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Triggering of a pressurized spark gap by a laser beam

A delay line was discharged into a terminating resistor by a spark gap of coaxial design. The spark gap was triggered by a focused laser beam, introduced along the axis; a Q-switched ruby laser giving pulses of 20 ns duration and up to 50 MW power was used. The range of operation of the gap, formati...

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Detalles Bibliográficos
Autor principal: Deutsch, F
Lenguaje:eng
Publicado: 1968
Materias:
Acceso en línea:https://dx.doi.org/10.1088/0022-3727/1/12/317
http://cds.cern.ch/record/2259720
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author Deutsch, F
author_facet Deutsch, F
author_sort Deutsch, F
collection CERN
description A delay line was discharged into a terminating resistor by a spark gap of coaxial design. The spark gap was triggered by a focused laser beam, introduced along the axis; a Q-switched ruby laser giving pulses of 20 ns duration and up to 50 MW power was used. The range of operation of the gap, formative time of the breakdown and jitter were investigated for different gases at pressures above atmospheric, gap widths of 4-10 mm and voltages of up to 120 kv. Mixtures of argon and nitrogen were found to have certain advantages, such as a low threshold for ionization by the laser beam, sufficient dielectric strength, low values of the formative-time jitter and chemical inertness. Formative times of down to about 1 ns and jitters below 1 ns were found. The laser power can be relatively low (0centerdot5-5 MW). An explanation for the breakdown mechanism is proposed.
id oai-inspirehep.net-1591391
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1968
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spelling oai-inspirehep.net-15913912019-09-30T06:29:59Zdoi:10.1088/0022-3727/1/12/317http://cds.cern.ch/record/2259720engDeutsch, FTriggering of a pressurized spark gap by a laser beamDetectors and Experimental TechniquesA delay line was discharged into a terminating resistor by a spark gap of coaxial design. The spark gap was triggered by a focused laser beam, introduced along the axis; a Q-switched ruby laser giving pulses of 20 ns duration and up to 50 MW power was used. The range of operation of the gap, formative time of the breakdown and jitter were investigated for different gases at pressures above atmospheric, gap widths of 4-10 mm and voltages of up to 120 kv. Mixtures of argon and nitrogen were found to have certain advantages, such as a low threshold for ionization by the laser beam, sufficient dielectric strength, low values of the formative-time jitter and chemical inertness. Formative times of down to about 1 ns and jitters below 1 ns were found. The laser power can be relatively low (0centerdot5-5 MW). An explanation for the breakdown mechanism is proposed.oai:inspirehep.net:15913911968
spellingShingle Detectors and Experimental Techniques
Deutsch, F
Triggering of a pressurized spark gap by a laser beam
title Triggering of a pressurized spark gap by a laser beam
title_full Triggering of a pressurized spark gap by a laser beam
title_fullStr Triggering of a pressurized spark gap by a laser beam
title_full_unstemmed Triggering of a pressurized spark gap by a laser beam
title_short Triggering of a pressurized spark gap by a laser beam
title_sort triggering of a pressurized spark gap by a laser beam
topic Detectors and Experimental Techniques
url https://dx.doi.org/10.1088/0022-3727/1/12/317
http://cds.cern.ch/record/2259720
work_keys_str_mv AT deutschf triggeringofapressurizedsparkgapbyalaserbeam