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Volumn 18, Issue 13, 2010, Pages 13492-13501

Sub-15 nm beam confinement by two crossed x-ray waveguides

Author keywords

[No Author keywords available]

Indexed keywords

HOLOGRAPHIC INTERFEROMETRY;

EID: 77953866569     PISSN: None     EISSN: 10944087     Source Type: Journal    
DOI: 10.1364/OE.18.013492     Document Type: Article
Times cited : (35)

References (23)
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    • Hard X-ray microscopy with reflecting mirrors status and perspectives of the ESRF technology
    • O. Hignette, P. Cloetens, W.-K. Lee, W. Ludwig, and G. Rostaing, "Hard X-ray microscopy with reflecting mirrors status and perspectives of the ESRF technology," J. Phys. IV France 104, 231-234 (2003).
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    • Hignette, O.1    Cloetens, P.2    Lee, W.-K.3    Ludwig, W.4    Rostaing, G.5
  • 8
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    • Soft X-ray microscopy at a spatial resolution better than 15 nm
    • W. Chao, B. D. Harteneck, J. A. Liddle, E. H. Anderson, and D. T. Attwood, "Soft X-ray microscopy at a spatial resolution better than 15 nm," Nature 435, 1210-1213 (2005).
    • (2005) Nature , vol.435 , pp. 1210-1213
    • Chao, W.1    Harteneck, B.D.2    Liddle, J.A.3    Anderson, E.H.4    Attwood, D.T.5
  • 11
    • 70349665354 scopus 로고    scopus 로고
    • Demonstration of 12 nm Resolution Fresnel Zone Plate Lens based Soft X-ray Microscopy
    • W. Chao, J. Kim, S. Rekawa, P. Fischer, and E. H. Anderson, "Demonstration of 12 nm Resolution Fresnel Zone Plate Lens based Soft X-ray Microscopy," Opt. Express 17, 17669-17677 (2009).
    • (2009) Opt. Express , vol.17 , pp. 17669-17677
    • Chao, W.1    Kim, J.2    Rekawa, S.3    Fischer, P.4    Anderson, E.H.5
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    • Phase retrieval algorithms: A comparison
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    • Finite-difference field calculations for one-dimensionally confined X-ray waveguides
    • C. Fuhse and T. Salditt, "Finite-difference field calculations for one-dimensionally confined X-ray waveguides," Physica B: Condensed Matter 357, 57-60 (2005).
    • (2005) Physica B: Condensed Matter , vol.357 , pp. 57-60
    • Fuhse, C.1    Salditt, T.2
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    • A minor difference with respect to one of the four parameters was the following: The detector area used for the reconstruction shown in Fig. 4 was 256 x 241 pixels, for the simulation we have used a square area of 248 x 248 pixels with the same pixel size as in the experiment
    • A minor difference with respect to one of the four parameters was the following: The detector area used for the reconstruction shown in Fig. 4 was 256 x 241 pixels, for the simulation we have used a square area of 248 x 248 pixels with the same pixel size as in the experiment.


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