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Dataset for the publication "Eco-friendly ironmaking by biomass CO2 gasification: Process simulations for ecological and economic evaluation of CO2 recycling in direct reduction ironmaking"
No full text<h2>Dataset description</h2>
<p>This dataset contains the simulation results and data evaluations for the journal publication "Eco-friendly ironmaking by biomass CO2 gasification: Process simulations for ecological and economic evaluation of CO2 recycling in direct reduction ironmaking" by Florian J. Müller, Stefan Jankovic, Josef Fuchs, Diana Dimande, Stefan Müller, and Franz Winter. That journal publication was accepted for publication in Energy Conversion and Management on the 7th of October 2025 and includes a link to this dataset.</p>
<h3>Context and methodology</h3>
<p>Eight mass and energy balances in IPSEpro 8.0 were created to investigate different direct reduction ironmaking routes. The mass and balancing data were exported from IPSEpro and analyzed in Excel.</p>
<ul>
<li>Two routes titled NGR-DRI show a classical process with Natural Gas Reforming as a benchmark process.</li>
<li>Six novel routes show how Biomass CO2 Gasification can replace Natural Gas Reforming. Those routes are called BCG-DRI.</li>
</ul>
<p>Explanations and interpretations of these data are available in the journal publication.</p>
<h3>Technical details</h3>
<p>The data consist of three files:</p>
<ul>
<li>Two PNG files that show how the mass and energy balances for NGR-DRI and BCG-DRI are organized in IPSEpro.
<ul>
<li>These files contain the names of relevant streams and are necessary for understanding the detailed stream data in Excel.</li>
</ul>
</li>
<li>One XLSX file that contains all raw and interpreted data.
<ul>
<li>This file contains stream data, techno-economic evaluations, carbon footprint evaluations, and figures.</li>
</ul>
</li>
</ul>
<h3>Further details</h3>
<p>The journal publication is meant to be understood on its own and is supported by this dataset. Therefore, you are highly encouraged to seek out the journal publication first before trying to interprete this dataset. The journal publication also provides further context, additional data, and properly formatted citations to all relevant literature, which were only given briefly in the XLSX. The date of access for web-based sources was generally in the first half of 2024, but more details are also available in the journal article. Further explanations on how to use the xlsx are given on the READ_ME sheet of the XLSX file.</p>
Dataset for "APD direct detection receiver OEIC operating 14.1 dB above the shot noise quantum limit"
No full text<h1>Overview</h1>
<p>This repository provides measurement data and evaluated data related to our manuscript "<em>APD direct detection receiver OEIC operating 14.1 dB above the shot noise quantum limit</em>" by Simon Michael Laube, Christoph Gasser, Kerstin Schneider-Hornstein, and Horst Zimmerman, published in Optics Express, 2025, DOI: <a title="APD direct detection receiver OEIC operating 14.1 dB above the shot noise quantum limit" href="https://doi.org/10.1364/OE.577195">10.1364/OE.577195</a>.</p>
<h1>Context</h1>
<p>In our study, we present the design and experimental verification of two optoelectronic integrated circuits (OEICs). The main difference between the OEICs is the photodiode. The two photodiodes are:</p>
<ol>
<li>Avalanche photodiode, denoted by "APD"</li>
<li>p-i-n photodiode, denoted by "PIN"</li>
</ol>
<p>We measured the transient output voltage of the OEICs across optical input power with an oscilloscope and stored the waveforms in HDF5 files. The bit error probability (BER) was evaluated from the transient measurements using post-processing in Python, as explained in our manuscript. A data rate of 100 Mb/s with 80% return-to-zero (RZ) on-off keying (OOK) modulation was used for all BER measurements.</p>
<h1>File structure</h1>
<p>All measurement data is provided separately for each OEIC sample. Two samples were measured for each photodiode. Please note that the OEIC samples have individual sample identifiers that are part of the file names. The sample identifiers are:</p>
<ol>
<li>APD 1: C4_4</li>
<li>APD 2: B4_4</li>
<li>PIN 1: G2_2</li>
<li>PIN 2: H2_2</li>
</ol>
<p>The main folders <code>/BER</code>, <code>/powermeter</code>, and<code> /waveforms</code> are provided.</p>
<h2>Waveforms</h2>
<p><code>/waveforms</code> contains raw waveform (transient measurement) data. Waveforms are stored as HDF5 files (.h5 file ending) that contain an internal file system with metadata and data, generated by the oscilloscope. HDF5 files can be read using the free HDFView program, h5py Python library, or other software.</p>
<p>The internal file system within our HDF5 files has the following structure:<br><code>/FileType/KeysightH5FileType</code><br><code>/Frame/TheFrame</code><br><code>/Waveforms</code><br><code> /Channel 1/Channel 1 Data</code><br><code> /Channel 2/Channel 2 Data</code><br><code> /Channel 3/Channel 3 Data</code><br><code> /Function 1/Function 1 Data</code></p>
<p><code>KeysightH5FileType</code> and <code>TheFrame</code> are oscilloscope metadata. The <code>Channel 1</code> sub-folder contains metadata and <code>Channel 1 Data</code>. <code>Channel 1 Data</code> is the raw waveform data of the pseudo-random bit sequence (PRBS) that was used as the input signal of our OEICs. The <code>Channel 2</code> sub-folder contains metadata and <code>Channel 2 Data</code>. The <code>Channel 3</code> sub-folder contains metadata and <code>Channel 3 Data</code>. <code>Channel 2 Data</code> and <code>Channel 3 Data</code> is the raw waveform data of the OEIC output voltage. The output voltage is calculated from the difference between <code>Channel 3 Data</code> and <code>Channel 2 Data</code>, that is<br> output voltage=<code>Channel 3 Data</code> - <code>Channel 2 Data</code><br>The <code>Function 1</code> sub-folder contains metadata and <code>Function 1 Data</code>. <code>Function 1 Data</code> is the OEIC output voltage computed on the oscilloscope that was used for debugging only. Not all HDF5 files may contain the <code>Function 1</code> sub-folder.</p>
<p>The file name structure of the HDF5 files is<br> <code><sample identifier>_<measurement identifier>x<VSUB>x1<optical power identifier>x1.h5</code></p>
<p>Here, the sample identifier is the same as explained above; the measurement identifier is an arbitrary text/number; the VSUB is the substrate bias identifier; and the optical power identifier connects the power measurement (see below) with the corresponding waveform. Note that the VSUB field can be any number. For the actual voltage values of VSUB, please refer to the manuscript. As an example, the file "<code>G2_2_17Lx1x1x5x1.h5</code>" is the raw waveform of the PIN 1 sample, measurement "17L", recorded for the 5th optical power setting. </p>
<p> </p>
<h2>Optical Power</h2>
<p><code>/powermeter</code> contains the raw optical power measurement results, as well as the calibration factor that was used to calculate the power incident on the chip. In other words,<br> chip power=raw power * calibration factor.</p>
<p>The optical power measurements are provided in CSV files (.csv file ending), separately for each OEIC and measurement. Within the CSV files, the first column is the optical power identifier of the measurement (see above), and the second column is the respective raw optical power. The file name structure of the CSV files is<br> <code>power_<sample identifier>_<measurement identifier>.csv</code></p>
<p>The calibration factor is provided in a TXT file (.txt file ending), separately for each OEIC and measurement. The TXT file contains only a single floating-point number that is the calibration factor. The file name structure of the TXT file is<br> <code>calibration_<sample identifier>_<measurement identifier>.txt</code></p>
<p>Here, the sample identifier and measurement identifier are the same as for the waveform files, as explained above. For example, the files "<code>calibration_G2_2_17L.txt</code>" and "<code>power_G2_2_17L.csv</code>" correspond to all waveforms with the prefix "G2_2_17L", such as the abovementioned "<code>G2_2_17Lx1x1x5x1.h5</code>".</p>
<h2>Bit error probability</h2>
<p><code>/BER</code> contains the evaluated bit error probability of the OEICs. All files within this folder are generated from the raw data provided in <code>/waveforms</code> and <code>/powermeter</code>, using our Python script. Three file types are provided for each sample and data rate:</p>
<ol>
<li>Log files (.log file ending) that document the result of the evaluation. These log files were used to plot Fig. 5 in our manuscript.</li>
<li>Image files (.png file ending) that illustrate the result of the evaluation.</li>
<li>A CSV file that contains a results summary (.csv file ending).</li>
</ol>
<p>The log file contains metadata about the evaluation process, the evaluation result (BER), as well as the input file (waveform) and output files of the evaluation. Note that the .tab output files are not provided because they were only used for debugging of our Python script. While most of the log file contents should be self-explanatory, some require special attention:</p>
<ul>
<li>In the "User settings" section, we provide settings for the evaluation of the reference PRBS (<code>Channel 1 Data</code> in the HDF5 files). The boolean flag "PRBS inverted" shows whether the PRBS waveform was processed as is, or was logically inverted. The "PRBS detection threshold" is the threshold voltage that was used to digitize the (analog) PRBS waveform. Because the SNR of the PRBS is very high, the threshold itself is uncritical and was auto-detected by our Python script. The "PRBS detection offset" marks the start of the PRBS with respect to the recorded waveform. This is necessary because the recording may start at an arbitrary time, so the first recorded bit is incomplete. The start of the PRBS was auto-detected by our Python script by rising edge detection. The "PRBS detection delay" shows at which time instant each PRBS bit is sampled, with respect to the start of a bit. Typically, the bit should be sampled at the center. For 100 Mb/s with 80% RZ modulation, the center is 4 ns (=PRBS detection delay) after the start of the bit.</li>
<li>In the "Results" section, the result and the optimized settings for the evaluation of the chip output (<code>Channel 2 Data</code> and <code>Channel 3 Data</code> in the HDF5 files) are provided. "Decision threshold" is the threshold (voltage) for bit decision. "CDS delta time" is the time between the two sample instants of correlated double sampling (CDS). "Best BER" is the BER result. The "Static delay" is the coarse delay between PRBS and chip output waveform, given in multiples of the bit period (10 ns at 100 Mb/s). The "Inter-bit delay" is the fine delay between PRBS and the chip output waveform, which is always less than the bit period. The sum of static delay and inter-bit delay is the total delay between PRBS and the chip output waveform.</li>
</ul>
<p>The file name structure of the log files is<br> <code><sample identifier>_<measurement identifier>x<VSUB>x1x<optical power identifier>x1.log</code><br>The file name structure of the image files is<br> <code><sample identifier>_<measurement identifier>x<VSUB>x1x<optical power identifier>x1.png</code></p>
<p>The results summary CSV contains all optical power settings, the BER results, and the underlying dataset file names.</p>
<p>The file name structure of the CSV is<br> <code>BER_<sample>_100Mbps_80RZ.csv</code><br>where sample is APD_1, APD_2, PIN_1, or PIN_2, as defined above.</p>
<h2>Other data</h2>
<p>Some raw data is given in the manuscript in tabular form. These data are not included in this dataset.</p>
<h1><br><br>Licensing</h1>
<p>The dataset consists of raw measurement data and processed data.<br>Raw data is licensed under the <strong>Creative Commons Zero 1.0 Universal (CC0)</strong> license.<br>Processed data is copyrighted and licensed under the <strong>Creative Commons Attribution 4.0 International (CC-BY)</strong> license.<br>All metadata is licensed under the<strong> Creative Commons Attribution 4.0 International (CC-BY)</strong> license.</p>
<p>The following list shows the license attached to the individual files:</p>
<ul>
<li>All files and sub-folders within <code>/waveforms</code>: <strong>CC0</strong> license</li>
<li>All files and sub-folders within <code>/powermeter</code>: <strong>CC0</strong> license</li>
<li>All files and sub-folders within <code>/BER</code>: <strong>CC-BY</strong> license</li>
<li><code>/README.txt</code>:<strong> CC-BY</strong> license</li>
</ul>
Adapting the IEC 62443 Standard for Representation in JSON
No full text<p>This dataset provides a structured representation of the <a href="https://www.isa.org/standards-and-publications/isa-standards/isa-iec-62443-series-of-standards"><strong>IEC 62443 Standard</strong></a> in JSON format, enabling developers, cybersecurity professionals, and automation engineers to programmatically access, analyze, and utilize the standard's content.</p>
<h2>Key Features</h2>
<ul>
<li><strong>JSON Representation</strong>: A machine-readable format of the IEC 62443 standard for easy integration into software solutions.</li>
<li><strong>Standard Mapping</strong>: Logical mapping of concepts, clauses, and requirements from IEC 62443 into JSON objects.</li>
<li><strong>Automation-Ready</strong>: Facilitates the development of tools for compliance assessment, system auditing, and cybersecurity management.</li>
<li><strong>Open Source</strong>: Contributions are welcome to enhance the structure and usability of the JSON transformation.</li>
</ul>
<h2>Use Cases</h2>
<ul>
<li><strong>Compliance Automation</strong>: Build tools to verify system conformance with IEC 62443 requirements.</li>
<li><strong>Data Integration</strong>: Integrate the standard into existing cybersecurity tools.</li>
<li><strong>Custom Visualization</strong>: Develop dashboards and reports using the JSON data.</li>
</ul>
<h2>IEC 62443</h2>
<p>The IEC 62443 standard aims to provide a framework for ensuring the security of Industrial Automation and Control Systems (IACS) throughout their lifecycle, from design and development to deployment, operation, and maintenance. Its objective is to minimize risks associated with cyber threats while ensuring the safe and reliable operation of industrial systems.</p>
<ul>
<li><strong>IEC 62443-2-4:</strong> Security program requirements for IACS service providers</li>
<li><strong>IEC 62443-3-2:</strong> Security risk assessment and system design</li>
<li><strong>IEC 62443-3-3:</strong> System security requirements and security levels</li>
<li><strong>IEC 62443-4-1:</strong> Secure product development lifecycle requirements</li>
<li><strong>IEC 62443-4-2:</strong> Technical security requirements for IACS components</li>
</ul>
Data for the publication "Size Effect on the Thermal Conductivity of a Type-I Clathrate"
No full text<h3>Context and methodology </h3>
<ul>
<li>This repository contains the data behind the publication "Size Effect on the Thermal Conductivity of a Type-I Clathrate" (10.3390/cryst13030453).</li>
<li>The dataset was created manually by collecting and ordering the relevant data.</li>
<li>The publication presents and discusses the thermal conductivity of type-I clathrate mesowires with different diameters, measured with a 3-omega technique. The fitting operations and simulations were conducted using data analysis software from OriginLab. </li>
</ul>
<h3>Description of the data </h3>
<ul>
<li><strong>Fig5</strong> illustrates the data analysis behind a 3-omega thermal conductivity measurement: <br>Fig5a.dat contains the measured frequency dependence of a 3rd harmonic voltage signal "V_3omega(f)" of a 25um Pt wire, as well as a fit to the data. <br>Fig5b.dat is a representative dataset of a 3-omega measurement done on one 920nm mesowire. It contains measurements of the 3rd harmonic voltage "V_3omega" as a function of excitation current "I^3" for temperatures ranging from 300K to 80K, in 20K steps and linear fits to the data, demonstrating the "V_3omega" ~ "I^3" dependence. </li>
<li><strong>Fig6</strong> presents the thermal conductivity and electrical resistivity of the mesowires. The results are the average of measurements of two different mesowires, the dispersion being represented by an error bar: <br>Fig6a.dat contains the lattice contribution to the thermal conductivity "kappa_ph" with an error bar "kappa_ph (Er+-)" and the electronic contribution "kappa_el" with an error bar "kappa_el (Er+-)" as a function of temperature "T" for mesowires of three different diameters 630nm, 920nm, and 1260nm.<br>Fig6b.dat contains the electrical resistivity "rho" with an error bar "rho (Er+-)" as a function of temperature "T" for mesowires of three different diameters 630nm, 920nm, and 1260nm. </li>
<li><strong>Fig7</strong> compares the accuracy of a modified Callaway model and the original Callaway model in describing our data: <br>Fig7a.dat contains the lattice contribution data "kappa_ph" for the mesowires from Fig6a, as well as a fit to bulk data (obtained from M. S. Ikeda for a different publication and therefore not inlcuded here) using a modified Callaway model. Simulations of the lattice thermal conductivity based on the model with the obtained fitting parameters are included for each mesowire diameter.<br>Fig7b.dat contains "kappa_ph" for the mesowires from Fig6a, as well as a fit to bulk data using the original Callaway and subsequent simulations for the mesowires. </li>
<li><strong>Fig8</strong> contains "kappa_ph" with an error bar "kappa_ph (Er+-)" as a function of boundary scattering length "lambda", as well as simulations using both the modified and the original Callaway model.</li>
<li><strong>Fig9</strong> contains the calculated figure of merit "ZT" with an error bar "ZT (Er+-)" as a function of temperature "T" for mesowires of three different diameters 630nm, 920nm, and 1260nm. </li>
</ul>
<h3>Technical details</h3>
<p>For each figure there is a corresponding file containing the data shown in the figure. Data files, with the extension .dat, are text files, and named logically after data they contain. </p>
<p>The dataset does not require any specific software for reading. </p>
Research data for "Highlighting the influence between physical and chemical crosslinking in dynamic hydrogels for two-photon micropatterning"
No full text<h2>Context</h2>
<p>This dataset was created from original work conducted in the framework of a PhD project and compiled in a publication (<em>"Highlighting the Influence between Physical and Chemical Cross-Linking in Dynamic Hydrogels for Two-Photon Micropatterning"</em>, <a href="https://doi.org/10.1021/acs.biomac.5c00062">https://doi.org/10.1021/acs.biomac.5c00062</a>). It provides the raw data of results presented and discussed therein.</p>
<h2>Technical details</h2>
<p>Microsoft Excel file “Raw Data_Photocleavable Hydrogels”:</p>
<p>Tab 1 - Raw Data obtained for real-time (RT) NIR photorheology of 5-10 wt% PVA-NB:SS-DT hydrogels</p>
<p>Tab 2 - Raw Data obtained for real-time (RT) NIR photorheology of 10 wt% PVA-NB:SS-DT hydrogels with varying Li-TPO content</p>
<p>Tab 3 - Raw Data obtained for real-time (RT) NIR photorheology of IPN5, IPN7.5 and IPN10</p>
<p>Tab 4 - Raw Data obtained for real-time (RT) NIR photorheology of hybrid gels containing 5-10 wt% PVA-NB:SS-DT and 10 wt% Gel-NB:SS-DT</p>
<p>Tab 5 - Mass swelling ratio of hydrogels</p>
<p>Tab 6 – Hydrolytic degradation of IPNs</p>
<p>Tab 7 – Hydrolytic degradation of hybrid gels</p>
<p>Tab 8 - Raw Data obtained for real-time (RT) NIR photorheology of IPN5 with varying irradiation times</p>
<p>Tab 9 - Raw Data obtained for real-time (RT) NIR photorheology of IPN5 with varying light sources</p>
<p>Tab 10 - Hydrolytic degradation + mass swell ratio of IPNs</p>
<p>Tab 11 - Raw Data obtained for real-time (RT) NIR photorheology of 10 wt% Gel-NB:SS-DT</p>
<p>Tab 12 - Hydrolytic degradation + mass swell ratio of hybrid gels</p>
<h3>NMR zip file</h3>
<p>‘1H SS-DT’, ‘13C SS-DT', ‘1H PVA-NB’ and ‘1H Gel-NB’ folders:</p>
<p>NMR data obtained during all synthesis steps of the dithiol crosslinker (SS-DT) and norbornene-modified macromers (PVA-NB, Gel-NB) used herein. See Supplementary Information Chapter 1 for structures and calculation of degree of substitution (DS).</p>
<p>A software to display NMR-spectra is needed, such as <a href="https://mestrelab.com/download/mnova/">MestreNova</a> or <a href="https://www.bruker.com/en/products-and-solutions/mr/nmr-software/topspin.html">Topspin</a>.</p>
<h3>Compund descriptions</h3>
<p>Compound descriptions in the files included herein adhere to the naming in the related publication referenced in the Related Works section, where all compounds are described in detail and drawn as structural formulas. In brief:</p>
<p>PVA-NB: norbornene-modified poly(vinyl alcohol)</p>
<p>Gel-NB: norbornene-modified gelatin (type A, bloom 300)</p>
<p>SS-DT: 2-[2-(3-Mercaptopropionoxy)ethyldithio]ethyl 3-mercaptopropionate</p>
<p>Li-TPO: Lithium-Phenyl-2,4,6-trimethylbenzoylphosphinat</p><p>Photolabile hydrogels have gained tremendous interest for a wide range of applications in materials and life sciences. Usually, photodegradability is introduced via chromophores and labile bonds, making such materials intrinsically light sensitive. In recent years, disulfide bonds have emerged as an innovative alternative, as they can be selectively cleaved in the presence of (photo)generated radicals. However, such materials suffer from limited network stability and high swelling as a result of thiol–disulfide metathesis reactions. Herein, we present two strategies to counteract such phenomena by network stabilization either via physical or chemical incorporation of (un)modified gelatin macromers to norbornene-modified poly(vinyl alcohol) networks. Photolabile behavior was introduced by a simple disulfide-containing dithiol cross-linker. Tunable material properties were investigated by means of in situ photorheology, in vitro swelling, and degradation experiments. Finally, we demonstrate an innovative method for localized disulfide cleavage via two-photon micropatterning.</p>
Digital twin-assisted process design for NK-cell therapies (FWF_DigiNK I5910)
No full text<p>Supporting and additional data, experimental data and multivariate evaluation sheets from project FWF_DigiNK (I5910). Data in this ZIP file are:</p>
<p>DoE1 = effect of cultivation medium componenets on growth and cytotoxicity of NK cells</p>
<p>DoE2 = extension of DoE1</p>
<p>Multivariate MODDE files (software <a href="https://www.sartorius.com/en">Sartorius</a>)</p>
<h2>Required software</h2>
<p>The software required to open and work with the files is:</p>
<ul>
<li><code>.xlsx</code> = Excel</li>
<li><code>.mip</code> = modde</li>
<li><code>.usp</code> = Simca</li>
<li><code>.wsp</code> = flowjow workspace (together with <code>.fcs</code>)</li>
</ul>
<h2>License</h2>
<p>All data are licensed under the CC BY 4.0 license.</p><p>Natural killer (NK) cells make only a small fraction of immune cells in the human body, however, play a pivotal role in the fight against cancer by the immune system. They are capable of eliminating abnormal cells via several direct or indirect cytotoxicity pathways in a self-regulating manner, which makes them a favorable choice as a cellular therapy against cancer. Additionally, allogeneic NK cells, unlike other lymphocytes, do not or only minimally cause graft-versus-host diseases opening the door for an off-the-shelf therapy. However, to date, the production of NK cells faces several difficulties, especially because the critical process parameters (CPPs) influencing the critical quality attributes (CQAs) are difficult to identify or correlate. There are numerous different cultivation platforms available, all with own characteristics, benefits and disadvantages that add further difficulty to define CPPs and relate them to CQAs. Our goal in this contribution was to summarize the current knowledge about NK cell expansion CPPs and CQAs, therefore we analyzed the available literature of both dynamic and static culture format experiments in a systematic manner. We present a list of the identified CQAs and CPPs and discuss the role of each CPP in the regulation of the CQAs. Furthermore, we could identify potential relationships between certain CPPs and CQAs. The findings based on this systematic literature research can be the foundation for meaningful experiments leading to better process understanding and eventually control.</p>
Coree Rosina [Proporz] (A-Wn_Mus.Hs._18688_n03) Audio recording
No full text<h1>Audio recording of a lute piece from the E-LAUTE project</h1><h2>Overview</h2><p>This dataset contains an audio recording of the piece "Coree Rosina [Proporz]", a 16th century lute music piece originally notated in lute tablature, created as part of the E-LAUTE project (<a href="https://e-laute.info/">https://e-laute.info/</a>). The recording preserves and makes historical lute music from the German-speaking regions during 1450-1550 accessible.</p><p>The recording is based on the work with the title "Coree Rosina [Proporz]" and the id "A-Wn_Mus.Hs._18688_n03" in the e-lautedb. It is found on the page(s) or folio(s) 5v-6r in the source "[Lautentabulatur des Stephan Craus]" with the source-id "A-Wn_Mus.Hs._18688".</p><p>The original source and multiple transcriptions of the work can be found on the E-LAUTE platform: <a href="https://edition.onb.ac.at/fedora/objects/o:lau.A-Wn_Mus.Hs._18688/methods/sdef:TEI/get?mode=n03" target="_blank">https://edition.onb.ac.at/fedora/objects/o:lau.A-Wn_Mus.Hs._18688/methods/sdef:TEI/get?mode=n03</a>.</p><p>Links to the source: <a href="http://data.onb.ac.at/rec/AC14316391" target="_blank">http://data.onb.ac.at/rec/AC14316391</a>, <a href="https://rism.online/sources/600141880" target="_blank">https://rism.online/sources/600141880</a>, .</p><h2>Dataset Contents</h2><p>This dataset includes:</p><ul><li><strong>Audio file</strong>: An audio recording of the lute piece in .wav format</li> <li><strong>Metadata file</strong>: A metadata file with detailed information about the recording in .json format</li></ul><h2>About the E-LAUTE Project</h2><p><strong>E-LAUTE: Electronic Linked Annotated Unified Tablature Edition - The Lute in the German-Speaking Area 1450-1550</strong></p><p>The E-LAUTE project creates innovative digital editions of lute tablatures from the German-speaking area between 1450 and 1550. This interdisciplinary "open knowledge platform" combines musicology, music practice, music informatics, and literary studies to transform traditional editions into collaborative research spaces.</p><p>For more information, visit the project website: <a href="https://e-laute.info/">https://e-laute.info/</a></p>
Mein hertz thut alezeit verlangen (Ger_1533-1_n24) Audio recording
No full text<h1>Audio recording of a lute piece from the E-LAUTE project</h1><h2>Overview</h2><p>This dataset contains an audio recording of the piece "Mein hertz thut alezeit verlangen", a 16th century lute music piece originally notated in lute tablature, created as part of the E-LAUTE project (<a href="https://e-laute.info/">https://e-laute.info/</a>). The recording preserves and makes historical lute music from the German-speaking regions during 1450-1550 accessible.</p><p>The recording is based on the work with the title "Mein hertz thut alezeit verlangen" and the id "Ger_1533-1_n24" in the e-lautedb. It is found on the page(s) or folio(s) XXIIIr-XXIIIv in the source "Tabulatur auff die Laudten" with the source-id "Ger_1533-1".</p><p>The original source and multiple transcriptions of the work can be found on the E-LAUTE platform: <a href="https://edition.onb.ac.at/fedora/objects/o:lau.Ger_1533-1/methods/sdef:TEI/get?mode=n24" target="_blank">https://edition.onb.ac.at/fedora/objects/o:lau.Ger_1533-1/methods/sdef:TEI/get?mode=n24</a>.</p><p>Links to the source: <a href="http://resolver.staatsbibliothek-berlin.de/SBB0001F5B500000000" target="_blank">http://resolver.staatsbibliothek-berlin.de/SBB0001F5B500000000</a>, <a href="https://opac.rism.info/rism/Record/rism993104093" target="_blank">https://opac.rism.info/rism/Record/rism993104093</a>, <a href="https://gateway-bayern.de/VD16+G+1578" target="_blank">https://gateway-bayern.de/VD16+G+1578</a>, .</p><h2>Dataset Contents</h2><p>This dataset includes:</p><ul><li><strong>Audio file</strong>: An audio recording of the lute piece in .wav format</li> <li><strong>Metadata file</strong>: A metadata file with detailed information about the recording in .json format</li></ul><h2>About the E-LAUTE Project</h2><p><strong>E-LAUTE: Electronic Linked Annotated Unified Tablature Edition - The Lute in the German-Speaking Area 1450-1550</strong></p><p>The E-LAUTE project creates innovative digital editions of lute tablatures from the German-speaking area between 1450 and 1550. This interdisciplinary "open knowledge platform" combines musicology, music practice, music informatics, and literary studies to transform traditional editions into collaborative research spaces.</p><p>For more information, visit the project website: <a href="https://e-laute.info/">https://e-laute.info/</a></p>
Rosina (A-Wn_Mus.Hs._18688_n29) Audio recording
No full text<h1>Audio recording of a lute piece from the E-LAUTE project</h1><h2>Overview</h2><p>This dataset contains an audio recording of the piece "Rosina", a 16th century lute music piece originally notated in lute tablature, created as part of the E-LAUTE project (<a href="https://e-laute.info/">https://e-laute.info/</a>). The recording preserves and makes historical lute music from the German-speaking regions during 1450-1550 accessible.</p><p>The recording is based on the work with the title "Rosina" and the id "A-Wn_Mus.Hs._18688_n29" in the e-lautedb. It is found on the page(s) or folio(s) 20v-21r in the source "[Lautentabulatur des Stephan Craus]" with the source-id "A-Wn_Mus.Hs._18688".</p><p>The original source and multiple transcriptions of the work can be found on the E-LAUTE platform: <a href="https://edition.onb.ac.at/fedora/objects/o:lau.A-Wn_Mus.Hs._18688/methods/sdef:TEI/get?mode=n29" target="_blank">https://edition.onb.ac.at/fedora/objects/o:lau.A-Wn_Mus.Hs._18688/methods/sdef:TEI/get?mode=n29</a>.</p><p>Links to the source: <a href="http://data.onb.ac.at/rec/AC14316391" target="_blank">http://data.onb.ac.at/rec/AC14316391</a>, <a href="https://rism.online/sources/600141880" target="_blank">https://rism.online/sources/600141880</a>, .</p><h2>Dataset Contents</h2><p>This dataset includes:</p><ul><li><strong>Audio file</strong>: An audio recording of the lute piece in .wav format</li> <li><strong>Metadata file</strong>: A metadata file with detailed information about the recording in .json format</li></ul><h2>About the E-LAUTE Project</h2><p><strong>E-LAUTE: Electronic Linked Annotated Unified Tablature Edition - The Lute in the German-Speaking Area 1450-1550</strong></p><p>The E-LAUTE project creates innovative digital editions of lute tablatures from the German-speaking area between 1450 and 1550. This interdisciplinary "open knowledge platform" combines musicology, music practice, music informatics, and literary studies to transform traditional editions into collaborative research spaces.</p><p>For more information, visit the project website: <a href="https://e-laute.info/">https://e-laute.info/</a></p>
Nach willen dein (A-Wn_Mus.Hs._18688_n63) Audio recording
No full text<h1>Audio recording of a lute piece from the E-LAUTE project</h1><h2>Overview</h2><p>This dataset contains an audio recording of the piece "Nach willen dein", a 16th century lute music piece originally notated in lute tablature, created as part of the E-LAUTE project (<a href="https://e-laute.info/">https://e-laute.info/</a>). The recording preserves and makes historical lute music from the German-speaking regions during 1450-1550 accessible.</p><p>The recording is based on the work with the title "Nach willen dein" and the id "A-Wn_Mus.Hs._18688_n63" in the e-lautedb. It is found on the page(s) or folio(s) 35r in the source "[Lautentabulatur des Stephan Craus]" with the source-id "A-Wn_Mus.Hs._18688".</p><p>The original source and multiple transcriptions of the work can be found on the E-LAUTE platform: <a href="https://edition.onb.ac.at/fedora/objects/o:lau.A-Wn_Mus.Hs._18688/methods/sdef:TEI/get?mode=n63" target="_blank">https://edition.onb.ac.at/fedora/objects/o:lau.A-Wn_Mus.Hs._18688/methods/sdef:TEI/get?mode=n63</a>.</p><p>Links to the source: <a href="http://data.onb.ac.at/rec/AC14316391" target="_blank">http://data.onb.ac.at/rec/AC14316391</a>, <a href="https://rism.online/sources/600141880" target="_blank">https://rism.online/sources/600141880</a>, .</p><h2>Dataset Contents</h2><p>This dataset includes:</p><ul><li><strong>Audio file</strong>: An audio recording of the lute piece in .wav format</li> <li><strong>Metadata file</strong>: A metadata file with detailed information about the recording in .json format</li></ul><h2>About the E-LAUTE Project</h2><p><strong>E-LAUTE: Electronic Linked Annotated Unified Tablature Edition - The Lute in the German-Speaking Area 1450-1550</strong></p><p>The E-LAUTE project creates innovative digital editions of lute tablatures from the German-speaking area between 1450 and 1550. This interdisciplinary "open knowledge platform" combines musicology, music practice, music informatics, and literary studies to transform traditional editions into collaborative research spaces.</p><p>For more information, visit the project website: <a href="https://e-laute.info/">https://e-laute.info/</a></p>