cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.34808/a5s5-qe07
title: Nonlinear impedance of  Bi2VO5.5 glass-ceramic annealed at 423 K was measured with impedance spectroscopy method at high temperature region

description: The nonlinear electrical properties of Bi2VO5.5 glass-ceramic annealed at 423 K was measured by impedance spectroscopy method. 
Bi2VO5.5 glas-ceramic was prepared from appropriate amounts of Bi2O3 and V2O5 powders. The melting was conducted in alumina crucibles at 1173 K for few minutes. The melt was poured onto a preheated (573 K) brass plate and pressed by another plate to obtain flat circular disks. Next samples were annealed at 423 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 913 K, frequency range of 10 mHz to 1 MHz, with the ac voltage of 1 Vrms with Concept 40 broadband dielectric spectrometer. The higher harmonic components (harmonic 2) were measured up to frequency of 1000 Hz. 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: 10.34808/13dk-8w23
title: Nonlinear impedance of  Bi2VO5.5 glass-ceramic heat-treated at 913 K was measured with impedance spectroscopy method at high temperature region

description: The nonlinear electrical properties of Bi2VO5.5 glass-ceramic heat-treated at 913 K was measured by impedance spectroscopy method. 
Bi2VO5.5 glas-ceramic was prepared from appropriate amounts of Bi2O3 and V2O5 powders. The melting was conducted in alumina crucibles at 1173 K for few minutes. The melt was poured onto a preheated (573 K) brass plate and pressed by another plate to obtain flat circular disks. Next samples were heat-treated at 913 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 913 K, frequency range of 10 mHz to 1 MHz, with the ac voltage of 1 Vrms with Concept 40 broadband dielectric spectrometer. The higher harmonic components (harmonic 2) were measured up to frequency of 1000 Hz. 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: 10.34808/94gm-rq84
title: D.C. electrical measurements of Bi2VO5.5 ceramic measured at high temperature region

description: D.C. electrical properties of Bi2VO5.5 ceramic was measured. 
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.
For the electrical measurements gold electrodes were evaporated at the preheated samples. D.C. measurements were carried out with the use of Hioki 3522–50 LCR HiTester. Measurements were done in temperature range from 370 K to 920 K in air atmosphere. The temperature was controlled with the use of high temperature Novotherm HT 1600.
DOI: 10.34808/axk1-5e75
title: Nonlinear impedance as a function of A.C. voltage of Bi2VO5.5 ceramic of thickness 1.63 mm was measured with impedance spectroscopy method at high temperature region

description: The nonlinear electrical properties of Bi2VO5.5 ceramic of thickness 1.63 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 1.63 mm.
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 of : 0.01, 0.1, 1, 10, 100 and 1000 Hz, with the ac voltage ranging from 0.01 to 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/fchq-ax94
title: Nonlinear impedance as a function of A.C. voltage of Bi2VO5.5 ceramic of thickness 2.91 mm was measured with impedance spectroscopy method at high temperature region

description: The nonlinear electrical properties of Bi2VO5.5 ceramic of thickness 2.91 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 2.91 mm.
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 of : 0.01, 0.1, 1, 10, 100 and 1000 Hz, with the ac voltage ranging from 0.01 to 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: 10.34808/0hrq-0660
title: Nonlinear impedance as a function of A.C. voltage of Bi2VO5.5 ceramic of thickness 4.03 mm was measured with impedance spectroscopy method at high temperature region

description: The nonlinear electrical properties of Bi2VO5.5 ceramic of thickness 4.03 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 4.03 mm.
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 of : 0.01, 0.1, 1, 10, 100 and 1000 Hz, with the ac voltage ranging from 0.01 to 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: 10.6084/m9.figshare.14980621.v1
title: Table A. Near real-time management of spectral interferences with portable XRF spectrometers: Application to Sc quantification in nickeliferous laterite ores

description: <b>Table A</b>: Spectral characteristics (ROI ranges, Kα, Kβ spectral lines and escape peaks) for Ca, Sc, Ti, Mn and Fe analysis using pXRF, expressed in keV. The ROI ranges are obtained by the NDT Alpha software relative to pXRF (NitonTM XL3t GOLDD+ of ThermoFisher Scientific<sup>TM</sup>) with the ‘Soil’ mode using the ‘Low’ filter (20 kV and Cu target). EDS resolution is 130 eV based on the Kα spectral line of Mn. For this study, the critical spectral interference is coloured blue-grey (Ca interfering with Sc), while other spectral interferences are coloured light grey (Sc with Ti and Fe with Mn).
DOI: 10.6084/m9.figshare.14980633
title: Table B. Near real-time management of spectral interferences with portable XRF spectrometers: Application to Sc quantification in nickeliferous laterite ores

description: <b>Table B</b>: Synthesis of the mineralogical and geochemical characteristics of the samples analysed in this study.
DOI: 10.6084/m9.figshare.14980633.v1
title: Table B. Near real-time management of spectral interferences with portable XRF spectrometers: Application to Sc quantification in nickeliferous laterite ores

description: <b>Table B</b>: Synthesis of the mineralogical and geochemical characteristics of the samples analysed in this study.
DOI: 10.6084/m9.figshare.14980621
title: Table A. Near real-time management of spectral interferences with portable XRF spectrometers: Application to Sc quantification in nickeliferous laterite ores

description: <b>Table A</b>: Spectral characteristics (ROI ranges, Kα, Kβ spectral lines and escape peaks) for Ca, Sc, Ti, Mn and Fe analysis using pXRF, expressed in keV. The ROI ranges are obtained by the NDT Alpha software relative to pXRF (NitonTM XL3t GOLDD+ of ThermoFisher Scientific<sup>TM</sup>) with the ‘Soil’ mode using the ‘Low’ filter (20 kV and Cu target). EDS resolution is 130 eV based on the Kα spectral line of Mn. For this study, the critical spectral interference is coloured blue-grey (Ca interfering with Sc), while other spectral interferences are coloured light grey (Sc with Ti and Fe with Mn).
DOI: 10.34808/2fe5-nk41
title: Luminescence properties of TeOx-Eu gels

description: The DataSet contains the emission and excitation spectra of TeOx-Eu gels. 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 europium 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. 
Luminescence emission and excitation spectra of gel were collected in a Horiba Yvon spectrofluorometer (Fluorolog 3).
DOI: 10.34808/0cd1-qv73
title: Luminescence properties of TeOx-Dy gels

description: The DataSet contains the emission and excitation spectra of TeOx-Dy gel. 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 dysprosium 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. 
Luminescence emission and excitation spectra of gel were collected in a Horiba Yvon spectrofluorometer (Fluorolog 3).
DOI: 10.34808/r7d7-xy11
title: Luminescence properties of TeOx-Tb gels

description: The DataSet contains the emission and excitation spectra of TeOx-Tb gel. 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. 
Luminescence emission and excitation spectra of gel were collected in a Horiba Yvon spectrofluorometer (Fluorolog 3).
DOI: 10.34808/1h6g-9m98
title: Linear impedance of Bi2VO5.5 ceramic of thickness 2.88 mm measured with impedance spectroscopy method at low temperature region

description: The linear 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 in the temperature range from 153 K to 423 K, in the frequency range from 10mHz to 10 MHz and with the ac voltage of 1 Vrms with Concept 40 broadband dielectric spectrometer.
DOI: 10.34808/6hnv-5j31
title: Linear impedance of Bi2VO5.5 ceramic of thickness 2.52 mm measured with impedance spectroscopy method at low temperature region

description: The linear 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 in the temperature range from 153 K to 423 K, in the frequency range from 10mHz to 10 MHz and with the ac voltage of 1 Vrms with Concept 40 broadband dielectric spectrometer.
DOI: 10.34808/gm17-ft49
title: Nonlinear impedance as a function of frequency for Bi2VO5.5 ceramic of thickness 2.88 mm was measured at high temperature range 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 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/nnrh-ef06
title: Luminescence properties of TeOx gels

description: The DataSet contains the emission and excitation spectra of TeOx gels. 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.  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. 
Luminescence emission and excitation spectra of gel were collected in a Horiba Yvon spectrofluorometer (Fluorolog 3).
DOI: 10.6084/m9.figshare.14412851
title: S15 File. B73 MNase Control fragment centers bigwig file for B73v5.

description: Read-normalized FRENTER (fragment center) profile from MNase partial digest DNA control aligned to B73v5 in 5 bp window bins and used as input for peak segmentation.
DOI: 10.6084/m9.figshare.14412851.v2
title: S15 File. B73 MNase Control fragment centers bigwig file for B73v5.

description: Read-normalized FRENTER (fragment center) profile from MNase partial digest DNA control aligned to B73v5 in 5 bp window bins and used as input for peak segmentation.
DOI: 10.17029/98e07456-ffec-4d1e-a003-cdbd63982733
title: Dataset for "Perceptions of Performativity in English Further Education"

description: Quantitative responses to an electronic questionnaire.
DOI: 10.15468/9n5zes
title: Taxonomic revision of the Temnothorax salvini clade (Hymenoptera: Formicidae), with a key to the clades of New World Temnothorax

description: This dataset contains the digitized treatments in Plazi based on the original journal article Prebus, Matthew M. (2021): Taxonomic revision of the Temnothorax salvini clade (Hymenoptera: Formicidae), with a key to the clades of New World Temnothorax. PeerJ (e 11514) 9: 1-462, DOI: 10.7717/peerj.11514, URL: http://dx.doi.org/10.7717/peerj.11514
DOI: 10.5281/zenodo.5101839
title: epicPCR sequencing data, July 7 2021

description: Samples: 1. Biolstd, Nomock, Nomag, 16S<br> 2. Biolstd, Nomock, Mag, 16S<br> 3. Biolstd, Nomock, Nomag, 18S<br> 4. Biolstd, Nomock, Mag, 18S<br> 5. Biolstd, Mock, Nomag, 16S<br> 6. Biolstd, Mock, Mag, 16S<br> 7. Biolstd, Mock, Nomag, 18S<br> 8. Biolstd, Mock, Mag, 18S<br> 9. Biolstd+WW, Nomock, Nomag, 16S<br> 10. Biolstd+WW, Nomock, Mag, 16S<br> 11. Biolstd+WW, Nomock, Nomag, 18S<br> 12. Biolstd+WW, Nomock, Mag, 18S<br> 13. Biolstd+WW, Mock, Nomag, 16S<br> 14. Biolstd+WW, Mock, Mag, 16S<br> 15. Biolstd+WW, Mock, Nomag, 18S<br> 16. Biolstd+WW, Mock, Mag, 18S<br> 17. WW, Nomock, Nomag, 16S<br> 18. WW, Nomock, Mag, 16S<br> 19. WW, Nomock, Nomag, 18S<br> 20. WW, Nomock, Mag, 18S<br> 21. WW, Mock, Nomag, 16S<br> 22. WW, Mock, Mag, 16S<br> 23. WW, Mock, Nomag, 18S<br> 24. WW, Mock, Mag, 18S
DOI: 10.5281/zenodo.5101838
title: epicPCR sequencing data, July 7 2021

description: Samples: 1. Biolstd, Nomock, Nomag, 16S<br> 2. Biolstd, Nomock, Mag, 16S<br> 3. Biolstd, Nomock, Nomag, 18S<br> 4. Biolstd, Nomock, Mag, 18S<br> 5. Biolstd, Mock, Nomag, 16S<br> 6. Biolstd, Mock, Mag, 16S<br> 7. Biolstd, Mock, Nomag, 18S<br> 8. Biolstd, Mock, Mag, 18S<br> 9. Biolstd+WW, Nomock, Nomag, 16S<br> 10. Biolstd+WW, Nomock, Mag, 16S<br> 11. Biolstd+WW, Nomock, Nomag, 18S<br> 12. Biolstd+WW, Nomock, Mag, 18S<br> 13. Biolstd+WW, Mock, Nomag, 16S<br> 14. Biolstd+WW, Mock, Mag, 16S<br> 15. Biolstd+WW, Mock, Nomag, 18S<br> 16. Biolstd+WW, Mock, Mag, 18S<br> 17. WW, Nomock, Nomag, 16S<br> 18. WW, Nomock, Mag, 16S<br> 19. WW, Nomock, Nomag, 18S<br> 20. WW, Nomock, Mag, 18S<br> 21. WW, Mock, Nomag, 16S<br> 22. WW, Mock, Mag, 16S<br> 23. WW, Mock, Nomag, 18S<br> 24. WW, Mock, Mag, 18S
DOI: 10.6084/m9.figshare.14534784
title: Hypoxylaceae BGCs

description: biosynthetic gene cluster identified from 13 fungal species of the family Hypoxylaceae and Xylaria hypoxylon