On the Stark broadening of the 537.8 nm and 441.6 nm $ Cd^{+} $ lines excited in a hollow cathode laser discharge

Abstract On the basis of available experimental and theoretical data the role of the Stark effect in the homogeneous line broadening of the green and blue laser lines in a hollow cathode He-$ Cd^{+} $ laser discharge is discussed. It is found, that at typical laser discharge parameters, for the 538...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Csillag, L. [verfasserIn] Dimitrijević, M.S.

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2003

Schlagwörter:	Single Mode Mode Operation Green Line Neutral Atom Laser Line

Anmerkung:	© Springer-Verlag 2003

Übergeordnetes Werk:	Enthalten in: Applied physics - Berlin : Springer, 1981, 78(2003), 2 vom: 19. Dez., Seite 221-223
Übergeordnetes Werk:	volume:78 ; year:2003 ; number:2 ; day:19 ; month:12 ; pages:221-223

Links:	Volltext

DOI / URN:	10.1007/s00340-003-1368-3

Katalog-ID:	SPR004204778

Internformat


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245	1	0	\|a On the Stark broadening of the 537.8 nm and 441.6 nm $ Cd^{+} $ lines excited in a hollow cathode laser discharge
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520			\|a Abstract On the basis of available experimental and theoretical data the role of the Stark effect in the homogeneous line broadening of the green and blue laser lines in a hollow cathode He-$ Cd^{+} $ laser discharge is discussed. It is found, that at typical laser discharge parameters, for the 538 nm line the Stark line-width amounts to $ Δν_{s} $(538 nm)=290 MHz, which is comparable with the natural line-width broadened by collisions with neutral atoms $ Δν_{c} $(538 nm)=370 MHz. For the 442 nm line, however, both are significantly smaller: $ Δν_{s} $(442 nm)=83 MHz and $ Δν_{c} $(442 nm)=200 MHz. The increased homogeneous line-width can result in single mode operation for the green line, while for the blue one it does not.
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912			\|a GBV_ILN_90
912			\|a GBV_ILN_95
912			\|a GBV_ILN_100
912			\|a GBV_ILN_101
912			\|a GBV_ILN_105
912			\|a GBV_ILN_110
912			\|a GBV_ILN_120
912			\|a GBV_ILN_138
912			\|a GBV_ILN_150
912			\|a GBV_ILN_151
912			\|a GBV_ILN_152
912			\|a GBV_ILN_161
912			\|a GBV_ILN_170
912			\|a GBV_ILN_171
912			\|a GBV_ILN_187
912			\|a GBV_ILN_206
912			\|a GBV_ILN_213
912			\|a GBV_ILN_224
912			\|a GBV_ILN_230
912			\|a GBV_ILN_250
912			\|a GBV_ILN_267
912			\|a GBV_ILN_281
912			\|a GBV_ILN_285
912			\|a GBV_ILN_293
912			\|a GBV_ILN_370
912			\|a GBV_ILN_602
912			\|a GBV_ILN_636
912			\|a GBV_ILN_702
912			\|a GBV_ILN_2001
912			\|a GBV_ILN_2003
912			\|a GBV_ILN_2004
912			\|a GBV_ILN_2005
912			\|a GBV_ILN_2006
912			\|a GBV_ILN_2007
912			\|a GBV_ILN_2008
912			\|a GBV_ILN_2009
912			\|a GBV_ILN_2010
912			\|a GBV_ILN_2011
912			\|a GBV_ILN_2014
912			\|a GBV_ILN_2015
912			\|a GBV_ILN_2020
912			\|a GBV_ILN_2021
912			\|a GBV_ILN_2025
912			\|a GBV_ILN_2026
912			\|a GBV_ILN_2027
912			\|a GBV_ILN_2031
912			\|a GBV_ILN_2034
912			\|a GBV_ILN_2037
912			\|a GBV_ILN_2038
912			\|a GBV_ILN_2039
912			\|a GBV_ILN_2044
912			\|a GBV_ILN_2048
912			\|a GBV_ILN_2049
912			\|a GBV_ILN_2050
912			\|a GBV_ILN_2055
912			\|a GBV_ILN_2056
912			\|a GBV_ILN_2057
912			\|a GBV_ILN_2059
912			\|a GBV_ILN_2061
912			\|a GBV_ILN_2064
912			\|a GBV_ILN_2065
912			\|a GBV_ILN_2068
912			\|a GBV_ILN_2070
912			\|a GBV_ILN_2086
912			\|a GBV_ILN_2088
912			\|a GBV_ILN_2093
912			\|a GBV_ILN_2106
912			\|a GBV_ILN_2107
912			\|a GBV_ILN_2108
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912			\|a GBV_ILN_2111
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912			\|a GBV_ILN_4335
912			\|a GBV_ILN_4336
912			\|a GBV_ILN_4338
912			\|a GBV_ILN_4393
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951			\|a AR
952			\|d 78 \|j 2003 \|e 2 \|b 19 \|c 12 \|h 221-223

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matchkey_str	article:14320649:2003----::nhsakraeigfh57nad46mdieectdnhlo
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publishDate	2003
allfields	10.1007/s00340-003-1368-3 doi (DE-627)SPR004204778 (SPR)s00340-003-1368-3-e DE-627 ger DE-627 rakwb eng Csillag, L. verfasserin aut On the Stark broadening of the 537.8 nm and 441.6 nm $ Cd^{+} $ lines excited in a hollow cathode laser discharge 2003 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag 2003 Abstract On the basis of available experimental and theoretical data the role of the Stark effect in the homogeneous line broadening of the green and blue laser lines in a hollow cathode He-$ Cd^{+} $ laser discharge is discussed. It is found, that at typical laser discharge parameters, for the 538 nm line the Stark line-width amounts to $ Δν_{s} $(538 nm)=290 MHz, which is comparable with the natural line-width broadened by collisions with neutral atoms $ Δν_{c} $(538 nm)=370 MHz. For the 442 nm line, however, both are significantly smaller: $ Δν_{s} $(442 nm)=83 MHz and $ Δν_{c} $(442 nm)=200 MHz. The increased homogeneous line-width can result in single mode operation for the green line, while for the blue one it does not. Single Mode (dpeaa)DE-He213 Mode Operation (dpeaa)DE-He213 Green Line (dpeaa)DE-He213 Neutral Atom (dpeaa)DE-He213 Laser Line (dpeaa)DE-He213 Dimitrijević, M.S. aut Enthalten in Applied physics Berlin : Springer, 1981 78(2003), 2 vom: 19. Dez., Seite 221-223 (DE-627)253389933 (DE-600)1458437-2 1432-0649 nnns volume:78 year:2003 number:2 day:19 month:12 pages:221-223 https://dx.doi.org/10.1007/s00340-003-1368-3 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 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_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 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_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 78 2003 2 19 12 221-223
spelling	10.1007/s00340-003-1368-3 doi (DE-627)SPR004204778 (SPR)s00340-003-1368-3-e DE-627 ger DE-627 rakwb eng Csillag, L. verfasserin aut On the Stark broadening of the 537.8 nm and 441.6 nm $ Cd^{+} $ lines excited in a hollow cathode laser discharge 2003 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag 2003 Abstract On the basis of available experimental and theoretical data the role of the Stark effect in the homogeneous line broadening of the green and blue laser lines in a hollow cathode He-$ Cd^{+} $ laser discharge is discussed. It is found, that at typical laser discharge parameters, for the 538 nm line the Stark line-width amounts to $ Δν_{s} $(538 nm)=290 MHz, which is comparable with the natural line-width broadened by collisions with neutral atoms $ Δν_{c} $(538 nm)=370 MHz. For the 442 nm line, however, both are significantly smaller: $ Δν_{s} $(442 nm)=83 MHz and $ Δν_{c} $(442 nm)=200 MHz. The increased homogeneous line-width can result in single mode operation for the green line, while for the blue one it does not. Single Mode (dpeaa)DE-He213 Mode Operation (dpeaa)DE-He213 Green Line (dpeaa)DE-He213 Neutral Atom (dpeaa)DE-He213 Laser Line (dpeaa)DE-He213 Dimitrijević, M.S. aut Enthalten in Applied physics Berlin : Springer, 1981 78(2003), 2 vom: 19. Dez., Seite 221-223 (DE-627)253389933 (DE-600)1458437-2 1432-0649 nnns volume:78 year:2003 number:2 day:19 month:12 pages:221-223 https://dx.doi.org/10.1007/s00340-003-1368-3 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 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_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 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_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 78 2003 2 19 12 221-223
allfields_unstemmed	10.1007/s00340-003-1368-3 doi (DE-627)SPR004204778 (SPR)s00340-003-1368-3-e DE-627 ger DE-627 rakwb eng Csillag, L. verfasserin aut On the Stark broadening of the 537.8 nm and 441.6 nm $ Cd^{+} $ lines excited in a hollow cathode laser discharge 2003 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag 2003 Abstract On the basis of available experimental and theoretical data the role of the Stark effect in the homogeneous line broadening of the green and blue laser lines in a hollow cathode He-$ Cd^{+} $ laser discharge is discussed. It is found, that at typical laser discharge parameters, for the 538 nm line the Stark line-width amounts to $ Δν_{s} $(538 nm)=290 MHz, which is comparable with the natural line-width broadened by collisions with neutral atoms $ Δν_{c} $(538 nm)=370 MHz. For the 442 nm line, however, both are significantly smaller: $ Δν_{s} $(442 nm)=83 MHz and $ Δν_{c} $(442 nm)=200 MHz. The increased homogeneous line-width can result in single mode operation for the green line, while for the blue one it does not. Single Mode (dpeaa)DE-He213 Mode Operation (dpeaa)DE-He213 Green Line (dpeaa)DE-He213 Neutral Atom (dpeaa)DE-He213 Laser Line (dpeaa)DE-He213 Dimitrijević, M.S. aut Enthalten in Applied physics Berlin : Springer, 1981 78(2003), 2 vom: 19. Dez., Seite 221-223 (DE-627)253389933 (DE-600)1458437-2 1432-0649 nnns volume:78 year:2003 number:2 day:19 month:12 pages:221-223 https://dx.doi.org/10.1007/s00340-003-1368-3 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 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_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 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_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 78 2003 2 19 12 221-223
allfieldsGer	10.1007/s00340-003-1368-3 doi (DE-627)SPR004204778 (SPR)s00340-003-1368-3-e DE-627 ger DE-627 rakwb eng Csillag, L. verfasserin aut On the Stark broadening of the 537.8 nm and 441.6 nm $ Cd^{+} $ lines excited in a hollow cathode laser discharge 2003 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag 2003 Abstract On the basis of available experimental and theoretical data the role of the Stark effect in the homogeneous line broadening of the green and blue laser lines in a hollow cathode He-$ Cd^{+} $ laser discharge is discussed. It is found, that at typical laser discharge parameters, for the 538 nm line the Stark line-width amounts to $ Δν_{s} $(538 nm)=290 MHz, which is comparable with the natural line-width broadened by collisions with neutral atoms $ Δν_{c} $(538 nm)=370 MHz. For the 442 nm line, however, both are significantly smaller: $ Δν_{s} $(442 nm)=83 MHz and $ Δν_{c} $(442 nm)=200 MHz. The increased homogeneous line-width can result in single mode operation for the green line, while for the blue one it does not. Single Mode (dpeaa)DE-He213 Mode Operation (dpeaa)DE-He213 Green Line (dpeaa)DE-He213 Neutral Atom (dpeaa)DE-He213 Laser Line (dpeaa)DE-He213 Dimitrijević, M.S. aut Enthalten in Applied physics Berlin : Springer, 1981 78(2003), 2 vom: 19. Dez., Seite 221-223 (DE-627)253389933 (DE-600)1458437-2 1432-0649 nnns volume:78 year:2003 number:2 day:19 month:12 pages:221-223 https://dx.doi.org/10.1007/s00340-003-1368-3 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 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_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 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_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 78 2003 2 19 12 221-223
allfieldsSound	10.1007/s00340-003-1368-3 doi (DE-627)SPR004204778 (SPR)s00340-003-1368-3-e DE-627 ger DE-627 rakwb eng Csillag, L. verfasserin aut On the Stark broadening of the 537.8 nm and 441.6 nm $ Cd^{+} $ lines excited in a hollow cathode laser discharge 2003 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer-Verlag 2003 Abstract On the basis of available experimental and theoretical data the role of the Stark effect in the homogeneous line broadening of the green and blue laser lines in a hollow cathode He-$ Cd^{+} $ laser discharge is discussed. It is found, that at typical laser discharge parameters, for the 538 nm line the Stark line-width amounts to $ Δν_{s} $(538 nm)=290 MHz, which is comparable with the natural line-width broadened by collisions with neutral atoms $ Δν_{c} $(538 nm)=370 MHz. For the 442 nm line, however, both are significantly smaller: $ Δν_{s} $(442 nm)=83 MHz and $ Δν_{c} $(442 nm)=200 MHz. The increased homogeneous line-width can result in single mode operation for the green line, while for the blue one it does not. Single Mode (dpeaa)DE-He213 Mode Operation (dpeaa)DE-He213 Green Line (dpeaa)DE-He213 Neutral Atom (dpeaa)DE-He213 Laser Line (dpeaa)DE-He213 Dimitrijević, M.S. aut Enthalten in Applied physics Berlin : Springer, 1981 78(2003), 2 vom: 19. Dez., Seite 221-223 (DE-627)253389933 (DE-600)1458437-2 1432-0649 nnns volume:78 year:2003 number:2 day:19 month:12 pages:221-223 https://dx.doi.org/10.1007/s00340-003-1368-3 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 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_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 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_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 78 2003 2 19 12 221-223
language	English
source	Enthalten in Applied physics 78(2003), 2 vom: 19. Dez., Seite 221-223 volume:78 year:2003 number:2 day:19 month:12 pages:221-223
sourceStr	Enthalten in Applied physics 78(2003), 2 vom: 19. Dez., Seite 221-223 volume:78 year:2003 number:2 day:19 month:12 pages:221-223
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Single Mode Mode Operation Green Line Neutral Atom Laser Line
isfreeaccess_bool	false
container_title	Applied physics
authorswithroles_txt_mv	Csillag, L. @@aut@@ Dimitrijević, M.S. @@aut@@
publishDateDaySort_date	2003-12-19T00:00:00Z
hierarchy_top_id	253389933
id	SPR004204778
language_de	englisch
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author	Csillag, L.
spellingShingle	Csillag, L. misc Single Mode misc Mode Operation misc Green Line misc Neutral Atom misc Laser Line On the Stark broadening of the 537.8 nm and 441.6 nm $ Cd^{+} $ lines excited in a hollow cathode laser discharge
authorStr	Csillag, L.
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topic_title	On the Stark broadening of the 537.8 nm and 441.6 nm $ Cd^{+} $ lines excited in a hollow cathode laser discharge Single Mode (dpeaa)DE-He213 Mode Operation (dpeaa)DE-He213 Green Line (dpeaa)DE-He213 Neutral Atom (dpeaa)DE-He213 Laser Line (dpeaa)DE-He213
topic	misc Single Mode misc Mode Operation misc Green Line misc Neutral Atom misc Laser Line
topic_unstemmed	misc Single Mode misc Mode Operation misc Green Line misc Neutral Atom misc Laser Line
topic_browse	misc Single Mode misc Mode Operation misc Green Line misc Neutral Atom misc Laser Line
format_facet	Elektronische Aufsätze Aufsätze Elektronische Ressource
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title	On the Stark broadening of the 537.8 nm and 441.6 nm $ Cd^{+} $ lines excited in a hollow cathode laser discharge
ctrlnum	(DE-627)SPR004204778 (SPR)s00340-003-1368-3-e
title_full	On the Stark broadening of the 537.8 nm and 441.6 nm $ Cd^{+} $ lines excited in a hollow cathode laser discharge
author_sort	Csillag, L.
journal	Applied physics
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author_browse	Csillag, L. Dimitrijević, M.S.
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author-letter	Csillag, L.
doi_str_mv	10.1007/s00340-003-1368-3
title_sort	on the stark broadening of the 537.8 nm and 441.6 nm $ cd^{+} $ lines excited in a hollow cathode laser discharge
title_auth	On the Stark broadening of the 537.8 nm and 441.6 nm $ Cd^{+} $ lines excited in a hollow cathode laser discharge
abstract	Abstract On the basis of available experimental and theoretical data the role of the Stark effect in the homogeneous line broadening of the green and blue laser lines in a hollow cathode He-$ Cd^{+} $ laser discharge is discussed. It is found, that at typical laser discharge parameters, for the 538 nm line the Stark line-width amounts to $ Δν_{s} $(538 nm)=290 MHz, which is comparable with the natural line-width broadened by collisions with neutral atoms $ Δν_{c} $(538 nm)=370 MHz. For the 442 nm line, however, both are significantly smaller: $ Δν_{s} $(442 nm)=83 MHz and $ Δν_{c} $(442 nm)=200 MHz. The increased homogeneous line-width can result in single mode operation for the green line, while for the blue one it does not. © Springer-Verlag 2003
abstractGer	Abstract On the basis of available experimental and theoretical data the role of the Stark effect in the homogeneous line broadening of the green and blue laser lines in a hollow cathode He-$ Cd^{+} $ laser discharge is discussed. It is found, that at typical laser discharge parameters, for the 538 nm line the Stark line-width amounts to $ Δν_{s} $(538 nm)=290 MHz, which is comparable with the natural line-width broadened by collisions with neutral atoms $ Δν_{c} $(538 nm)=370 MHz. For the 442 nm line, however, both are significantly smaller: $ Δν_{s} $(442 nm)=83 MHz and $ Δν_{c} $(442 nm)=200 MHz. The increased homogeneous line-width can result in single mode operation for the green line, while for the blue one it does not. © Springer-Verlag 2003
abstract_unstemmed	Abstract On the basis of available experimental and theoretical data the role of the Stark effect in the homogeneous line broadening of the green and blue laser lines in a hollow cathode He-$ Cd^{+} $ laser discharge is discussed. It is found, that at typical laser discharge parameters, for the 538 nm line the Stark line-width amounts to $ Δν_{s} $(538 nm)=290 MHz, which is comparable with the natural line-width broadened by collisions with neutral atoms $ Δν_{c} $(538 nm)=370 MHz. For the 442 nm line, however, both are significantly smaller: $ Δν_{s} $(442 nm)=83 MHz and $ Δν_{c} $(442 nm)=200 MHz. The increased homogeneous line-width can result in single mode operation for the green line, while for the blue one it does not. © Springer-Verlag 2003
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container_issue	2
title_short	On the Stark broadening of the 537.8 nm and 441.6 nm $ Cd^{+} $ lines excited in a hollow cathode laser discharge
url	https://dx.doi.org/10.1007/s00340-003-1368-3
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author2	Dimitrijević, M.S.
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doi_str	10.1007/s00340-003-1368-3
up_date	2024-07-04T00:07:16.062Z
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On the Stark broadening of the 537.8 nm and 441.6 nm $ Cd^{+} $ lines excited in a hollow cathode laser discharge

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