1931
DOI: 10.1007/bf01339581
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Zur Theorie der Feinstruktur in den R�ntgenabsorptionsspektren

Abstract: Das Auftreten einer ausgedehnten Sekundiirstruktur in den K-Absorptionsbanden yon I%ristallen und namentlieh yon Metallen im festen Zustand wird in Verbindung gebracht mit der Tatsache, dab das Energiespektrum eines Elektrons, welches sich durch ein periodisches Potentialfeld in einer bestimmten Riehtung bewegt, aus erlaubten und verbotenen Zonen endlicher Breite besteht.Man erhg]t hiermit aueh eine Deutung der yon Hanawalt untersuchten Beeinflussung dieser Sekundgrstruktur dm'ch TemperaturerhShung. Mit tIilfe… Show more

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Cited by 285 publications
(27 citation statements)
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“…In his first work he suggested the long range order (LRO) interpretation of XAFS in crystalline materials; i.e. the fine structure in x-ray absorption is determined by the features of the band structure (Kronig, 1931). In his second paper he developed a short range order (SRO) theory for the molecules within a single scattering plane wave approximation (Kronig,1932).…”
mentioning
confidence: 99%
“…In his first work he suggested the long range order (LRO) interpretation of XAFS in crystalline materials; i.e. the fine structure in x-ray absorption is determined by the features of the band structure (Kronig, 1931). In his second paper he developed a short range order (SRO) theory for the molecules within a single scattering plane wave approximation (Kronig,1932).…”
mentioning
confidence: 99%
“…The fine structure above an absorption edge is known since almost a century. The first observations were made by Fricke [189] and by Hertz [190] and theoretically interpreted by de Kronig [191] involving a long range order theory. It took until the early 1970s of the last century to formulate a correct theory of EXAFS in terms of a short range order [192]: it also established a path for the analysis using the Fourier Transformation (FT) of the χðkÞ function which is defined as χðkÞ ¼ ½μðEÞÀμ 0 ðEÞ=μ 0 ðEÞ, where k represents the wavenumber of the electron at an energy E above E 0 according to the…”
Section: Historical Background and Theorymentioning
confidence: 96%
“…In this way the EXAFS can be interpreted in terms of the number, nature and distance of the backscattering atoms near to the absorbing (target) atom. The XANES structure was first recognised by Kossel (1920) and the EXAFS by Kronig (1931). Although both phenomena have been known for over sixty years, the earlier developments were slow mainly due to the lack of high quality experimental data for comparison with the different theories based on the concepts of the long-range order and short-range order.…”
Section: (A) (B)mentioning
confidence: 99%