The reflection of long X-rays
Introduction.—For X-rays passing through matter, theory and experiment give a refractive index μ slightly less than unity, so that if a beam of X-rays falls on the plane surface of a solid at a small glancing angle less than the critical glancing angle, it is totally reflected. Determinations of the...
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Veröffentlicht in: | Proceedings of the Royal Society of London. Series A, Containing papers of a mathematical and physical character Containing papers of a mathematical and physical character, 1931-09, Vol.133 (821), p.292-303 |
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description | Introduction.—For X-rays passing through matter, theory and experiment give a refractive index μ slightly less than unity, so that if a beam of X-rays falls on the plane surface of a solid at a small glancing angle less than the critical glancing angle, it is totally reflected. Determinations of the refractive indices of short wave X-rays by the total reflection method have been carried out by a considerable number of observers. The work of Forster and of Doan is of particular importance in that determinations have been made with many refinements of technique for various substances over a range of wave-lengths. |
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The work of Forster and of Doan is of particular importance in that determinations have been made with many refinements of technique for various substances over a range of wave-lengths.</description><identifier>ISSN: 0950-1207</identifier><identifier>EISSN: 2053-9150</identifier><identifier>DOI: 10.1098/rspa.1931.0148</identifier><language>eng</language><publisher>London: The Royal Society</publisher><subject>Calcite ; Density ; Electrons ; Glass ; Mirrors ; Optical reflection ; Quartz ; Silver ; Steels ; Wave reflection</subject><ispartof>Proceedings of the Royal Society of London. 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The work of Forster and of Doan is of particular importance in that determinations have been made with many refinements of technique for various substances over a range of wave-lengths.</description><subject>Calcite</subject><subject>Density</subject><subject>Electrons</subject><subject>Glass</subject><subject>Mirrors</subject><subject>Optical reflection</subject><subject>Quartz</subject><subject>Silver</subject><subject>Steels</subject><subject>Wave reflection</subject><issn>0950-1207</issn><issn>2053-9150</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1931</creationdate><recordtype>article</recordtype><recordid>eNp9j1FLwzAUhYMoOKevPghC_0DrvU2TNI9a1AlDh5viW2jTVDvnOpNOrL_e1spARJ8uuV_OPecQcogQIMj4xLpVGqCkGABG8RYZhMCoL5HBNhmAZOBjCGKX7Dk3B2AMeTwgx7Mn41lTLIyuy2rpVYW3qJaP3oNv08btk50iXThz8D2H5O7ifJaM_PHN5VVyOvZ1hLz2tZEmiygPwwyzUMvI5JqanOeQ5lyKQgueCQwNQIapoSwFiZnWPGO6W2d0SIL-rraVc20ctbLlS2obhaC6cqorp7pyqivXCl57ga2aNlilS1M3al6t7bJ9qtvp5BQlsDektIzDVhRThCgSoVAf5errWsdVy1Xp3Nqo7tdPk9-e9D_PP5Me9aq5qyu76SUZZ6KFfg9LV5v3DUzts-KCCqbu40idTVmC15ORSugnaMqPhg</recordid><startdate>19310901</startdate><enddate>19310901</enddate><creator>Mohr, C. 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A</addtitle><date>1931-09-01</date><risdate>1931</risdate><volume>133</volume><issue>821</issue><spage>292</spage><epage>303</epage><pages>292-303</pages><issn>0950-1207</issn><eissn>2053-9150</eissn><abstract>Introduction.—For X-rays passing through matter, theory and experiment give a refractive index μ slightly less than unity, so that if a beam of X-rays falls on the plane surface of a solid at a small glancing angle less than the critical glancing angle, it is totally reflected. Determinations of the refractive indices of short wave X-rays by the total reflection method have been carried out by a considerable number of observers. The work of Forster and of Doan is of particular importance in that determinations have been made with many refinements of technique for various substances over a range of wave-lengths.</abstract><cop>London</cop><pub>The Royal Society</pub><doi>10.1098/rspa.1931.0148</doi><tpages>12</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Calcite Density Electrons Glass Mirrors Optical reflection Quartz Silver Steels Wave reflection |
title | The reflection of long X-rays |
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