000062889 001__ 62889 000062889 005__ 20200423204621.0 000062889 0247_ $$2DOI$$a10.1063/1.2963956 000062889 0247_ $$2WOS$$aWOS:000258493900156 000062889 0247_ $$2Handle$$a2128/17121 000062889 037__ $$aPreJuSER-62889 000062889 041__ $$aeng 000062889 082__ $$a530 000062889 084__ $$2WoS$$aPhysics, Applied 000062889 1001_ $$0P:(DE-Juel1)VDB34109$$aTschersich, K. G.$$b0$$uFZJ 000062889 245__ $$aDesign and characterization of a thermal hydrogen atom source 000062889 260__ $$aMelville, NY$$bAmerican Institute of Physics$$c2008 000062889 300__ $$a034908 000062889 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article 000062889 3367_ $$2DataCite$$aOutput Types/Journal article 000062889 3367_ $$00$$2EndNote$$aJournal Article 000062889 3367_ $$2BibTeX$$aARTICLE 000062889 3367_ $$2ORCID$$aJOURNAL_ARTICLE 000062889 3367_ $$2DRIVER$$aarticle 000062889 440_0 $$03051$$aJournal of Applied Physics$$v104$$x0021-8979 000062889 500__ $$aRecord converted from VDB: 12.11.2012 000062889 520__ $$aThe hydrogen atom source considered here incorporates a hot capillary fed by hydrogen gas. Our earlier measurements on a source heated by electron bombardment are interpreted in terms of a simple model which encourages us to design a source heated by the radiation from a filament. The radiatively heated source is much simpler, more reliable, and easier to run than the electronically heated source. Furthermore, the radiatively heated source is free of any energetic particles. In order to obtain quantitative data on the intensity, an apparatus is constructed revealing the angular distribution of the hydrogen atoms and molecules by means of a quadrupole mass analyzer. The intensity of the source is controlled by the mass flow rate of the feed gas and the electric power to the filament. The flux density of hydrogen atoms at a substrate 6 cm away from the source is variable over two orders of magnitude and extends up to some 10(15) atoms/cm(2) s. (C) 2008 American Institute of Physics. 000062889 536__ $$0G:(DE-Juel1)FUEK414$$2G:(DE-HGF)$$aKondensierte Materie$$cP54$$x0 000062889 588__ $$aDataset connected to Web of Science 000062889 650_7 $$2WoSType$$aJ 000062889 7001_ $$0P:(DE-Juel1)VDB77155$$aFleischhauer, J.P.$$b1$$uFZJ 000062889 7001_ $$0P:(DE-HGF)0$$aSchuler, H.$$b2 000062889 773__ $$0PERI:(DE-600)1476463-5$$a10.1063/1.2963956$$gVol. 104, p. 034908$$p034908$$q104<034908$$tJournal of applied physics$$v104$$x0021-8979$$y2008 000062889 8567_ $$uhttp://dx.doi.org/10.1063/1.2963956 000062889 8564_ $$uhttps://juser.fz-juelich.de/record/62889/files/1.2963956.pdf$$yOpenAccess 000062889 8564_ $$uhttps://juser.fz-juelich.de/record/62889/files/1.2963956.gif?subformat=icon$$xicon$$yOpenAccess 000062889 8564_ $$uhttps://juser.fz-juelich.de/record/62889/files/1.2963956.jpg?subformat=icon-180$$xicon-180$$yOpenAccess 000062889 8564_ $$uhttps://juser.fz-juelich.de/record/62889/files/1.2963956.jpg?subformat=icon-700$$xicon-700$$yOpenAccess 000062889 8564_ $$uhttps://juser.fz-juelich.de/record/62889/files/1.2963956.pdf?subformat=pdfa$$xpdfa$$yOpenAccess 000062889 909CO $$ooai:juser.fz-juelich.de:62889$$pdnbdelivery$$pdriver$$pVDB$$popen_access$$popenaire 000062889 9131_ $$0G:(DE-Juel1)FUEK414$$bMaterie$$kP54$$lKondensierte Materie$$vKondensierte Materie$$x0$$zentfällt bis 2009 000062889 9141_ $$y2008 000062889 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess 000062889 915__ $$0StatID:(DE-HGF)0010$$aJCR/ISI refereed 000062889 9201_ $$0I:(DE-Juel1)VDB802$$d31.12.2010$$gIBN$$kIBN-4$$lBiomechanik$$x0 000062889 970__ $$aVDB:(DE-Juel1)99802 000062889 9801_ $$aFullTexts 000062889 980__ $$aVDB 000062889 980__ $$aConvertedRecord 000062889 980__ $$ajournal 000062889 980__ $$aI:(DE-Juel1)ICS-7-20110106 000062889 980__ $$aUNRESTRICTED 000062889 981__ $$aI:(DE-Juel1)IBI-2-20200312 000062889 981__ $$aI:(DE-Juel1)ICS-7-20110106