cadot|2020|Inorg.Chem.|59|11396|doi:10.1021/acs.inorgchem.0c01160
DOI: 10.5517/ccdc.csd.cc266ty6
title: CCDC 2032358: Experimental Crystal Structure Determination

description: Related Article: Alexey Gusev, Mikhail Kiskin, Irina Lutsenko, Roman Svetogorov, Sergey Veber, Olga Minakova, Vladislav Korshunov, Ilya Taydakov, Wolfgang Linert|2021|J.Lumin.|238|118305|doi:10.1016/j.jlumin.2021.118305
DOI: 10.5517/ccdc.csd.cc266tz7
title: CCDC 2032359: Experimental Crystal Structure Determination

description: Related Article: Alexey Gusev, Mikhail Kiskin, Irina Lutsenko, Roman Svetogorov, Sergey Veber, Olga Minakova, Vladislav Korshunov, Ilya Taydakov, Wolfgang Linert|2021|J.Lumin.|238|118305|doi:10.1016/j.jlumin.2021.118305
DOI: 10.5517/ccdc.csd.cc261pyx
title: CCDC 2027429: Experimental Crystal Structure Determination

description: Related Article: Neal Hickey, Barbara Medagli, Alessandro Pedrini, Roberta Pinalli, Enrico Dalcanale, Silvano Geremia|2021|Cryst.Growth Des.|21|3650|doi:10.1021/acs.cgd.1c00463
DOI: 10.15128/r2pk02c9794
title: Sulphur constraints on the carbon cycle of a blanket bog peatland [dataset]

description: Data for JGR Biogeosciences manuscript
description: The reduction of sulphate (SO42-) represents an alternative terminal electron acceptor for the oxidation of organic matter in peat soils. The greenhouse gas budget in peatlands will be constrained by how much a peatland can utilise SO42- reduction as an alternative to methanogenesis. Using records of atmospheric deposition and stream chemistry coupled with elemental analysis of peat soil, vegetation, particulate organic matter (POM) and dissolved organic matter (DOM), this study estimated a 23-year long sulphur (S) budget for a blanket bog-covered catchment in the North Pennines, England. The study showed that: 1) Atmospheric deposition of total S significantly declined over the study period from 2.4 to 0.5 t S/km2/yr. 2) Long term accumulation of S into deep peat at 1 m depth averaged 127 kg S/km2/yr. 3) Total S fluvial flux peaked as 4.5 t S/km2/yr with an average of 0.7 t S/km2/yr. 4) On average, over 23 years, 0.25 t S/km2/yr were reduced to either mineral sulphides or hydrogen sulphide; however, in 8 out of the 23 years the catchment was a net producer of S to the streams of the catchment. At maximum observed S reduction capacity the peatland was capable of a net removal of 71% of atmospheric S deposition. Allowing for the efficiency of energy transfer in the redox process and the oxidation state of peat organic matter means that for every mole of SO42- reduced, 1.69 moles of CO2 were produced and an average of 0.47 t C/km2/yr are diverted from methanogenesis.
description: See manuscript
DOI: 10.6084/m9.figshare.14974698.v1
title: Table S2. A thermal event in the Dolpo region (Nepal): a consequence of the shifting from orogen perpendicular to orogen parallel extension in central Himalaya?

description: Table S2. <sup>40</sup>Ar/<sup>39</sup>Ar in-situ and step-heating data. Data are relative abundances, corrected for post-irradiation decay, mass discrimination effects and line blank.
DOI: 10.6084/m9.figshare.14974695.v1
title: Table S1. A thermal event in the Dolpo region (Nepal): a consequence of the shifting from orogen perpendicular to orogen parallel extension in central Himalaya?

description: Table S1. Electron microprobe analyses of dark mica and white mica (wt% oxides) and atoms per formula unit (a.p.f.u.) recalculated based on 11 oxygens.
DOI: 10.6084/m9.figshare.14974632.v1
title: TESE.sav

description: In the sport of artistic roller skating the athletes use shoes fitted with small wheels to use in rinks and consists of seven disciplines characterized by different physical demands. Roller skaters are judged on content and manner of performance, and this includes the skater’s ability to do jumps, spins, and footwork. The purpose of this study was to compare the body composition, flexibility, balance, reactive strength, maximum strength, and aerobic capacity based on skating discipline and skating level. A total of 108 female athletes from the three individual disciplines (figures, freestyle, and solo dance) and three different levels (elite, sub-elite, and non-elite) volunteered to participate in this study. Findings showed that freestyle skaters have less body fat, and higher levels of reactive and maximum strength than figures and solo dance skaters. Elite skaters demonstrate greater values of flexibility, balance, strength, and aerobic capacity compared to their sub-elite and non-elite counterparts. The results of this study showed that there are differences between elite and non-elite athletes and between skating disciplines. Strength and conditioning professionals should have that into consideration when training these athletes.
DOI: 10.6084/m9.figshare.14974698
title: Table S2. A thermal event in the Dolpo region (Nepal): a consequence of the shifting from orogen perpendicular to orogen parallel extension in central Himalaya?

description: Table S2. <sup>40</sup>Ar/<sup>39</sup>Ar in-situ and step-heating data. Data are relative abundances, corrected for post-irradiation decay, mass discrimination effects and line blank.
DOI: 10.6084/m9.figshare.14974695
title: Table S1. A thermal event in the Dolpo region (Nepal): a consequence of the shifting from orogen perpendicular to orogen parallel extension in central Himalaya?

description: Table S1. Electron microprobe analyses of dark mica and white mica (wt% oxides) and atoms per formula unit (a.p.f.u.) recalculated based on 11 oxygens.
DOI: 10.6084/m9.figshare.14974632
title: TESE.sav

description: In the sport of artistic roller skating the athletes use shoes fitted with small wheels to use in rinks and consists of seven disciplines characterized by different physical demands. Roller skaters are judged on content and manner of performance, and this includes the skater’s ability to do jumps, spins, and footwork. The purpose of this study was to compare the body composition, flexibility, balance, reactive strength, maximum strength, and aerobic capacity based on skating discipline and skating level. A total of 108 female athletes from the three individual disciplines (figures, freestyle, and solo dance) and three different levels (elite, sub-elite, and non-elite) volunteered to participate in this study. Findings showed that freestyle skaters have less body fat, and higher levels of reactive and maximum strength than figures and solo dance skaters. Elite skaters demonstrate greater values of flexibility, balance, strength, and aerobic capacity compared to their sub-elite and non-elite counterparts. The results of this study showed that there are differences between elite and non-elite athletes and between skating disciplines. Strength and conditioning professionals should have that into consideration when training these athletes.
DOI: 10.5281/zenodo.5095219
title: Data for thesis: Online Discovery and Model-to-Model Comparison of DCR Models from Event Streams

description: This is the collection of data referenced in the Thesis
DOI: 10.5281/zenodo.5095218
title: Data for thesis: Online Discovery and Model-to-Model Comparison of DCR Models from Event Streams

description: This is the collection of data referenced in the Thesis
DOI: 10.25345/c5w24s
title: MassIVE MSV000087806 - GNPS GC/MS analysis of various compounds for library search 13
title: GC/MS analysis of various compounds for library search 13 RIGHT_SSL_EI_WO_sleep_10dg_min_35-290_as_needle_split50