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Digital Holographic Microscopy for Quantitative Visualization
Li, Yan GERI weekly seminar Digital Holographic Microscopy for Quantitative Visualization
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Outline Introduction Quantitative phase-contrast imaging Experiments
Conclusions Future work
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Holography A method for obtaining the amplitude and phase of a wavefield Two-step imaging Recording: interference pattern Reconstruction Digital holography Recording medium: CCD or CMOS camera Reconstruction: numerical algorithms
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General methods Digital holography Phase shifting
Fourier transform analysis Digital holography Numerical reconstruction
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Intensity-contrast image (Photograph)
Amplitude-contrast result Phase-contrast result Hologram
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Macroscopic object Surface roughness
Multiple holograms: wavelength, illumination, refractive index Macroscopic objects may be defined as objects with dimensions at least 4 orders of magnitude greater than the wavelength of the optical field. Because their roughness is comparable to the wavelength of the optical wave, their phase-contrast images consist of values randomly distributed between the range and . Therefore, a point-to-point subtraction of two phase-contrast images is necessary to determine the 3D contours of large objects. The result of this subtraction produces fringes which are absolute contours of surface height above some reference surface. Usually these two phase-contrast images of the same macroscopic object are obtained by using either two different illumination sources, two different wavelengths or two different refractive indices.
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Microscopic objects: Quantitative phase-contrast image from single hologram Amplitude-contrast result Phase-contrast result
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Three contributions to the reconstructed phase
The absolute phase of the object The tilt aberration due to the off-axis geometry and the curvature produced by the microscopic objective Other aberrations or wavefront deformations induced by the setup
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Quantitative phase-contrast imaging
Capturing a reference hologram without the object to compensate the unwanted phase terms Digital phase mask Manually generated 1D fitting procedure 2D fitting procedure
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1D fitting procedure Y = a0 + a1x + a2x2 + b1y + b2y2
Yh = a0 + a1x + a2x2
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2D fitting procedure
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Holographic microscope for reflection imaging
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Holographic microscope for transmission imaging
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Example 1: mirror
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Example 2: resolution test target
Object Standard deviation Max value Min value Mirror Test target The physical resolutions of the bar patterns in ROI are as below: Resolution(line pair per millimetre) Bars with “3” aside 40.32 Bars with “4” aside 45.25 Bars with “5” aside 50.80
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Example 3: bull sperms slide
20x magnification Size of the sperm: about 20~30 microns
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Conclusions Feasibility Advantages Disadvantages
Noncontact, full-field, vibration insensitive, marker free, investigation of dynamic processes Disadvantages Speckles, compromised resolution Approaches to deal with disadvantages Light source Microscope objective with higher magnification
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Future work 2D fitting procedure
Applying digital phase mask in hologram plane Setup for living cell applications Quality microscope objectives with higher magnification Other algorithms for numerical reconstruction
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Thank you! Questions?
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