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Journal articles on the topic 'Holographic optical component'

Author: Grafiati

Published: 4 June 2021

Last updated: 4 February 2022

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1

Batomunkuev, Yury Ts. "ACHROMATIZATION OF THE VOLUME HOLOGRAPHIC OPTICAL ELEMENS." Interexpo GEO-Siberia 8, no. 1 (2020): 139–45. http://dx.doi.org/10.33764/2618-981x-2020-8-1-139-145.

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The work considers a two-component holographic optical system having a base element in the form of a thick (volume) hologram optical element and intended for use in a given spectral range. The calculation of a two-component holographic system is carried out using formulas obtained from the mirror-lens model of the thick hologram element proposed by the author. It is indicated that according to the mirror model a thick hologram optical element is achromatic in a first approximation. For this the local period of the volume diffraction structure of the hologram element must be many times greater

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2

Chanishvili, A., N. Ponjavidze, G. Petriashvili, et al. "Photo-Induced Holographic Recording in an Optically Active Cholesteric Liquid Crystal Layer." Optical Data Processing and Storage 4, no. 1 (2018): 1–7. http://dx.doi.org/10.1515/odps-2018-0001.

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Abstract A few microns thick layer of an optically active cholesteric liquid crystal is realized by using a photoisomerizable nematic component and a chiral dopant. It is shown that such a photosensitive optically active medium can be used as a holographic material for optical information and dynamic grating recording. The photo-induced gratings are written by exploiting the light-induced photoisomerization phase transition from an optically active chiral liquid crystal to an isotropic liquid, which results in the rotation of the light polarization plane from 90 to 0 degrees and corresponding

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3

Wang Yunxin, 王云新, 王大勇 Wang Dayong, 赵洁 Zhao Jie, 李艳 Li Yan, and 万玉红 Wan Yuhong. "3D Profile Measurement for Micro-Optical Component by Using Digital Holographic Microscopy." Acta Optica Sinica 31, no. 4 (2011): 0412003. http://dx.doi.org/10.3788/aos201131.0412003.

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4

WANG Fan-jing, 王璠璟, 肖文 XIAO Wen, 潘锋 PAN Feng, 丛琳 CONG Lin, and 李建毅 LI Jian-yi. "Digital holographic on-line detection of optic component surface." Optics and Precision Engineering 20, no. 6 (2012): 1182–87. http://dx.doi.org/10.3788/ope.20122006.1182.

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5

Hsu, Chih Wei, Feng Tsai Weng, and Chi Ting Ho. "Using Micro-Pressing Method to Fabricate Bragg Grating on D-Shaped Optical Fiber." Advanced Materials Research 314-316 (August 2011): 1799–805. http://dx.doi.org/10.4028/www.scientific.net/amr.314-316.1799.

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In this paper, we proposed a method to fabricate a D-shaped optical fiber of Bragg surface grating filter component by D-shaped fiber polishing along with photolithography、holographic interference lithography technologies and micro-molding process. The optical fiber was side-polished until it reaches the core of fiber. The master Bragg grating was first fabricated on the positive photoresister by using the holography interference lithography, then the patterned resist was used as a mother mold to transfer the pattern onto a hard polydimethylsiloxane (hPDMS)/ polydimethylsiloxane (PDMS) mold. T

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Hsu, Fang Chang, Farn Tsei Chen, and Chi Ting Ho. "To Fabricate Bragg Grating on D-Shaped Optical Fibre by Micro-Pressing Method." Applied Mechanics and Materials 311 (February 2013): 472–76. http://dx.doi.org/10.4028/www.scientific.net/amm.311.472.

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In this paper, we proposed a method to fabricate a D-shaped optical fiber of Bragg surface grating filter component by D-shaped fiber polishing along with photolithography、holographic interference lithography technologies and micro-molding process. The optical fiber was side-polished until it reaches the core of fiber. The master Bragg grating was first fabricated on the positive photoresister by using the holography interference lithography, then the patterned resist was used as a mother mold to transfer the pattern onto a hard polydimethylsiloxane (hPDMS)/ polydimethylsiloxane (PDMS) mold. T

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7

Coufal, Hans, and Lisa Dhar. "Materials for Optical Data Storage." MRS Bulletin 31, no. 4 (2006): 294–98. http://dx.doi.org/10.1557/mrs2006.67.

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AbstractThe development of recording materials has been a critical component in the advancement of optical data storage. The continual need for improved performance in both consumer and business applications has pushed forward the capabilities of optical storage. In this issue of MRS Bulletin, we review some of the important developments in the materials behind established technologies such as compact discs, digital versatile discs, and magneto-optical recording; the emerging technology of blue recording; and two technologies that seek to extend the performance roadmap for optical storage, mul

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8

Sakhno, Oksana, Pavel Yezhov, Volodymyr Hryn, Valentyn Rudenko, and Tatiana Smirnova. "Optical and Nonlinear Properties of Photonic Polymer Nanocomposites and Holographic Gratings Modified with Noble Metal Nanoparticles." Polymers 12, no. 2 (2020): 480. http://dx.doi.org/10.3390/polym12020480.

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Nanocomposites based on transparent polymer matrices containing nanoparticles (NPs) of noble metals are modern-day materials that can be specially designed for photonics, linear and nonlinear optics, laser physics and sensing applications. We present the improved photosensitive nanocomposites doped with Au and Ag NPs allowing fabrication of high effective submicrometer dimensional diffraction structures using holographic method. A general approach for the fabrication of holographic structures using a two-component mixture of the monomers of different reactivity was developed. Two different met

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9

Mensov, S. N., and Yu V. Polushtaytsev. "Stable holographic lenses formation from multi-component photopolymerizable compositions." Optical Memory and Neural Networks 22, no. 2 (2013): 90–96. http://dx.doi.org/10.3103/s1060992x13020045.

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10

Do, Cuong Manh, and Bahram Javidi. "Multifocus Holographic 3-D Image Fusion Using Independent Component Analysis." Journal of Display Technology 3, no. 3 (2007): 326–32. http://dx.doi.org/10.1109/jdt.2007.900918.

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11

Tang, Min Jin, Hui Min Xie, Jian Guo Zhu, Peng Wan Chen, Qing Ming Zhang, and Xiao Jun Li. "A New Moiré Grating Fabrication Technique Using Hot Embossing Lithography." Applied Mechanics and Materials 83 (July 2011): 7–12. http://dx.doi.org/10.4028/www.scientific.net/amm.83.7.

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Moiré grating is a basic optical component, and can be used in various moiré methods. The conventional grating fabrication technology is based on photolithography and holographic interferometry, however, it requires complex optical components and is very difficult to put into practice. In this study, nanoimprint lithography (NIL), or rather, hot embossing lithography (HEL), is proposed for producing high frequency grating. Compared with silicon mold, holographic moiré grating mold costs less and is not easy to break, thus is chosen to be the mold in HEL. Using this mold and the hot embossing s

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12

Batomunkuev, Yury Ts, and Alexandra A. Pechenkina. "CALCULATION OF THE ACHROMATIC DIFFRACTION SYSTEM WITH CORRECTED SPHERICAL ABERRATION (part 2)." Interexpo GEO-Siberia 8, no. 1 (2020): 127–33. http://dx.doi.org/10.33764/2618-981x-2020-8-1-127-133.

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Achromatization of a three-component diffraction system consisting of one thick and two thin hologram optical elements is considered in the work. Analytical expressions are obtained for correcting the chromatic aberration of the position of a thick focusing hologram optical element by two scattering thin hologram optical elements in a given spectrum range. It is shown that achromatization is achieved for such a three-component system using two thin hologram elements located symmetrically on both sides of the thick element and having a value of the working diffraction order greater than the rat

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13

Ibrahim, Ahmad, Christian Ley, Xavier Allonas, Christiane Carre, and Isabelle Pillin. "Tailoring 3-Component Photoinitiating Systems for Use as Efficient Photopolymerizable Holographic Material." Journal of Display Technology 10, no. 6 (2014): 456–63. http://dx.doi.org/10.1109/jdt.2014.2314863.

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14

RUZAK, O., N. COLLINGS, W. A. CROSSLAND, T. D. WILKINSON, A. B. DAVEY, and I. C. KHOO. "DYNAMIC HOLOGRAPHIC GRATINGS IN METHYL RED-DOPED NEMATIC LIQUID CRYSTALS." Journal of Nonlinear Optical Physics & Materials 12, no. 04 (2003): 441–46. http://dx.doi.org/10.1142/s0218863503001560.

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Orientational photorefractivity in liquid crystals doped with azo dye MR crystals is studied. The experiments are carried out with no voltage applied. Dynamic behavior and its dependence on writing beams intensity are presented. When excited by light, the dye tends to bond to the cell surface. Such an effect is irreversible and leads to the permanent component formation in diffracted signal. This is not beneficial for applications where change of written information is required (OASLMs, dynamic holography, all-optical switching). The process was strongly suppressed and was virtually eliminated

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15

Shin, Sanghoon, and Younghun Yu. "Determining the Refractive Index and Three-Dimensional Shape of an Optical Component using Digital Holographic Microscopy with Liquid." Korean Journal of Optics and Photonics 25, no. 3 (2014): 137–41. http://dx.doi.org/10.3807/kjop.2014.25.3.137.

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16

Rehrauer, Owen G., Vu C. Dinh, Bharat R. Mankani, Gregery T. Buzzard, Bradley J. Lucier, and Dor Ben-Amotz. "Binary Complementary Filters for Compressive Raman Spectroscopy." Applied Spectroscopy 72, no. 1 (2017): 69–78. http://dx.doi.org/10.1177/0003702817732324.

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The previously described optimized binary compressive detection (OB-CD) strategy enables fast hyperspectral Raman (and fluorescence) spectroscopic analysis of systems containing two or more chemical components. However, each OB-CD filter collects only a fraction of the scattered photons and the remainder of the photons are lost. Here, we present a refinement of OB-CD, the OB-CD2 strategy, in which all of the collected Raman photons are detected using a pair of complementary binary optical filters that direct photons of different colors to two photon counting detectors. The OB-CD2 filters are g

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17

Zhang, Heng, Yun Zhou, and Lin Sen Chen. "Fabrication of Micro-Grating Structure on Glazed Stainless-Steel by Two-Beam Holographic Method Using Nanosecond Laser Pulses." Key Engineering Materials 364-366 (December 2007): 1133–37. http://dx.doi.org/10.4028/www.scientific.net/kem.364-366.1133.

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A new method of etching micro-grating structures (MGSs) on the surface of glazed stainless-steel directly is reported, which makes good use of the interference of nanosecond laser pulses. Through changing the experimental parameters such as working current of the laser and source beam diameter, the influences of these parameters on the depth of grooves and duty cycle of MGSs are analyzed. The results measured with conventional optical microscopy and atomic force microscopy (AFM) show that the depth of grooves of MGSs varies from 0 nm to 350 nm, the duty cycle of MGSs changes between 0.4 and 0.

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18

Hwang, Kildong, Jessica P. Houston, John C. Rasmussen, et al. "Improved Excitation Light Rejection Enhances Small-Animal Fluorescent Optical Imaging." Molecular Imaging 4, no. 3 (2005): 153535002005051. http://dx.doi.org/10.1162/15353500200505142.

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Small-animal fluorescence-enhanced imaging involves the detection of weak fluorescent signals emanating from nanomolar to picomolar concentrations of exogenous or endogenously produced fluorophore concurrent with the rejection of an overwhelmingly large component of backscattered excitation light. The elimination of the back-reflected excitation light of the collected signal remains a major and often unrecognized challenge for further reducing the noise floor and increasing sensitivity of small-animal fluorescence imaging. Herein, we show that the combination of three-cavity interference and h

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HERRALA, ESKO, and JUKKA OKKONEN. "IMAGING SPECTROGRAPH AND CAMERA SOLUTIONS FOR INDUSTRIAL APPLICATIONS." International Journal of Pattern Recognition and Artificial Intelligence 10, no. 01 (1996): 43–54. http://dx.doi.org/10.1142/s0218001496000050.

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An imaging spectrometer instrument based on a prism-grating-prism (PGP) element as the dispersive component and advanced camera solutions for on-line applications are presented. The PGP element uses a volume type holographic plane transmission grating made of dichromated gelatin (DCG). Currently, spectrographs have been realized for the 400–1050 nm region but applicable spectral region of the PGP is 380–1800 nm. Spectral resolution is typically between 1.5 and 5 nm. The on-axis optical configuration and simple rugged tubular optomechanical construction of the spectrograph provides a good image

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20

Zhang, Xiao, and David Joy. "Divergent-beam holography with a 200keV FE TEM." Proceedings, annual meeting, Electron Microscopy Society of America 49 (August 1991): 678–79. http://dx.doi.org/10.1017/s0424820100087707.

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A hologram, first described and named by Gabor (1949), permits a medium such as photographic film, which responds only to intensity, to store the complete amplitude and phase information which characterizes an electron wavefront. The hologram is formed by allowing some fraction of a coherent electron wave which has interacted with a specimen to interact again with original incident wave so as to generate an interference pattern. If the hologram is then itself illuminated by a coherent light source and optical system which mimic the original electron-optical system then a pair of images -one re

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21

Wilby, David, Matthew B. Toomey, Peter Olsson, et al. "Optics of cone photoreceptors in the chicken ( Gallus gallus domesticus )." Journal of The Royal Society Interface 12, no. 111 (2015): 20150591. http://dx.doi.org/10.1098/rsif.2015.0591.

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Vision is the primary sensory modality of birds, and its importance is evident in the sophistication of their visual systems. Coloured oil droplets in the cone photoreceptors represent an adaptation in the avian retina, acting as long-pass colour filters. However, we currently lack understanding of how the optical properties and morphology of component structures (e.g. oil droplet, mitochondrial ellipsoid and outer segment) of the cone photoreceptor influence the transmission of light into the outer segment and the ultimate effect they have on receptor sensitivity. In this study, we use data f

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22

Sobolewska, Anna, Joanna Zawada, Stanislaw Bartkiewicz, and Zbigniew Galewski. "Mechanism of Photochemical Phase Transition of Single-Component Phototropic Liquid Crystals Studied by Means of Holographic Grating Recording." Journal of Physical Chemistry C 117, no. 19 (2013): 10051–58. http://dx.doi.org/10.1021/jp403159w.

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23

Jayaswal, R. K., H. L. Yadav, and P. K. Barhai. "Design and analysis of modified version of double aperture speckle interferometer consisting of holographic optical element: Application to measurement of in plane displacement component." Optik 126, no. 18 (2015): 1700–1704. http://dx.doi.org/10.1016/j.ijleo.2015.05.043.

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24

Scheuer, Jacob. "Metasurfaces-based holography and beam shaping: engineering the phase profile of light." Nanophotonics 6, no. 1 (2017): 137–52. http://dx.doi.org/10.1515/nanoph-2016-0109.

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AbstractThe ability to engineer and shape the phase profile of optical beams is in the heart of any optical element. Be it a simple lens or a sophisticated holographic element, the functionality of such components is dictated by their spatial phase response. In contrast to conventional optical components which rely on thickness variation to induce a phase profile, metasurfaces facilitate the realization of arbitrary phase distributions using large arrays with sub-wavelength and ultrathin (tens of nanometers) features. Such components can be easily realized using a single lithographic step and

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25

Jiang, Hao, Zhao Ma, Honggang Gu, Xiuguo Chen, and Shiyuan Liu. "Characterization of Volume Gratings Based on Distributed Dielectric Constant Model Using Mueller Matrix Ellipsometry." Applied Sciences 9, no. 4 (2019): 698. http://dx.doi.org/10.3390/app9040698.

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Volume grating is a key optical component due to its comprehensive applications. Other than the common grating structures, volume grating is essentially a predesigned refractive index distribution recorded in materials, which raises the challenges of metrology. Although we have demonstrated the potential application of ellipsometry for volume grating characterization, it has been limited due to the absence of general forward model reflecting the refractive index distribution. Herein, we introduced a distributed dielectric constant based rigorous coupled-wave analysis (RCWA) model to interpret

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Martín Minguez, Alfredo, and Paloma R. Horche. "Tunable holographic components in WDM optical networks." Optical and Quantum Electronics 42, no. 1 (2010): 45–67. http://dx.doi.org/10.1007/s11082-010-9420-0.

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27

Trolinger, James D., Amit Lal, Joshua Jo, and Stephen Kupiec. "Programmable Holographic Optical Elements as Adaptive Optics in Optical Diagnostics Devices." Key Engineering Materials 437 (May 2010): 108–12. http://dx.doi.org/10.4028/www.scientific.net/kem.437.108.

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This paper reports a combined, Hartmann/Digital Holographic interferometry inspection system for inspecting optical components that do not easily lend themselves to conventional interferometric or Hartmann inspection. A programmable holographic optical element (HOE) preconditions wavefronts to extend the dynamic range of interferometry measurements and also transforms the same system into a scanning Hartmann operation, which has lower resolution but higher dynamic range. Inspecting aspherical surfaces with existing interferometers requires special, computer generated holographic optical elemen

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Chen, Huang-Ming, Jhou-Pu Yang, Hao-Ting Yen, Zheng-Ning Hsu, Yuge Huang, and Shin-Tson Wu. "Pursuing High Quality Phase-Only Liquid Crystal on Silicon (LCoS) Devices." Applied Sciences 8, no. 11 (2018): 2323. http://dx.doi.org/10.3390/app8112323.

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Fine pixel size and high-resolution liquid crystal on silicon (LCoS) backplanes have been developed by various companies and research groups since 1973. The development of LCoS is not only beneficial for full high definition displays but also to spatial light modulation. The high-quality and well-calibrated panels can project computer generated hologram (CGH) designs faithfully for phase-only holography, which can be widely utilized in 2D/3D holographic video projectors and components for optical telecommunications. As a result, we start by summarizing the current status of high-resolution pan

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Навныко, В. Н., С. Ф. Ничипорко, А. В. Макаревич та С. М. Шандаров. "Вырожденное четырехволновое взаимодействие на пропускающих голографических решетках в кристалле Bi-=SUB=-12-=/SUB=-TiO-=SUB=-20-=/SUB=- среза (110)". Журнал технической физики 91, № 5 (2021): 832. http://dx.doi.org/10.21883/jtf.2021.05.50697.322-20.

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The regularities of the stationary degenerate four-wave mixing on transmission holographic gratings formed in the Bi12TiO20 crystal of the (110)-cut are analyzed. The system of differential equations has been obtained; this system that can be used to find the components of the vector amplitudes of linearly polarized light waves in the case of four-wave mixing on phase and phase-amplitude holographic gratings. The theoretical model take into account the linear electrooptic, the photoelastic and the inverse piezoelectric effects, as well as natural optical activity, circular dichroism and crysta

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Навныко, В. Н., С. Ф. Ничипорко, А. В. Макаревич та С. М. Шандаров. "Вырожденное четырехволновое взаимодействие на пропускающих голографических решетках в кристалле Bi-=SUB=-12-=/SUB=-TiO-=SUB=-20-=/SUB=- среза (110)". Журнал технической физики 91, № 5 (2021): 832. http://dx.doi.org/10.21883/jtf.2021.05.50697.322-20.

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The regularities of the stationary degenerate four-wave mixing on transmission holographic gratings formed in the Bi12TiO20 crystal of the (110)-cut are analyzed. The system of differential equations has been obtained; this system that can be used to find the components of the vector amplitudes of linearly polarized light waves in the case of four-wave mixing on phase and phase-amplitude holographic gratings. The theoretical model take into account the linear electrooptic, the photoelastic and the inverse piezoelectric effects, as well as natural optical activity, circular dichroism and crysta

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31

Veitch, PJ, J. Munch, MW Hamilton, D. Ottaway, A. Greentree, and A. Tikhomirov. "High Power Lasers and Novel Optics for Laser Interferometric Gravitational Wave Detectors." Australian Journal of Physics 48, no. 6 (1995): 999. http://dx.doi.org/10.1071/ph950999.

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Research at Adelaide is directed towards the development of critical optical components for second generation long baseline gravitational wave interferometers. In particular, the development of high power, low noise lasers, and an investigation to determine the potential of holographic, diffractive and nonlinear optical components for solving some of the problems which could limit the sensitivity of second generation detectors. In this paper we will outline the proposed research and present some early results.

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Jaroszewicz, Zbigniew, Eugeniusz Czech, and Tomasz Osuch. "Diffractive gratings with varying period’s shape." Photonics Letters of Poland 11, no. 2 (2019): 41. http://dx.doi.org/10.4302/plp.v11i2.904.

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The aim of this short review is to recall various designs of diffraction gratings when the condition of the period’s identity is relaxed and to mention resulting thus some of their applications. Among others the apodization function can be implemented as a variable diffraction efficiency due to the gradual change of the period’s shape. Another possible application is the passive achromatization of the diffraction efficiency of the blazed gratings by randomizing their blaze angle. Full Text: PDF ReferencesP. Jacquinot and B. Roizen-Dossier, "II Apodisation", Prog. Opt. 3, 29 (1964). CrossRef H.

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Joshi, Pankaj, Oliver Willekens, Xiaobing Shang, et al. "Tunable light beam steering device using polymer stabilized blue phase liquid crystals." Photonics Letters of Poland 9, no. 1 (2017): 11. http://dx.doi.org/10.4302/plp.v9i1.704.

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A polarization independent and fast electrically switchable beam steering device is presented, based on a surface relief grating combined with polymer stabilized blue phase liquid crystals. Switching on and off times are both less than 2 milliseconds. The prospects of further improvements are discussed. Full Text: PDF ReferencesD.C. Wright, et al., "Crystalline liquids: the blue phases", Rev. Mod. Phys. 61, 385 (1989). CrossRef H. Kikuchi, et al., "Polymer-stabilized liquid crystal blue phases", Nat. Mater. 1, 64 (2002). CrossRef Samsung, Korea, SID exhibition, (2008).J. Yan, et al., "Direct m

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Joubert, C., B. Loiseaux, A. Delboulbé, and J. P. Huignard. "Phase volume holographic optical components for high-brightness single-LCD projectors." Applied Optics 36, no. 20 (1997): 4761. http://dx.doi.org/10.1364/ao.36.004761.

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Hayashi, Terutake, Masaki Michihata, and Yasuhiro Takaya. "Development of an Optical Heterogeneity Evaluation System Using Phase-Shift Digital Holography." Key Engineering Materials 523-524 (November 2012): 865–70. http://dx.doi.org/10.4028/www.scientific.net/kem.523-524.865.

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The nondestructive, non-contact, three-dimensional evaluation of optical glass has been important to the manufacturing of high-precision optical components. In order to achieve high-precision nondestructive evaluation of optical heterogeneity, we develop a versatile evaluation system using the parallel phase- shift digital holography, which enables measurements of the optical path differences at a nanometer-scale resolution. The amplitude and phase distributions of the object wave can be reconstructed directly from a single hologram by using the parallel phase-shift digital holography system.

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Kraiskii, A. V., V. A. Postnikov, T. T. Suitanov, and A. V. Khamidulin. "Holographic sensors for diagnostics of solution components." Quantum Electronics 40, no. 2 (2010): 178–82. http://dx.doi.org/10.1070/qe2010v040n02abeh014169.

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Podshivalov, Aleksandr, Alexandra Toropova, Maria Fokina, and Mayya Uspenskaya. "Surface Morphology Formation of Edible Holographic Marker on Potato Starch with Gelatin or Agar Thin Coatings." Polymers 12, no. 5 (2020): 1123. http://dx.doi.org/10.3390/polym12051123.

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Edible films and coatings based on biopolymers to protect and extend the shelf life of food and medicine can be functionalized, by applying a holographic marker on the coating surface for marking products or sensing storage conditions. In this work, holographic markers were prepared on the surface of thin biopolymer coatings based on starch, gelatin, agar and also starch/gelatin and starch/agar blends by the nanoimprint method from a film-forming solution. The morphology of the surface of holographic markers using optical microscopy in reflection mode was examined, as well as the reasons for i

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Hanson, Steen G., Lars R. Lindvold, and Lars Lading. "A surface velocimeter based on a holographic optical element and semiconductor components." Measurement Science and Technology 7, no. 1 (1996): 69–78. http://dx.doi.org/10.1088/0957-0233/7/1/010.

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WEBB, R. P. "OPTOELECTRONIC IMPLEMENTATION OF NEURAL NETWORKS." International Journal of Neural Systems 04, no. 04 (1993): 435–44. http://dx.doi.org/10.1142/s0129065793000365.

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The performance of electronic neural networks will eventually be limited by the capacity of their interconnections as operating speeds are increased. The use of optical connections to link electronic elements offers a way to overcome this problem. In particular, spatial optic techniques are especially suited to neural systems because of their parallel structure. Three experimental optoelectronic networks are described that employ holographic components and arrays of high-speed optical modulators. These networks have been used to demonstrate operation at 50 MHz, novel training algorithms and th

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Montes-Usategui, Mario, Encarnación Pleguezuelos, Jordi Andilla, and Estela Martín-Badosa. "Fast generation of holographic optical tweezers by random mask encoding of Fourier components." Optics Express 14, no. 6 (2006): 2101. http://dx.doi.org/10.1364/oe.14.002101.

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Cha, Soyoung S., Kejian Huang, and James S. Slepicka. "Holographic technique for three-dimensional three-component particle fields." Optics Letters 19, no. 19 (1994): 1577. http://dx.doi.org/10.1364/ol.19.001577.

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NA, Silin, and Younghun YU*. "Refractive Index Distribution Measurement of an Optical Component by Using Digital Holography." New Physics: Sae Mulli 67, no. 11 (2017): 1393–98. http://dx.doi.org/10.3938/npsm.67.1393.

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Machnio, Piotr, Michał Ziemczonok, and Małgorzata Kujawińska. "Reconstruction enhancement via projection screening in holographic tomography." Photonics Letters of Poland 13, no. 2 (2021): 37. http://dx.doi.org/10.4302/plp.v13i2.1104.

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This paper presents an algorithm for automatic detection of erroneous amplitude and phase components of a sample’s optical field, acquired by a holographic tomograph with a limited angle of projection. By applying image processing methods and statistical analysis to find and remove unfit projections, the quality of tomographic reconstruction of a 3D refractive index distribution of an object is greatly improved. The proposed methods can find their application in preprocessing of data in holographic tomography. Full Text: PDF ReferencesA. Kuś, W. Krauze, P. L. Makowski, and M. Kujawińska, "Holo

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Yeo, Jong Bin, and Hyun Yong Lee. "Fabrication of Photonic Crystals by Holographic Lithography Method." Advanced Materials Research 31 (November 2007): 98–100. http://dx.doi.org/10.4028/www.scientific.net/amr.31.98.

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In this study, we found out the new fabrication process condition for Photonic crystals(PCs). PCs were fabricated by holographic lithography(HL), instead of commonly used electron beam lithography(EBL). HL process enable periodic large area fabrication of PCs. Also this method can easily control the pitch of periodic patterns. We set up holographic lithography system by laser and some optical components. The source of light used laser of 442 nm wavelength. Photo-resist(PR) used DMI-150 model. The viscosity of PR is diluted with propylene glycol monomethyl ether acetate(PGMEA) which is solvent

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Rao, M. V. "Applications of holographic interferometry for spacecraft structural components." Optical Engineering 33, no. 6 (1994): 1876. http://dx.doi.org/10.1117/12.168851.

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Hara, Masaaki, Kenji Tanaka, Kazutatsu Tokuyama, et al. "Linear Reproduction of a Holographic Storage Channel using Coherent Addition of Optical DC Components." Japanese Journal of Applied Physics 47, no. 7 (2008): 5885–90. http://dx.doi.org/10.1143/jjap.47.5885.

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Yasuda, Shin, Katsunori Kawano, Jiro Minabe, et al. "Coaxial holographic data storage without recording the dc components." Optics Letters 31, no. 17 (2006): 2607. http://dx.doi.org/10.1364/ol.31.002607.

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Smirnova, T. N., L. M. Kokhtich, O. V. Sakhno, and J. Stumpe. "Holographic nanocomposites for recording polymer-nanoparticle periodic structures: I. General approach to choice of components of nanocomposites and their holographic properties." Optics and Spectroscopy 110, no. 1 (2011): 129–36. http://dx.doi.org/10.1134/s0030400x11010206.

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Konar, S., Soumendu Jana, and Woo-Pyo Hong. "Two-component spatial holographic solitons supported by cross-phase modulation." Physica Scripta 76, no. 5 (2007): 470–74. http://dx.doi.org/10.1088/0031-8949/76/5/012.

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Hariharan, P., B. F. Oreb, and C. H. Freund. "Stroboscopic holographic interferometry: measurements of vector components of a vibration." Applied Optics 26, no. 18 (1987): 3899. http://dx.doi.org/10.1364/ao.26.003899.

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