In this exploration, we present a compact and easy-to-set imaging system to analyze the quantitative phase information of macroscopic and microscopic transparent phase samples using a radial shearing interferometric design. The proposed setup introduces a wire-grid polarizer as a beam-splitting optical element in a triangular cyclic configuration to render the two counter-propagating beams linearly polarized in orthogonal directions. These beams are made to pass through the samples in a counter direction. The focusing lens to image the sample is aligned in such a way that either the p-polarized beam illuminates the phase sample in a focused position concerning the imaging lens position and the remaining s-polarized beam is far apart from its focal length or vice versa. Hence, polarization phase shifting is implemented to generate a three-dimensional phase pattern, which is digitally captured in a charge-coupled device camera to yield the sample phase. The proposed setup is robust and sufficiently tolerant to ambient vibrations and shows encouraging experimental results using the minimum optics.
In the presence of astigmatism, the three-dimensional distribution of rays in the image region passes through two orthogonal lines, the vertical sagittal foci and the horizontal tangential foci. With increasing astigmatic behaviour of the imaging system, the sagittal and tangential foci will be farther removed from each other and the separation between these two planesserves as the measure of astigmatism. Midway between these planes, i.e., corresponding to the defocus term, 𝑊20 = − 𝑊22⁄2 , where 𝑊22 is the co-efficient of astigmatism, the intensity spread is found to be minimum and the transverse plane passing through this point is referred to as the plane of minimum aberration variance. For a diffraction-limited imaging system, the IPSF on this plane is the Airy pattern. In our study, each sector of the azimuthal Walsh aperture is masked by suitably oriented linear polarizers. The polarization phase introduced is a function of the state of polarization (SOP) of the input beam, the transmission axis of orientation of the masking polarizer and the orientation of the analyzer. A feasible method to assess the degree of astigmatic compensation is to compute the IPSF at the plane of minimum astigmatic variance and compare the intensity distribution with that of airy pattern. IPSFs for different values of 𝑊22 are computed with the presence of compensating polarization masked azimuthal Walsh filters at 0° and 90° with input beam parameters a=b=1 , 𝛿 = 90° and analyser kept at a particular angle. The results are compared with IPSFs computed for an unmasked lens and airy pattern.
Imaging of transparent phase samples using a wire grid polarizer (WGP)-based shearing interferometer is demonstrated. The proposed setup employs a WGP as a beam splitter in a triangular cyclic interferometer setup, so that the two counterpropagating beams are rendered linearly polarized in orthogonal directions as they emerge from the interferometer. These sheared waved fronts are made to pass through the phase sample. The magnitude of shear is affected by controlled angular shifts of one mirror about the reference X and Y axes. For each of these directional shears, the polarization phase shifting is implemented so as to generate a three-dimensional phase pattern, which is digitally combined and integrated to yield the sample phase. The proposed setup is robust, sufficiently tolerant to ambient vibrations, and shows very encouraging experimental results.
High-resolution images are essential in many remote sensing applications such as weather prediction, deforestation, crop monitoring, land mapping, urban growth, etc. In these applications, it is necessary to use multiple high-resolution images for proper analysis. These images carry a lot of information; therefore, multiplexing plays an important role for efficient storage of the images. Hence, we provide an idea of multiplexing high-resolution images using amplitude grating. Initially, images are modulated with variable spatial frequencies and orientation angles followed by the addition of modulated spectrums to form a single spectrum plane. The resultant spectrum plane is filtered before transmission to eliminate noise. To optimize storage space, only a part of the filtered spectrum is transmitted. A pixel intensity graph is plotted to identify the location of maximum information of the images, which is required during the retrieval process. The quality of the output images is analyzed by peak signal-to-noise ratio, structural similarity index measurement, and correlation coefficient methods. The entire work is done by simulation software, and we prove that our proposed multiplexing method is suitable for efficient storage of high-resolution images in remote sensing applications.
The development of a laser-based quantitative phase microscope with phase-shifting capability is reported. The proposed arrangement utilizes a suitably converging laser beam to illuminate the sample, a long working distance microscope objective, a wire grid polarizer to generate collinearly propagating and orthogonally polarized sample and reference beams, and polarizing devices for polarization phase shifting. Reorientation of a polarizer will revert the microscope back to a standard bright-field microscope that can be used for viewing the object under test.
Recent developments in the areas of image processing have guided a new paradigm for research work in communication of images over the internet. Hence, secure storage and retrieval of digital images is a demanding task for future communication services. A scheme to securely store and encrypt multiple images using sinusoidal phase grating is highlighted. In the proposed scheme, images are modulated using different spatial frequencies and orientation angles. In addition, images have been encrypted using random phase mask after filtering. In order to avoid any human intervention in the system, an intensity graph is plotted to retrieve the images by applying inverse Fourier transform. Using this method, it is possible to independently store, encrypt, and retrieve multiple images due to absence of aliasing problem.
In this paper, we report an interferometric method to extract the phase information available in a desired band of spatial frequencies. The phase sample is placed in the path of a converging beam of light entering a Mach Zehnder interferometer so that the two Fourier Transform (FT) planes are located in the two interferometer arms. One of the FT planes is filtered by suitable masks so that only the frequencies that are blocked appears in the final interferogram. An imaging lens images the phase object on a CCD. Polarization Phase Shifting is incorporated so that the final frequency filtered image is reconstructed from the four phase shifted interferograms. The interferometer is made to operate in null fringe condition so that residual phase is eliminated. Simulated and experimental results are presented.
Phase retarders normally exhibit strong wavelength dependence. However, for use with polychromatic light, achromatic retarders, which exhibit ideally nearly identical characteristics over a wide wavelength region, are in demand. Designing such a superachromatic retarder is a challenging task for an optical system designer where retardation will be almost constant within a wide range of wavelengths. The present investigation considers a system consisting of wave plates made of different materials, which focus on near-infrared wavelength range, viz. 800 to 2000 nm. Here, a flower pollination algorithm has been used for this nonlinear optimization problem. With the help of the mentioned optimization technique, the optimal values of thicknesses of wave plates are calculated for which the system act as a quarter-wave plate. The obtained result shows a significant improvement in terms of maximum deviation of retardation for the above-mentioned wavelength range. The proposed methodology holds promise for optimizing the design of optical systems.
It is well known that the phase change in total internal reflection (TIR) is a function of the refractive indices of the pair of media involved. The spatial phase variations in a totally internally reflected beam are accurately measured using a Mach Zehnder interferometer employing polarization phase shifting technique. The evaluated phase change is then related to the refractive index variations of the rarer medium. One of the salient features of the proposed technique is that, unlike most interferometric methods where the measured phase is a function of the sample thickness, TIR phase is independent of the sample thickness as long as the evanescent wave field is fully confined within the sample. The theory of the technique is discussed and experimental results showing the three-dimensional profiles of the measured refractive indices and its spatial variations are presented.
An interferometric method for quantitative evaluation of the magnitude and direction of birefringence of an arbitrarily oriented birefringent sample is developed and presented. The analysis shows that full-field analysis of a spatially varying birefringence is possible by suitably combining several interferogram frames obtained by varying the polarization parameters involved. The preliminary experimental result for a uniformly birefringent sample with a known direction of birefringence is presented.
A mathematical model which has been developed for interferometric analysis of birefringent sample is experimentally
verified using a modified Mach – Zehnder arrangement. It is shown that full field analysis of samples with varying
birefringence in magnitude and orientation is possible.
In the present communication, a procedure for the synthesis of an optical finite impulse response (FIR) birefringent filter
generating arbitrary spectral output is presented. The basic filter consists of a cascaded system of n identical retarders
between two polarizers at the two ends. A mathematical model of the optical FIR filter is introduced using the FIR
theory of digital filter design. The parameters determined by the synthesis procedure are the angles of the optic axes of
the individual crystals and the angle of the output polarizer. Classical FIR filter design method along with the optical
backward transfer technique has been used. Two different arbitrarily specified spectral output profiles have been studied.
However, the method is equally applicable for any periodic transfer function whose corresponding impulse response is
real and causal.
The aim of this study is to model edge enhancement effect in purely phase samples. A self compensating interferometer
similar to Sagnac’s, employed with a polarizing beam splitter where two counter propagating orthogonally polarized
mutually coherent beams are modulated by the phase shifts introduced by a phase sample. An afocal imaging system is
used to image the phase sample on the CCD so that one of the images is slightly defocused. Real-time subtraction of two
images results in intensity modulation of phase interfaces.
KEYWORDS: 3D image reconstruction, Digital holography, Holograms, Image enhancement, Charge-coupled devices, Optical simulations, Digital imaging, Holography, Digital recording, Microscopes
A simple edge enhancement technique in the digital holo-microscopy is presented here. In Digital Holo-microscopy
(DHM) the intensity distribution of the CCD is produced by the interference of a plane reference wave and that
scattered by the object. The reconstruction is accomplished by multiplication of the digitally stored hologram with a
digital model of the reference wave and subsequent numerical determination of the diffracted field of the object in a
defined image plane. Hence, a focused and a defocused version of the object may be reconstructed from only one
recorded hologram by varying the reconstruction distance during numerical reconstruction. The edge enhancement
of the object is possible by simply subtracting this numerically reconstructed defocused real image from the focused
real image. It is interesting to note that using this technique edge enhancement technique is possible for amplitude
and phase objects. The simulation and experimental results presented validate our theoretical expectations.
Interference Microscope with exception of the widely used Mirau objective, involves a setup having Michelson
or Mach-Zender Configuration. The present work proposes an in-line interference laser microscope
configuration.
Calibration of phase in spatial light modulators is a prerequisite for applications where a prespecified phase distribution needs to be implemented over the surface of the modulator. The present work proposes a full-field polarization phase shifting interferometric technique, based on the Twyman-Green interferometer, for the purpose.
An interferometric technique for three-dimensional phase measurement of optically transparent microscopic phase samples is presented. An obliquely aligned polarizer-masked cube beam-splitter, an infinity-corrected microscope objective, and a couple of simple polarization phase-shifting components serve as the setup for such a measurement. Surface phase profiles are then extracted using standard phase-shifting algorithms. The salient features of the proposed technique are its simple design, in-line configuration, possibility of integration with standard microscopic systems, and inherent compensation of the substrate phase. Experimental results are presented. The overall lateral magnification is restricted due to the low numerical aperture offered by the microscope objective and cube beam-splitter combination.
Phase retarders usually exhibit strong wavelength dependence. For this paper, the design and characteristics of an achromatic cascaded system of birefringent plates were studied. The combination of three retarders in a series had been previously proposed by Pancharatnam, and he discussed the possibility of fabricating reasonably good achromatic quarter-wave plates with a suitable level of retardance. This combination, however, still shows substantial variation in terms of retardance within 500 to 700 nm. Here, the combination of four plates for the construction of an almost achromatic quarter-wave plate, which has a variation of only ± 1 degree over the wavelength spectrum of 500 to 700 nm, is proposed. Moreover, spherical trigonometric considerations have been used by Pancharatnam for obtaining the transmission characteristics of a cascaded system. We, however, used the succinct and relatively simple Jones matrix formalism to derive a general expression for the equivalent retardation of this combination. The proposed arrangement of four birefringent plates promises better achromatic combinations.
A simple and rugged optical hardware configuration for digital holography of microscopic reflecting structures is presented. The proposed technique employs a cube beam splitter, oriented as in the Gates interferometer, for recording a hologram. The experimental results for the United States Air Force resolution target and the reflection coating of a compact disk are presented. The salient features of the proposed configuration for reflection digital holography are its simplicity and low sensitivity to ambient vibrations.
Birefringent wave plates, often referred to as retarders, generally exhibit a strong wavelength dependence. However, there is a real need for achromatic retarders that exhibit identical characteristics over a broad wavelength range. In this paper, we have studied the design and characteristics of a cascaded system of birefringent plates in the near infrared region. Here we have studied a cascaded system of three birefringent plates using matrix analysis and designed a system which, by suitable reorientation of one of the plates, may perform both as an achromatic quarter-wave plate and half-wave plate, over the wavelength range of 1000 to 1800 nm. An inexpensive design for such an achromatic combination using crystalline quartz is described. The new arrangement of three birefringent plates proposed has the promise of producing achromatic combinations with fairly good accuracy.
A technique is described for the continuous variation of the resultant retardance and effective privileged directions of a cascaded system of three optical retarders. The system consists of a rotatable retarder sandwiched between two fixed, identical, parallel retarders. The primary aim of the study was to develop a simple technique for a variable retarder for monochromatic light, but the robustness of the system for a narrow band on either side of the design wavelength was also studied. Simulated plots show that a linear variation of the effective retardance from 0 to 2 is achievable, as is a linear variation of the effective azimuth from 0 to . It is also shown that these two parameters may be varied independently of each other.
A cube beam splitter (CBS), which is more often used in two beam interferometers to generate orthogonally directed
light beams, can be used to construct a two beam interferometer by aligning its beam-splitting interface parallel to the
direction of propagation of light. The monolithic design of the CBS interferometer renders sufficient immunity to
ambient vibrations and is worth considering as a convenient arrangement for interferometric testing. The proposed set-up
can be used to construct a phase shifting interferometer as well by suitably incorporationg a quarter-wave plate and two
polarizers for polarization phase shifting. It is also shown that the CBS interferometer, in a slightly different testing
configuration, is birefringence sensitive in the sense that the displacement of the fringes is solely dependent on the
birefringence of the sample and not on its surface quality.
Measurement and analysis of birefringence distribution in samples such as silicon wafers, electro-optic crystals and some biological specimens often poses a challenging task. Most of the standard methods for photoelastic analysis are not exactly suited to testing of samples having microscopic dimensions. The present paper proposes an interference microscopic technique where, unlike conventional interference microscopy, both the interference beams are derived from the light transmitted through the sample. As a consequence of this, the surface finish of the sample need not be of the optical order and thickness variations in the sample are not reflected in the results.
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