Attenuation of vacuum ultraviolet light in liquid argon
Abstract The transmission of liquid argon has been measured, wavelength resolved, for a wavelength interval from 118 to 250 nm. The wavelength dependent attenuation length is presented for pure argon. It is shown that no universal wavelength independent attenuation length can be assigned to liquid a...
Ausführliche Beschreibung
Autor*in: |
Neumeier, A. [verfasserIn] Hofmann, M. [verfasserIn] Oberauer, L. [verfasserIn] Potzel, W. [verfasserIn] Schönert, S. [verfasserIn] Dandl, T. [verfasserIn] Heindl, T. [verfasserIn] Ulrich, A. [verfasserIn] Wieser, J. [verfasserIn] |
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E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2012 |
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Übergeordnetes Werk: |
Enthalten in: The European physical journal - Berlin : Springer, 1998, 72(2012), 10 vom: 25. Okt. |
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Übergeordnetes Werk: |
volume:72 ; year:2012 ; number:10 ; day:25 ; month:10 |
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DOI / URN: |
10.1140/epjc/s10052-012-2190-z |
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Katalog-ID: |
SPR00832705X |
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520 | |a Abstract The transmission of liquid argon has been measured, wavelength resolved, for a wavelength interval from 118 to 250 nm. The wavelength dependent attenuation length is presented for pure argon. It is shown that no universal wavelength independent attenuation length can be assigned to liquid argon for its own fluorescence light due to the interplay between the wavelength dependent emission and absorption. A decreasing transmission is observed below 130 nm in both chemically cleaned and distilled liquid argon and assigned to absorption by the analogue of the first argon excimer continuum. For not perfectly cleaned argon a strong influence of impurities on the transmission is observed. Two strong absorption bands at 126.5 and 141.0 nm with approximately 2 and 4 nm width, respectively, are assigned to traces of xenon in argon. A broad absorption region below 180 nm is found for unpurified argon and tentatively attributed to the presence of water in the argon sample. | ||
650 | 4 | |a Xenon |7 (dpeaa)DE-He213 | |
650 | 4 | |a Krypton |7 (dpeaa)DE-He213 | |
650 | 4 | |a Liquid Argon |7 (dpeaa)DE-He213 | |
650 | 4 | |a Attenuation Length |7 (dpeaa)DE-He213 | |
650 | 4 | |a Deuterium Lamp |7 (dpeaa)DE-He213 | |
700 | 1 | |a Hofmann, M. |e verfasserin |4 aut | |
700 | 1 | |a Oberauer, L. |e verfasserin |4 aut | |
700 | 1 | |a Potzel, W. |e verfasserin |4 aut | |
700 | 1 | |a Schönert, S. |e verfasserin |4 aut | |
700 | 1 | |a Dandl, T. |e verfasserin |4 aut | |
700 | 1 | |a Heindl, T. |e verfasserin |4 aut | |
700 | 1 | |a Ulrich, A. |e verfasserin |4 aut | |
700 | 1 | |a Wieser, J. |e verfasserin |4 aut | |
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10.1140/epjc/s10052-012-2190-z doi (DE-627)SPR00832705X (SPR)s10052-012-2190-z-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Neumeier, A. verfasserin aut Attenuation of vacuum ultraviolet light in liquid argon 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The transmission of liquid argon has been measured, wavelength resolved, for a wavelength interval from 118 to 250 nm. The wavelength dependent attenuation length is presented for pure argon. It is shown that no universal wavelength independent attenuation length can be assigned to liquid argon for its own fluorescence light due to the interplay between the wavelength dependent emission and absorption. A decreasing transmission is observed below 130 nm in both chemically cleaned and distilled liquid argon and assigned to absorption by the analogue of the first argon excimer continuum. For not perfectly cleaned argon a strong influence of impurities on the transmission is observed. Two strong absorption bands at 126.5 and 141.0 nm with approximately 2 and 4 nm width, respectively, are assigned to traces of xenon in argon. A broad absorption region below 180 nm is found for unpurified argon and tentatively attributed to the presence of water in the argon sample. Xenon (dpeaa)DE-He213 Krypton (dpeaa)DE-He213 Liquid Argon (dpeaa)DE-He213 Attenuation Length (dpeaa)DE-He213 Deuterium Lamp (dpeaa)DE-He213 Hofmann, M. verfasserin aut Oberauer, L. verfasserin aut Potzel, W. verfasserin aut Schönert, S. verfasserin aut Dandl, T. verfasserin aut Heindl, T. verfasserin aut Ulrich, A. verfasserin aut Wieser, J. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 72(2012), 10 vom: 25. Okt. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:72 year:2012 number:10 day:25 month:10 https://dx.doi.org/10.1140/epjc/s10052-012-2190-z kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_63 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_206 GBV_ILN_267 GBV_ILN_293 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_4012 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4305 GBV_ILN_4307 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4338 33.50 ASE AR 72 2012 10 25 10 |
spelling |
10.1140/epjc/s10052-012-2190-z doi (DE-627)SPR00832705X (SPR)s10052-012-2190-z-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Neumeier, A. verfasserin aut Attenuation of vacuum ultraviolet light in liquid argon 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The transmission of liquid argon has been measured, wavelength resolved, for a wavelength interval from 118 to 250 nm. The wavelength dependent attenuation length is presented for pure argon. It is shown that no universal wavelength independent attenuation length can be assigned to liquid argon for its own fluorescence light due to the interplay between the wavelength dependent emission and absorption. A decreasing transmission is observed below 130 nm in both chemically cleaned and distilled liquid argon and assigned to absorption by the analogue of the first argon excimer continuum. For not perfectly cleaned argon a strong influence of impurities on the transmission is observed. Two strong absorption bands at 126.5 and 141.0 nm with approximately 2 and 4 nm width, respectively, are assigned to traces of xenon in argon. A broad absorption region below 180 nm is found for unpurified argon and tentatively attributed to the presence of water in the argon sample. Xenon (dpeaa)DE-He213 Krypton (dpeaa)DE-He213 Liquid Argon (dpeaa)DE-He213 Attenuation Length (dpeaa)DE-He213 Deuterium Lamp (dpeaa)DE-He213 Hofmann, M. verfasserin aut Oberauer, L. verfasserin aut Potzel, W. verfasserin aut Schönert, S. verfasserin aut Dandl, T. verfasserin aut Heindl, T. verfasserin aut Ulrich, A. verfasserin aut Wieser, J. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 72(2012), 10 vom: 25. Okt. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:72 year:2012 number:10 day:25 month:10 https://dx.doi.org/10.1140/epjc/s10052-012-2190-z kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_63 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_206 GBV_ILN_267 GBV_ILN_293 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_4012 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4305 GBV_ILN_4307 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4338 33.50 ASE AR 72 2012 10 25 10 |
allfields_unstemmed |
10.1140/epjc/s10052-012-2190-z doi (DE-627)SPR00832705X (SPR)s10052-012-2190-z-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Neumeier, A. verfasserin aut Attenuation of vacuum ultraviolet light in liquid argon 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The transmission of liquid argon has been measured, wavelength resolved, for a wavelength interval from 118 to 250 nm. The wavelength dependent attenuation length is presented for pure argon. It is shown that no universal wavelength independent attenuation length can be assigned to liquid argon for its own fluorescence light due to the interplay between the wavelength dependent emission and absorption. A decreasing transmission is observed below 130 nm in both chemically cleaned and distilled liquid argon and assigned to absorption by the analogue of the first argon excimer continuum. For not perfectly cleaned argon a strong influence of impurities on the transmission is observed. Two strong absorption bands at 126.5 and 141.0 nm with approximately 2 and 4 nm width, respectively, are assigned to traces of xenon in argon. A broad absorption region below 180 nm is found for unpurified argon and tentatively attributed to the presence of water in the argon sample. Xenon (dpeaa)DE-He213 Krypton (dpeaa)DE-He213 Liquid Argon (dpeaa)DE-He213 Attenuation Length (dpeaa)DE-He213 Deuterium Lamp (dpeaa)DE-He213 Hofmann, M. verfasserin aut Oberauer, L. verfasserin aut Potzel, W. verfasserin aut Schönert, S. verfasserin aut Dandl, T. verfasserin aut Heindl, T. verfasserin aut Ulrich, A. verfasserin aut Wieser, J. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 72(2012), 10 vom: 25. Okt. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:72 year:2012 number:10 day:25 month:10 https://dx.doi.org/10.1140/epjc/s10052-012-2190-z kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_63 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_206 GBV_ILN_267 GBV_ILN_293 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_4012 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4305 GBV_ILN_4307 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4338 33.50 ASE AR 72 2012 10 25 10 |
allfieldsGer |
10.1140/epjc/s10052-012-2190-z doi (DE-627)SPR00832705X (SPR)s10052-012-2190-z-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Neumeier, A. verfasserin aut Attenuation of vacuum ultraviolet light in liquid argon 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The transmission of liquid argon has been measured, wavelength resolved, for a wavelength interval from 118 to 250 nm. The wavelength dependent attenuation length is presented for pure argon. It is shown that no universal wavelength independent attenuation length can be assigned to liquid argon for its own fluorescence light due to the interplay between the wavelength dependent emission and absorption. A decreasing transmission is observed below 130 nm in both chemically cleaned and distilled liquid argon and assigned to absorption by the analogue of the first argon excimer continuum. For not perfectly cleaned argon a strong influence of impurities on the transmission is observed. Two strong absorption bands at 126.5 and 141.0 nm with approximately 2 and 4 nm width, respectively, are assigned to traces of xenon in argon. A broad absorption region below 180 nm is found for unpurified argon and tentatively attributed to the presence of water in the argon sample. Xenon (dpeaa)DE-He213 Krypton (dpeaa)DE-He213 Liquid Argon (dpeaa)DE-He213 Attenuation Length (dpeaa)DE-He213 Deuterium Lamp (dpeaa)DE-He213 Hofmann, M. verfasserin aut Oberauer, L. verfasserin aut Potzel, W. verfasserin aut Schönert, S. verfasserin aut Dandl, T. verfasserin aut Heindl, T. verfasserin aut Ulrich, A. verfasserin aut Wieser, J. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 72(2012), 10 vom: 25. Okt. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:72 year:2012 number:10 day:25 month:10 https://dx.doi.org/10.1140/epjc/s10052-012-2190-z kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_63 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_206 GBV_ILN_267 GBV_ILN_293 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_4012 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4305 GBV_ILN_4307 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4338 33.50 ASE AR 72 2012 10 25 10 |
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10.1140/epjc/s10052-012-2190-z doi (DE-627)SPR00832705X (SPR)s10052-012-2190-z-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Neumeier, A. verfasserin aut Attenuation of vacuum ultraviolet light in liquid argon 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The transmission of liquid argon has been measured, wavelength resolved, for a wavelength interval from 118 to 250 nm. The wavelength dependent attenuation length is presented for pure argon. It is shown that no universal wavelength independent attenuation length can be assigned to liquid argon for its own fluorescence light due to the interplay between the wavelength dependent emission and absorption. A decreasing transmission is observed below 130 nm in both chemically cleaned and distilled liquid argon and assigned to absorption by the analogue of the first argon excimer continuum. For not perfectly cleaned argon a strong influence of impurities on the transmission is observed. Two strong absorption bands at 126.5 and 141.0 nm with approximately 2 and 4 nm width, respectively, are assigned to traces of xenon in argon. A broad absorption region below 180 nm is found for unpurified argon and tentatively attributed to the presence of water in the argon sample. Xenon (dpeaa)DE-He213 Krypton (dpeaa)DE-He213 Liquid Argon (dpeaa)DE-He213 Attenuation Length (dpeaa)DE-He213 Deuterium Lamp (dpeaa)DE-He213 Hofmann, M. verfasserin aut Oberauer, L. verfasserin aut Potzel, W. verfasserin aut Schönert, S. verfasserin aut Dandl, T. verfasserin aut Heindl, T. verfasserin aut Ulrich, A. verfasserin aut Wieser, J. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 72(2012), 10 vom: 25. Okt. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:72 year:2012 number:10 day:25 month:10 https://dx.doi.org/10.1140/epjc/s10052-012-2190-z kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_63 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_206 GBV_ILN_267 GBV_ILN_293 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_4012 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4305 GBV_ILN_4307 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4338 33.50 ASE AR 72 2012 10 25 10 |
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530 ASE 33.50 bkl Attenuation of vacuum ultraviolet light in liquid argon Xenon (dpeaa)DE-He213 Krypton (dpeaa)DE-He213 Liquid Argon (dpeaa)DE-He213 Attenuation Length (dpeaa)DE-He213 Deuterium Lamp (dpeaa)DE-He213 |
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Attenuation of vacuum ultraviolet light in liquid argon |
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Attenuation of vacuum ultraviolet light in liquid argon |
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Neumeier, A. |
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Neumeier, A. Hofmann, M. Oberauer, L. Potzel, W. Schönert, S. Dandl, T. Heindl, T. Ulrich, A. Wieser, J. |
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attenuation of vacuum ultraviolet light in liquid argon |
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Attenuation of vacuum ultraviolet light in liquid argon |
abstract |
Abstract The transmission of liquid argon has been measured, wavelength resolved, for a wavelength interval from 118 to 250 nm. The wavelength dependent attenuation length is presented for pure argon. It is shown that no universal wavelength independent attenuation length can be assigned to liquid argon for its own fluorescence light due to the interplay between the wavelength dependent emission and absorption. A decreasing transmission is observed below 130 nm in both chemically cleaned and distilled liquid argon and assigned to absorption by the analogue of the first argon excimer continuum. For not perfectly cleaned argon a strong influence of impurities on the transmission is observed. Two strong absorption bands at 126.5 and 141.0 nm with approximately 2 and 4 nm width, respectively, are assigned to traces of xenon in argon. A broad absorption region below 180 nm is found for unpurified argon and tentatively attributed to the presence of water in the argon sample. |
abstractGer |
Abstract The transmission of liquid argon has been measured, wavelength resolved, for a wavelength interval from 118 to 250 nm. The wavelength dependent attenuation length is presented for pure argon. It is shown that no universal wavelength independent attenuation length can be assigned to liquid argon for its own fluorescence light due to the interplay between the wavelength dependent emission and absorption. A decreasing transmission is observed below 130 nm in both chemically cleaned and distilled liquid argon and assigned to absorption by the analogue of the first argon excimer continuum. For not perfectly cleaned argon a strong influence of impurities on the transmission is observed. Two strong absorption bands at 126.5 and 141.0 nm with approximately 2 and 4 nm width, respectively, are assigned to traces of xenon in argon. A broad absorption region below 180 nm is found for unpurified argon and tentatively attributed to the presence of water in the argon sample. |
abstract_unstemmed |
Abstract The transmission of liquid argon has been measured, wavelength resolved, for a wavelength interval from 118 to 250 nm. The wavelength dependent attenuation length is presented for pure argon. It is shown that no universal wavelength independent attenuation length can be assigned to liquid argon for its own fluorescence light due to the interplay between the wavelength dependent emission and absorption. A decreasing transmission is observed below 130 nm in both chemically cleaned and distilled liquid argon and assigned to absorption by the analogue of the first argon excimer continuum. For not perfectly cleaned argon a strong influence of impurities on the transmission is observed. Two strong absorption bands at 126.5 and 141.0 nm with approximately 2 and 4 nm width, respectively, are assigned to traces of xenon in argon. A broad absorption region below 180 nm is found for unpurified argon and tentatively attributed to the presence of water in the argon sample. |
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Attenuation of vacuum ultraviolet light in liquid argon |
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