Cargando…
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...
Autores principales: | , , , , , , , , , , , , , , , |
---|---|
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 |
_version_ | 1784677899868045312 |
---|---|
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. |
format | Online Article Text |
id | pubmed-8963010 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2022 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
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 |
work_keys_str_mv | AT bastianquernerbenjamin thewavelengthshiftingopticalmodule AT binnlucass thewavelengthshiftingopticalmodule AT bosersebastian thewavelengthshiftingopticalmodule AT brosteankaiserjannes thewavelengthshiftingopticalmodule AT hebeckerdustin thewavelengthshiftingopticalmodule AT helbingklaus thewavelengthshiftingopticalmodule AT kargtimo thewavelengthshiftingopticalmodule AT kopkelutz thewavelengthshiftingopticalmodule AT kowalskimarek thewavelengthshiftingopticalmodule AT peifferpeter thewavelengthshiftingopticalmodule AT pollmannanna thewavelengthshiftingopticalmodule AT rackhelleisjohn thewavelengthshiftingopticalmodule AT rongenmartin thewavelengthshiftingopticalmodule AT schlickmannlea thewavelengthshiftingopticalmodule AT thomasflorian thewavelengthshiftingopticalmodule AT vockeanna thewavelengthshiftingopticalmodule AT bastianquernerbenjamin wavelengthshiftingopticalmodule AT binnlucass wavelengthshiftingopticalmodule AT bosersebastian wavelengthshiftingopticalmodule AT brosteankaiserjannes wavelengthshiftingopticalmodule AT hebeckerdustin wavelengthshiftingopticalmodule AT helbingklaus wavelengthshiftingopticalmodule AT kargtimo wavelengthshiftingopticalmodule AT kopkelutz wavelengthshiftingopticalmodule AT kowalskimarek wavelengthshiftingopticalmodule AT peifferpeter wavelengthshiftingopticalmodule AT pollmannanna wavelengthshiftingopticalmodule AT rackhelleisjohn wavelengthshiftingopticalmodule AT rongenmartin wavelengthshiftingopticalmodule AT schlickmannlea wavelengthshiftingopticalmodule AT thomasflorian wavelengthshiftingopticalmodule AT vockeanna wavelengthshiftingopticalmodule |