By Natan T. Shaked, Zeev Zalevsky, Lisa L Satterwhite

ISBN-10: 0124158714

ISBN-13: 9780124158719

Written via top optical part microscopy specialists, this ebook is a accomplished connection with part microscopy and nanoscopy ideas for biomedical functions, together with differential interference distinction (DIC) microscopy, part distinction microscopy, electronic holographic microscopy, optical coherence tomography, tomographic section microscopy, spectral-domain section detection, and nanoparticle utilization for part nanoscopy

The Editors exhibit biomedical and optical engineers how you can use section microscopy for visualizing unstained specimens, and help the theoretical insurance with utilized content material and examples on designing platforms and analyzing ends up in bio- and nanoscience applications.

  • Provides a finished evaluate of the rules and methods of optical part microscopy and nanoscopy with biomedical applications.
  • Tips/advice on construction structures and dealing with complex imaging biomedical innovations, together with  interpretation of part photos, and methods for quantitative research in line with section microscopy.
  • Interdisciplinary technique that mixes optical engineering, nanotechnology, biology and scientific facets of this subject. each one chapter includes sensible implementations and labored examples.

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Extra info for Biomedical Optical Phase Microscopy and Nanoscopy

Example text

Let us consider a simplified sample with a binary gradient magnitude distribution such that half of the sample has a gradient magnitude of 1γ and the other half has a phase difference of 2γ (see Eq. 2)). The shear and gradient directions of the sample are parallel (θ 5 0 ). 13) C5 Imax 1 Imin where Imax and Imin are the maximal and minimal intensities in the image. 4 Contrast as a function of the sample optical path difference at biases 1/20th the wavelength (A) and quarter wavelength (B). The green color illustrates a case without depolarization (infinity extinction) and the red one corresponds to extinction 100.

Yatagai, A new method of three-dimensional measurement by differential interference contrast microscope, Opt. Commun. 260 (2006) 117. [18] H. Ishiwata, M. Itoh, T. Yatagai, A new analysis for extending the measurement range of the retardationmodulated differential interference contrast (RM-DIC) microscope, Opt. Commun. 281 (2008) 1412. [19] A. Noguchi, H. Ishiwata, M. Itoh, T. Yatagai, Optical sectioning in differential interference contrast microscopy, Opt. Commun. 282 (2009) 3223. [20] M. Shribak, Orientation-independent differential interference contrast microscopy technique and device, US Patent 7233434, (17 December 2003).

3 Bias Optimization In polarization microscopy, the Bra¨ce-Ko¨hler compensator, an azimuthally rotatable birefringent plate with bias retardance up to λ/10, allows investigation of a specimen with small birefringence more precisely than the Senarmont compensator, which has a retardance of λ/4 [7,26]. 028 nm retardation. In order to achieve high sensitivity with the LC-PolScope (a commercially available polarization microscope), we apply alternate bias retardance λ/30 [28,29]. 036 nm. The bias λ/5, which was used for studying a sample with large retardance, produces much higher noise.

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Biomedical Optical Phase Microscopy and Nanoscopy by Natan T. Shaked, Zeev Zalevsky, Lisa L Satterwhite

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