The Hydrogen Dissociation Laser
The H2 dissociation laser buffered with argon using electron beam excitation is considered. The argon buffer greatly increases the light output from the upper laser level, compared with pure hydrogen. It does this by absorbing much more of the electron beam energy, and by transferring it more effici...
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creator | Cohn,Arthur Rubin,Allen G Besse,Arthur L |
description | The H2 dissociation laser buffered with argon using electron beam excitation is considered. The argon buffer greatly increases the light output from the upper laser level, compared with pure hydrogen. It does this by absorbing much more of the electron beam energy, and by transferring it more efficiently to the upper laser level. Upper laser level densities of 3 x 10 to the 13th power per cc are experimentally obtained. This should be sufficient for practical gain if auxiliary loss processes such as photoionization absorption do not cancel the gain. This problem has not yet been determined. If these adsorption processes are within estimated bounds, an energy density of approximately 5 joules per liter, over a pulse time of about 10 nsec, at an efficiency of about 10 percent for tunable radiation in the 0.4- to 0.6- micrometer wavelength range is predicted. (Author) |
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The argon buffer greatly increases the light output from the upper laser level, compared with pure hydrogen. It does this by absorbing much more of the electron beam energy, and by transferring it more efficiently to the upper laser level. Upper laser level densities of 3 x 10 to the 13th power per cc are experimentally obtained. This should be sufficient for practical gain if auxiliary loss processes such as photoionization absorption do not cancel the gain. This problem has not yet been determined. If these adsorption processes are within estimated bounds, an energy density of approximately 5 joules per liter, over a pulse time of about 10 nsec, at an efficiency of about 10 percent for tunable radiation in the 0.4- to 0.6- micrometer wavelength range is predicted. (Author)</description><language>eng</language><subject>Dissociation ; Electron irradiation ; Excitation ; Gas lasers ; Hydrogen ; Hydrogen lasers ; Lasers and Masers ; Photoionization ; Visible spectra</subject><creationdate>1974</creationdate><rights>APPROVED FOR PUBLIC RELEASE</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,776,881,27546,27547</link.rule.ids><linktorsrc>$$Uhttps://apps.dtic.mil/sti/citations/AD0780622$$EView_record_in_DTIC$$FView_record_in_$$GDTIC$$Hfree_for_read</linktorsrc></links><search><creatorcontrib>Cohn,Arthur</creatorcontrib><creatorcontrib>Rubin,Allen G</creatorcontrib><creatorcontrib>Besse,Arthur L</creatorcontrib><creatorcontrib>AIR FORCE CAMBRIDGE RESEARCH LABS L G HANSCOM FIELD MASS</creatorcontrib><title>The Hydrogen Dissociation Laser</title><description>The H2 dissociation laser buffered with argon using electron beam excitation is considered. The argon buffer greatly increases the light output from the upper laser level, compared with pure hydrogen. It does this by absorbing much more of the electron beam energy, and by transferring it more efficiently to the upper laser level. Upper laser level densities of 3 x 10 to the 13th power per cc are experimentally obtained. This should be sufficient for practical gain if auxiliary loss processes such as photoionization absorption do not cancel the gain. This problem has not yet been determined. If these adsorption processes are within estimated bounds, an energy density of approximately 5 joules per liter, over a pulse time of about 10 nsec, at an efficiency of about 10 percent for tunable radiation in the 0.4- to 0.6- micrometer wavelength range is predicted. (Author)</description><subject>Dissociation</subject><subject>Electron irradiation</subject><subject>Excitation</subject><subject>Gas lasers</subject><subject>Hydrogen</subject><subject>Hydrogen lasers</subject><subject>Lasers and Masers</subject><subject>Photoionization</subject><subject>Visible spectra</subject><fulltext>true</fulltext><rsrctype>report</rsrctype><creationdate>1974</creationdate><recordtype>report</recordtype><sourceid>1RU</sourceid><recordid>eNrjZJAPyUhV8KhMKcpPT81TcMksLs5PzkwsyczPU_BJLE4t4mFgTUvMKU7lhdLcDDJuriHOHropJZnJ8cUlmXmpJfGOLgbmFgZmRkbGBKQBoNwhsw</recordid><startdate>19740405</startdate><enddate>19740405</enddate><creator>Cohn,Arthur</creator><creator>Rubin,Allen G</creator><creator>Besse,Arthur L</creator><scope>1RU</scope><scope>BHM</scope></search><sort><creationdate>19740405</creationdate><title>The Hydrogen Dissociation Laser</title><author>Cohn,Arthur ; Rubin,Allen G ; Besse,Arthur L</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-dtic_stinet_AD07806223</frbrgroupid><rsrctype>reports</rsrctype><prefilter>reports</prefilter><language>eng</language><creationdate>1974</creationdate><topic>Dissociation</topic><topic>Electron irradiation</topic><topic>Excitation</topic><topic>Gas lasers</topic><topic>Hydrogen</topic><topic>Hydrogen lasers</topic><topic>Lasers and Masers</topic><topic>Photoionization</topic><topic>Visible spectra</topic><toplevel>online_resources</toplevel><creatorcontrib>Cohn,Arthur</creatorcontrib><creatorcontrib>Rubin,Allen G</creatorcontrib><creatorcontrib>Besse,Arthur L</creatorcontrib><creatorcontrib>AIR FORCE CAMBRIDGE RESEARCH LABS L G HANSCOM FIELD MASS</creatorcontrib><collection>DTIC Technical Reports</collection><collection>DTIC STINET</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Cohn,Arthur</au><au>Rubin,Allen G</au><au>Besse,Arthur L</au><aucorp>AIR FORCE CAMBRIDGE RESEARCH LABS L G HANSCOM FIELD MASS</aucorp><format>book</format><genre>unknown</genre><ristype>RPRT</ristype><btitle>The Hydrogen Dissociation Laser</btitle><date>1974-04-05</date><risdate>1974</risdate><abstract>The H2 dissociation laser buffered with argon using electron beam excitation is considered. The argon buffer greatly increases the light output from the upper laser level, compared with pure hydrogen. It does this by absorbing much more of the electron beam energy, and by transferring it more efficiently to the upper laser level. Upper laser level densities of 3 x 10 to the 13th power per cc are experimentally obtained. This should be sufficient for practical gain if auxiliary loss processes such as photoionization absorption do not cancel the gain. This problem has not yet been determined. If these adsorption processes are within estimated bounds, an energy density of approximately 5 joules per liter, over a pulse time of about 10 nsec, at an efficiency of about 10 percent for tunable radiation in the 0.4- to 0.6- micrometer wavelength range is predicted. (Author)</abstract><oa>free_for_read</oa></addata></record> |
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subjects | Dissociation Electron irradiation Excitation Gas lasers Hydrogen Hydrogen lasers Lasers and Masers Photoionization Visible spectra |
title | The Hydrogen Dissociation Laser |
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