2006
DOI: 10.1039/b607252f
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X-ray standing waves: a method for thin layered systems

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Cited by 33 publications
(19 citation statements)
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“…The dependence of the primary intensity on the glancing angle and the height in accord with Equations 2.14 and 2.17 can be demonstrated as a threedimensional graph I int (α,z)/I 0 after Krämer et al [10][11][12]. Both functions of intensity 2.14 and 2.17 coincide at the surface of the substrate, that is, for z = 0.…”
Section: Standing Waves In Front Of a Thick Substratementioning
confidence: 83%
“…The dependence of the primary intensity on the glancing angle and the height in accord with Equations 2.14 and 2.17 can be demonstrated as a threedimensional graph I int (α,z)/I 0 after Krämer et al [10][11][12]. Both functions of intensity 2.14 and 2.17 coincide at the surface of the substrate, that is, for z = 0.…”
Section: Standing Waves In Front Of a Thick Substratementioning
confidence: 83%
“…The intensity distribution inside the XSW strongly depends on the incident angle. Thus, angular variation of the emitted fluorescence lines reveals information about the vertical distribution of the element of interest [34,35,36].…”
Section: Txrf Calibration Samplesmentioning
confidence: 99%
“…Adapted from [30]. a handful of studies report on the localization of such light elements by XSW fluorescence [62,66,67]. For example, Zheludeva et al determined the distribution of phosphorus in a relatively thick (N100 nm) protein/ phospholipid film at an air/water interface [67].…”
Section: Light Elements At Soft Interfacesmentioning
confidence: 99%