H − and D − production by backscattering from alkali-metal targets
Measurements have been made of the total backscattered D -- and H -- yields from thick, clean targets of Cs, Rb, potassium, Na and Li, bombarded with H+2, H+3, D+2, D+3 with incident energies from 0.15 to 4.0 keV/nucleus. For each target, the H -- and D -- yields exhibited max. (as high as 0.08/inci...
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Veröffentlicht in: | Physical review. B, Condensed matter Condensed matter, 1981-02, Vol.23 (3), p.941-948 |
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creator | Schneider, P. J. Berkner, K. H. Graham, W. G. Pyle, R. V. Stearns, J. W. |
description | Measurements have been made of the total backscattered D -- and H -- yields from thick, clean targets of Cs, Rb, potassium, Na and Li, bombarded with H+2, H+3, D+2, D+3 with incident energies from 0.15 to 4.0 keV/nucleus. For each target, the H -- and D -- yields exhibited max. (as high as 0.08/incident proton and deuteron) at incident energies between 0.3 and 1.4 keV/nucleus. For both hydrogen and deuterium incident at any energy, the negative-ion yield decreases in going from Cs to Li in the order given above. Also, a definite isotope effect was observed for every target used, with the H -- yield peaking at a lower incident energy than the D -- yield and, in most cases, the max. H -- yield was higher than the max. D -- yield. Measurements of the D -- yield as a function of Cs coverage were also made for D+3 bombarding a Ni substrate. The D -- yield maximized at or near the coverage at which the surface work function reached a min.21 refs.--AA |
doi_str_mv | 10.1103/PhysRevB.23.941 |
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J. ; Berkner, K. H. ; Graham, W. G. ; Pyle, R. V. ; Stearns, J. W.</creator><creatorcontrib>Schneider, P. J. ; Berkner, K. H. ; Graham, W. G. ; Pyle, R. V. ; Stearns, J. W.</creatorcontrib><description>Measurements have been made of the total backscattered D -- and H -- yields from thick, clean targets of Cs, Rb, potassium, Na and Li, bombarded with H+2, H+3, D+2, D+3 with incident energies from 0.15 to 4.0 keV/nucleus. For each target, the H -- and D -- yields exhibited max. (as high as 0.08/incident proton and deuteron) at incident energies between 0.3 and 1.4 keV/nucleus. For both hydrogen and deuterium incident at any energy, the negative-ion yield decreases in going from Cs to Li in the order given above. Also, a definite isotope effect was observed for every target used, with the H -- yield peaking at a lower incident energy than the D -- yield and, in most cases, the max. H -- yield was higher than the max. D -- yield. Measurements of the D -- yield as a function of Cs coverage were also made for D+3 bombarding a Ni substrate. The D -- yield maximized at or near the coverage at which the surface work function reached a min.21 refs.--AA</description><identifier>ISSN: 0163-1829</identifier><identifier>DOI: 10.1103/PhysRevB.23.941</identifier><language>eng</language><ispartof>Physical review. B, Condensed matter, 1981-02, Vol.23 (3), p.941-948</ispartof><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c270t-5f33d6cf1b52dfa0d7c7464608d73e4941f0e3a5336f4b648196827b5a9154313</citedby><cites>FETCH-LOGICAL-c270t-5f33d6cf1b52dfa0d7c7464608d73e4941f0e3a5336f4b648196827b5a9154313</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,2863,2864,27901,27902</link.rule.ids></links><search><creatorcontrib>Schneider, P. 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Also, a definite isotope effect was observed for every target used, with the H -- yield peaking at a lower incident energy than the D -- yield and, in most cases, the max. H -- yield was higher than the max. D -- yield. Measurements of the D -- yield as a function of Cs coverage were also made for D+3 bombarding a Ni substrate. 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W.</creatorcontrib><collection>CrossRef</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><jtitle>Physical review. B, Condensed matter</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Schneider, P. J.</au><au>Berkner, K. H.</au><au>Graham, W. G.</au><au>Pyle, R. V.</au><au>Stearns, J. W.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>H − and D − production by backscattering from alkali-metal targets</atitle><jtitle>Physical review. B, Condensed matter</jtitle><date>1981-02-01</date><risdate>1981</risdate><volume>23</volume><issue>3</issue><spage>941</spage><epage>948</epage><pages>941-948</pages><issn>0163-1829</issn><abstract>Measurements have been made of the total backscattered D -- and H -- yields from thick, clean targets of Cs, Rb, potassium, Na and Li, bombarded with H+2, H+3, D+2, D+3 with incident energies from 0.15 to 4.0 keV/nucleus. For each target, the H -- and D -- yields exhibited max. (as high as 0.08/incident proton and deuteron) at incident energies between 0.3 and 1.4 keV/nucleus. For both hydrogen and deuterium incident at any energy, the negative-ion yield decreases in going from Cs to Li in the order given above. Also, a definite isotope effect was observed for every target used, with the H -- yield peaking at a lower incident energy than the D -- yield and, in most cases, the max. H -- yield was higher than the max. D -- yield. Measurements of the D -- yield as a function of Cs coverage were also made for D+3 bombarding a Ni substrate. The D -- yield maximized at or near the coverage at which the surface work function reached a min.21 refs.--AA</abstract><doi>10.1103/PhysRevB.23.941</doi><tpages>8</tpages></addata></record> |
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title | H − and D − production by backscattering from alkali-metal targets |
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