Dataset Open Access

High-count rate photon detection with scintillators coupled to photomultiplier tubes and fast digitizers

García Rivas, Iris; Fernández Prieto, Antonio; Kögler, Toni; Roemer, Katja Ellen; Hueso González, Fernando


JSON-LD (schema.org) Export

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  "name": "High-count rate photon detection with scintillators coupled to photomultiplier tubes and fast digitizers", 
  "description": "<p>This repository contains raw experimental data acquired during the gELBE beam time performed in October 2023 under proposal number 23203137-ST, at Helmholtz-Zentrum Dresden - Rossendorf.</p>\n\n<p>In this setup, a bremsstrahlung beam of up to 12.5 MeV energy in 13 MHz pulses irradiates a CeBr<sub>3</sub> scintillation detector (by Hilger&reg;) of &Oslash; 1&#39;&#39; x 1&#39;&#39;, coupled to a Hamamatsu&reg; R13408-100 PMT, custom voltage divider and shaping electronics, and a commercial digitizer (SFMC01+SIS1160) by Struck&reg;, containing an AD9689 chip that supports a data sampling rate of 2.5 Gsps and 14-bits. This detector is developed in the context of the coaxial prompt gamma-ray monitoring method <a href=\"https://doi.org/10.1109/TRPMS.2019.2930362\">[1]</a>, where very high count rates are expected <a href=\"https://doi.org/10.1016/j.nima.2018.09.062\">[2]</a>. The dead-time-free data acquisition is programmed in-house using ROOT <a href=\"https://doi.org/10.1016/j.nima.2022.166701\">[3]</a>. In addition, a plastic scintillation detector (paddle) was placed inbetween the beam and the CeBr<sub>3</sub> crystal to serve as reference beam monitor. An Arduino is used to monitor the high-voltage supply for the PMT and active divider electronics in terms of current, voltage and temperature. A Comet Systems&reg; T7310 is used to monitor ambient temperature, humidity and pressure.</p>\n\n<p>The published data consist of the raw signal waveforms acquired during ~450 measurements. Each measurement is stored in a separate folder, its name being the acquisition time start, and lasts between 3 and 20 seconds (16 GiB up to 100 GiB). The data format is little-endian binary. Each sample uses two bytes, being the 14 first bits the digitized signal in a 1.7 V<sub>pp</sub> range, and the 15<sup>th</sup> bit the (negated) logic status of the reference beam monitor (paddle). Samples are stored consecutively, without headers. Sample time separation is 0.4 ns (2.5 Gsps). The digitizer is phase-locked to the accelerator radiofrequency (RF), so that each 2500 stored samples correspond to 13 consecutive periods of 13 MHz.</p>\n\n<p>The data can be directly opened using the open-source pulse visualization software (PulseSurfer) available in this link: <a href=\"https://igit.ific.uv.es/ferhue/pulse-surfer/\">https://igit.ific.uv.es/ferhue/pulse-surfer/</a>, with ROOT as a dependency. One just needs to run:</p>\n\n<pre><code class=\"language-bash\">root -l test_gui.cpp+(\\\"/path-to-folder/chA.bin\\\") </code></pre>\n\n<p>and then set 192.307692307692307696 in the &quot;Cycle&quot; box. Use the slider in the bottom to navigate across different consecutive frames. To visualize the paddle counter (negated) logic status, change the &quot;Mask&quot; box from 3FFF to 4000. There is also a checkbox to activate the baseline subtraction.</p>\n\n<p>In addition to the raw waveform data (<em>chA.bin</em>), each folder contains following metadata:</p>\n\n<ul>\n\t<li><em>log.root</em> a ROOT file storing all the measurement and hardware settings as TObjString. It also contains the T7310 monitoring as a TTree (&quot;pth&quot;)</li>\n\t<li><em>chA.root</em> a ROOT file storing a TTree that benchmarks the readout speed of the DAQ for this channel</li>\n\t<li><em>zdt.log</em> a text file storing the output printed by the DAQ software to terminal</li>\n\t<li><em>gui.png</em> Screenshot of the DAQ window</li>\n\t<li><em>hv.txt</em> a test file storing the monitoring of the high-voltage supply and electronics</li>\n</ul>", 
  "inLanguage": {
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  "citation": [
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      "@id": "https://doi.org/10.1016/j.nima.2022.166701"
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      "@id": "https://doi.org/10.1109/TRPMS.2019.2930362"
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      "@id": "https://doi.org/10.1016/j.nima.2018.09.062"
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    {
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      "@id": "https://doi.org/10.1088/1361-6560/ab176d"
    }, 
    {
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      "@id": "https://doi.org/10.1016/j.sna.2023.114859"
    }, 
    {
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      "@id": "https://doi.org/10.1109/JSEN.2021.3062428"
    }
  ], 
  "creator": [
    {
      "name": "Garc\u00eda Rivas, Iris", 
      "affiliation": "Triple Alpha Innovation SL - Instituto Galego de F\u00edsica de Altas Enerx\u00edas (IGFAE - USC)", 
      "@type": "Person", 
      "@id": "https://orcid.org/0000-0002-0968-7772"
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      "name": "Fern\u00e1ndez Prieto, Antonio", 
      "affiliation": "Instituto Galego de Fisica de Altas Enerxias, Santiago de Compostela, Spain", 
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      "@id": "https://orcid.org/0000-0003-1984-6367"
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      "name": "K\u00f6gler, Toni", 
      "affiliation": "Helmholtz-Zentrum Dresden \u2013 Rossendorf, Institute for Radiooncology \u2013 OncoRay, Dresden, Germany", 
      "@type": "Person", 
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      "affiliation": "Instituto de Fisica Corpuscular (IFIC), CSIC-UV, Paterna, Spain", 
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  "url": "https://rodare.hzdr.de/record/2807", 
  "keywords": [
    "Proton Therapy", 
    "Range Verification", 
    "High-count rate photon detection", 
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    "pile-up deconvolution"
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  "license": "https://creativecommons.org/licenses/by/4.0/legalcode", 
  "datePublished": "2024-04-16", 
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}
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