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Coherent diffractive imaging (CDI) is a "lensless" technique for 2D or 3D reconstruction of the image of nanoscale structures such as nanotubes, nanocrystals, porous nanocrystalline layers, defects, potentially proteins, and more. In CDI, a highly coherent beam of X-rays, electrons or other wavelike particle or photon is incident on an object.

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  • Coherent diffraction imaging (en)
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  • Coherent diffractive imaging (CDI) is a "lensless" technique for 2D or 3D reconstruction of the image of nanoscale structures such as nanotubes, nanocrystals, porous nanocrystalline layers, defects, potentially proteins, and more. In CDI, a highly coherent beam of X-rays, electrons or other wavelike particle or photon is incident on an object. (en)
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  • http://commons.wikimedia.org/wiki/Special:FilePath/CNT_CDI_Reconstruction.png
  • http://commons.wikimedia.org/wiki/Special:FilePath/DWCNT_CDI_Reconstruction.png
  • http://commons.wikimedia.org/wiki/Special:FilePath/Lrec_17-1.png
  • http://commons.wikimedia.org/wiki/Special:FilePath/Wikipedia_1_(a)_Volume_representation_of_a_particle_formed_by_a_collection_of_octahedral_Si_nanoparticles,_(b)_The_central_slice_showing_the_high_degree_of_porosity._.jpg
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  • Coherent diffractive imaging (CDI) is a "lensless" technique for 2D or 3D reconstruction of the image of nanoscale structures such as nanotubes, nanocrystals, porous nanocrystalline layers, defects, potentially proteins, and more. In CDI, a highly coherent beam of X-rays, electrons or other wavelike particle or photon is incident on an object. The beam scattered by the object produces a diffraction pattern downstream which is then collected by a detector. This recorded pattern is then used to reconstruct an image via an iterative feedback algorithm. Effectively, the objective lens in a typical microscope is replaced with software to convert from the reciprocal space diffraction pattern into a real space image. The advantage in using no lenses is that the final image is aberration–free and so resolution is only diffraction and dose limited (dependent on wavelength, aperture size and exposure). Applying a simple inverse Fourier transform to information with only intensities is insufficient for creating an image from the diffraction pattern due to the missing phase information. This is called the phase problem. (en)
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