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The Wavelength-Shifting Optical Module

The Wavelength-shifting Optical Module (WOM) is a novel photosensor concept for the instrumentation of large detector volumes with single-photon sensitivity. The key objective is to improve the signal-to-noise ratio, which is achieved by decoupling the photosensitive area of a sensor from the cathod...

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Autores principales: Bastian-Querner, Benjamin, Binn, Lucas S., Böser, Sebastian, Brostean-Kaiser, Jannes, Hebecker, Dustin, Helbing, Klaus, Karg, Timo, Köpke, Lutz, Kowalski, Marek, Peiffer, Peter, Pollmann, Anna, Rack-Helleis, John, Rongen, Martin, Schlickmann, Lea, Thomas, Florian, Vocke, Anna
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8963010/
https://www.ncbi.nlm.nih.gov/pubmed/35214298
http://dx.doi.org/10.3390/s22041385
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author Bastian-Querner, Benjamin
Binn, Lucas S.
Böser, Sebastian
Brostean-Kaiser, Jannes
Hebecker, Dustin
Helbing, Klaus
Karg, Timo
Köpke, Lutz
Kowalski, Marek
Peiffer, Peter
Pollmann, Anna
Rack-Helleis, John
Rongen, Martin
Schlickmann, Lea
Thomas, Florian
Vocke, Anna
author_facet Bastian-Querner, Benjamin
Binn, Lucas S.
Böser, Sebastian
Brostean-Kaiser, Jannes
Hebecker, Dustin
Helbing, Klaus
Karg, Timo
Köpke, Lutz
Kowalski, Marek
Peiffer, Peter
Pollmann, Anna
Rack-Helleis, John
Rongen, Martin
Schlickmann, Lea
Thomas, Florian
Vocke, Anna
author_sort Bastian-Querner, Benjamin
collection PubMed
description The Wavelength-shifting Optical Module (WOM) is a novel photosensor concept for the instrumentation of large detector volumes with single-photon sensitivity. The key objective is to improve the signal-to-noise ratio, which is achieved by decoupling the photosensitive area of a sensor from the cathode area of its photomultiplier tube (PMT). The WOM consists of a transparent tube with two PMTs attached to its ends. The tube is coated with wavelength-shifting paint that absorbs ultraviolet photons with nearly 100% efficiency. Depending on the environment, e.g., air (ice), up to 73% (41%) of the subsequently emitted optical photons can be captured by total internal reflection and propagate towards the PMTs, where they are recorded. The optical properties of the paint, the geometry of the tube, and the coupling of the tube to the PMTs have been optimized for maximal sensitivity based on theoretical derivations and experimental evaluations. Prototypes were built to demonstrate the technique and to develop a reproducible construction process. Important measurable characteristics of the WOM are the wavelength-dependent effective area, the transit time spread of detected photons, and the signal-to-noise ratio. The WOM outperforms bare PMTs, especially with respect to the low signal-to-noise ratio with an increase of a factor up to 8.9 in air (5.2 in ice). Since the gain in sensitivity is mostly in the UV regime, the WOM is an ideal sensor for Cherenkov and scintillation detectors.
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spelling pubmed-89630102022-03-30 The Wavelength-Shifting Optical Module Bastian-Querner, Benjamin Binn, Lucas S. Böser, Sebastian Brostean-Kaiser, Jannes Hebecker, Dustin Helbing, Klaus Karg, Timo Köpke, Lutz Kowalski, Marek Peiffer, Peter Pollmann, Anna Rack-Helleis, John Rongen, Martin Schlickmann, Lea Thomas, Florian Vocke, Anna Sensors (Basel) Article The Wavelength-shifting Optical Module (WOM) is a novel photosensor concept for the instrumentation of large detector volumes with single-photon sensitivity. The key objective is to improve the signal-to-noise ratio, which is achieved by decoupling the photosensitive area of a sensor from the cathode area of its photomultiplier tube (PMT). The WOM consists of a transparent tube with two PMTs attached to its ends. The tube is coated with wavelength-shifting paint that absorbs ultraviolet photons with nearly 100% efficiency. Depending on the environment, e.g., air (ice), up to 73% (41%) of the subsequently emitted optical photons can be captured by total internal reflection and propagate towards the PMTs, where they are recorded. The optical properties of the paint, the geometry of the tube, and the coupling of the tube to the PMTs have been optimized for maximal sensitivity based on theoretical derivations and experimental evaluations. Prototypes were built to demonstrate the technique and to develop a reproducible construction process. Important measurable characteristics of the WOM are the wavelength-dependent effective area, the transit time spread of detected photons, and the signal-to-noise ratio. The WOM outperforms bare PMTs, especially with respect to the low signal-to-noise ratio with an increase of a factor up to 8.9 in air (5.2 in ice). Since the gain in sensitivity is mostly in the UV regime, the WOM is an ideal sensor for Cherenkov and scintillation detectors. MDPI 2022-02-11 /pmc/articles/PMC8963010/ /pubmed/35214298 http://dx.doi.org/10.3390/s22041385 Text en © 2022 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Bastian-Querner, Benjamin
Binn, Lucas S.
Böser, Sebastian
Brostean-Kaiser, Jannes
Hebecker, Dustin
Helbing, Klaus
Karg, Timo
Köpke, Lutz
Kowalski, Marek
Peiffer, Peter
Pollmann, Anna
Rack-Helleis, John
Rongen, Martin
Schlickmann, Lea
Thomas, Florian
Vocke, Anna
The Wavelength-Shifting Optical Module
title The Wavelength-Shifting Optical Module
title_full The Wavelength-Shifting Optical Module
title_fullStr The Wavelength-Shifting Optical Module
title_full_unstemmed The Wavelength-Shifting Optical Module
title_short The Wavelength-Shifting Optical Module
title_sort wavelength-shifting optical module
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8963010/
https://www.ncbi.nlm.nih.gov/pubmed/35214298
http://dx.doi.org/10.3390/s22041385
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