Academic literature on the topic 'Stokes polarimetry'

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Journal articles on the topic "Stokes polarimetry"

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Leiber, Th, and K. Reif. "First Observations by the Bonn Wide-Field Photometer and Polarimeter (WWFPP): Surface Polarimetry of the Crab Nebula." Symposium - International Astronomical Union 161 (1994): 481–83. http://dx.doi.org/10.1017/s0074180900047926.

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To test the performance of the WWFPP in polarimetric mode, we performed surface polarimetry of the Crab nebula in February 1993 using the Asiago 1.82 m telescope of the ‘Osservatorio Astronomico di Padova’. The polarimeter is a new design and enables us to do simultaneous wide-field polarimetry (15 × 15 arcmin field with 0.43 arcsec/pixel) of four polarization angles using a twin Wollaston prism or simultaneous polarimetry of two angles using a double wedge plate with orthogonal sheet polarizers in combination with an achromatic half wave plate. For the observations described here we used the twin Wollaston. The advantages of this design are independency of fluctuations of atmospheric transmission and identical seeing for one set of Stokes parameters. The results of the observations are in agreement with results of other investigators who performed surface polarimetry of the Crab Nebula.
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Espinosa-Soria, Alba, Francisco J. Rodríguez-Fortuño, Amadeu Griol, and Alejandro Martínez. "Full Measurement of the Stokes Parameters Using a Subwavelength Silicon On-Chip Polarimeter." Advances in Science and Technology 98 (October 2016): 103–8. http://dx.doi.org/10.4028/www.scientific.net/ast.98.103.

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Polarimetry enables to measure the state of polarization (SoP) of a light beam, which is essential in many disciplines. Typical polarimeters use bulky and expensive optical elements such as half-wave plates and grid polarizers. Plasmonic nanostructures may help to transform such bulky components into subwavelength metallic elements showing similar performance. Based on the concept of spin-orbit coupling, here we demonstrate a nanophotonic polarimeter that measures the Stokes parameters of a light beam over an ultrabroad bandwidth in a less than a square wavelength active region. Furthermore, the presented approach is applicable to any wavelength regime and technological platform, paving the way for the miniaturization of polarimeters.
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Guo, Jing, Deqing Ren, Yongtian Zhu, and Xi Zhang. "A high-speed and high-efficiency imaging polarimeter based on ferroelectric liquid crystal retarders: Design and test." Publications of the Astronomical Society of Japan 73, no. 2 (February 16, 2021): 405–16. http://dx.doi.org/10.1093/pasj/psab007.

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Abstract Polarimeters play a key role in investigating solar magnetic fields. In this paper, a High speed and high efficiency Imaging POlarimeter (HIPO) is proposed based on a pair of ferroelectric liquid crystal retarders (FLCs), with the ultimate goal of measuring magnetic fields of prominences and filaments from the ground. A unique feature of the HIPO is that it enables high cadence polarization measurements covering a wide field of view (FOV); the modulation frequency of the HIPO is able to achieve ∼100 Hz, which greatly suppresses the seeing-induced crosstalk, and the maximum FOV can reach 62″ × 525″. Additionally, FLC retardances under low and high states were calibrated individually and found to have a slight discrepancy, which is neglected in most works. Based on FLC calibration results, an optimization was performed using a constrained nonlinear minimization approach to obtain the maximum polarimetric efficiency. Specifically, optimized efficiencies of the Stokes Q, U, and V are well balanced and determined as (ξQ, ξU, ξV) = (0.5957, 0.5534, 0.5777), yielding a total efficiency of 0.9974. Their practical efficiencies are measured as (ξQ′, ξU′, ξV′) = (0.5934, 0.5385, 0.5747), slightly below the optimized values but still resulting in a high total efficiency of 0.9861. The HIPO shows advantages in terms of modulation frequency and polarimetric efficiency compared with most other representative ground-based solar polarimeters. In the observations, measurement accuracy is found to be better than 2.7 × 10−3 by evaluating full Stokes Hα polarimetry results of the chromosphere. This work lays a foundation for the development of high-speed and high-accuracy polarimeters for our next-generation solar instruments.
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Hannonen, Antti, Bernhard J. Hoenders, Wolfgang Elsässer, Ari T. Friberg, and Tero Setälä. "Ghost polarimetry using Stokes correlations." Journal of the Optical Society of America A 37, no. 5 (April 2, 2020): 714. http://dx.doi.org/10.1364/josaa.385851.

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Eshaghi, Mahdi, and Aristide Dogariu. "Single-shot omnidirectional Stokes polarimetry." Optics Letters 45, no. 15 (July 30, 2020): 4340. http://dx.doi.org/10.1364/ol.396528.

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Raney, R. Keith. "Hybrid Dual-Polarization Synthetic Aperture Radar." Remote Sensing 11, no. 13 (June 27, 2019): 1521. http://dx.doi.org/10.3390/rs11131521.

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Compact polarimetry for a synthetic aperture radar (SAR) system is reviewed. Compact polarimetry (CP) is intended to provide useful polarimetric image classifications while avoiding the disadvantages of space-based quadrature-polarimetric (quad-pol) SARs. Two CP approaches are briefly described, π/4 and circular. A third form, hybrid compact polarimetry (HCP) has emerged as the preferred embodiment of compact polarimetry. HCP transmits circular polarization and receives on two orthogonal linear polarizations. When seen through its associated data processing and image classification algorithms, HPC’s heritage dates back to the Stokes parameters (1852), which are summarized and explained in plain language. Hybrid dual-polarimetric imaging radars were in the payloads of two lunar-orbiting satellites, India’s Earth-observing RISAT-1, and Japan’s ALOS-2. In lunar or planetary orbit, a satellite equipped with an HCP imaging radar delivers the same class of polarimetric information as Earth-based radar astronomy. In stark contrast to quad-pol, compact polarimetry is compatible with wide swath modes of a SAR, including ScanSAR. All operational modes of the SARs aboard Canada’s three-satellite Radarsat Constellation Mission (RCM) are hybrid dual-polarimetric. Image classification methodologies for HCP data are reviewed, two of which introduce errors for reasons explained. Their use is discouraged. An alternative and recommended group of methodologies yields reliable results, illustrated by polarimetrically classified images. A survey over numerous quantitative studies demonstrates HCP polarimetric classification effectiveness. The results verify that the performance accuracy of the HCP architecture is comparable to the accuracy delivered by a quadrature-polarized SAR. Four appendices are included covering related topics, including comments on inflight calibration of an HCP radar.
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Krouglov, Serguei, and Virginijus Barzda. "Three-dimensional nonlinear Stokes–Mueller polarimetry." Journal of the Optical Society of America B 36, no. 2 (February 1, 2019): 541. http://dx.doi.org/10.1364/josab.36.000541.

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Arbabi, Ehsan, Seyedeh Mahsa Kamali, Amir Arbabi, and Andrei Faraon. "Full-Stokes Imaging Polarimetry Using Dielectric Metasurfaces." ACS Photonics 5, no. 8 (July 16, 2018): 3132–40. http://dx.doi.org/10.1021/acsphotonics.8b00362.

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Tomczyk, Steven, Roberto Casini, Alfred G. de Wijn, and Peter G. Nelson. "Wavelength-diverse polarization modulators for Stokes polarimetry." Applied Optics 49, no. 18 (June 17, 2010): 3580. http://dx.doi.org/10.1364/ao.49.003580.

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Azzam, R. M. A. "Stokes-vector and Mueller-matrix polarimetry [Invited]." Journal of the Optical Society of America A 33, no. 7 (June 24, 2016): 1396. http://dx.doi.org/10.1364/josaa.33.001396.

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Dissertations / Theses on the topic "Stokes polarimetry"

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Kudenov, Michael W. "Infrared Stokes Polarimetry and Spectropolarimetry." Diss., The University of Arizona, 2009. http://hdl.handle.net/10150/193729.

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In this work, three methods of measuring the polarization state of light in the thermal infrared (3-12 microns) are modeled, simulated, calibrated and experimentally verified in the laboratory. The first utilizes the method of channeled spectropolarimetry (CP) to encode the Stokes polarization parameters onto the optical power spectrum. This channeled spectral technique is implemented with the use of two Yttrium Vanadate (YVO4) crystal retarders. A basic mathematical model for the system is presented, showing that all the Stokes parameters are directly present in the interferogram. Theoretical results are compared with real data from the system, an improved model is provided to simulate the effects of absorption within the crystal, and a modified calibration technique is introduced to account for this absorption. Lastly, effects due to interferometer instabilities on the reconstructions, including nonuniform sampling and interferogram translations, are investigated and techniques are employed to mitigate them.Second is the method of prismatic imaging polarimetry (PIP), which can be envisioned as the monochromatic application of channeled spectropolarimetry. Unlike CP, PIP encodes the 2-dimensional Stokes parameters in a scene onto spatial carrier frequencies. However, the calibration techniques derived in the infrared for CP are extremely similar to that of the PIP. Consequently, the PIP technique is implemented with a set of four YVO4 crystal prisms. A mathematical model for the polarimeter is presented in which diattenuation due to Fresnel effects and dichroism in the crystal are included. An improved polarimetric calibration technique is introduced to remove the diattenuation effects, along with the relative radiometric calibration required for the BPIP operating with a thermal background and large detector offsets. Data demonstrating emission polarization are presented from various blackbodies, which are compared to data from our Fourier transform infrared spectropolarimeter. Additionally, limitations in the PIP technique with regards to the spectral bandwidth and F/# of the imaging system are analyzed. A model able to predict the carrier frequency's fringe visibility is produced and experimentally verified, further reinforcing the PIP's limitations.The last technique is significantly different from CP or PIP and involves the simulation and calibration of a thermal infrared division of amplitude imaging Stokes polarimeter. For the first time, application of microbolometer focal plane array (FPA) technology to polarimetry is demonstrated. The sensor utilizes a wire-grid beamsplitter with imaging systems positioned at each output to analyze two orthogonal linear polarization states simultaneously. Combined with a form birefringent wave plate, the system is capable of snapshot imaging polarimetry in any one Stokes vector (S1, S2 or S3). Radiometric and polarimetric calibration procedures for the instrument are provided and the reduction matrices from the calibration are compared to rigorous coupled wave analysis (RCWA) and raytracing simulations. The design and optimization of the sensor's wire-grid beam splitter and wave plate are presented, along with their corresponding prescriptions. Polarimetric calibration error due to the spectrally broadband nature of the instrument is also overviewed. Image registration techniques for the sensor are discussed and data from the instrument are presented, demonstrating a microbolometer's ability to measure the small intensity variations corresponding to polarized emission in natural environments.
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Yong, Siow Yin. "Radar polarimetry." Thesis, Monterey, Calif. : Springfield, Va. : Naval Postgraduate School ; Available from National Technical Information Service, 2004. http://library.nps.navy.mil/uhtbin/hyperion/04Dec%5FYong.pdf.

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Bernasconi, Pietro Nicola. "Stokes vector-polarimetry : observation and analysis of solar magnetic fields /." [S.l.] : [s.n.], 1997. http://e-collection.ethbib.ethz.ch/show?type=diss&nr=12227.

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Narayan, Chaya. "Study of Optically Active Biological Fluids Using Polarimetric Data Analysis." University of Akron / OhioLINK, 2011. http://rave.ohiolink.edu/etdc/view?acc_num=akron1314038487.

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Adams, Ian. "SIMULATION AND STUDY OF THE STOKES VECTOR IN A PRECIPITATING ATMOSPHERE." Doctoral diss., University of Central Florida, 2007. http://digital.library.ucf.edu/cdm/ref/collection/ETD/id/3479.

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Precipitation is a dominating quantity in microwave radiometry. The large emission and scattering signals of rain and ice, respectively, introduce large contributions to the measured brightness temperature. While this allows for accurate sensing of precipitation, it also results in degraded performance when retrieving other geophysical parameters, such as near-surface ocean winds. In particular, the retrieval of wind direction requires precise knowledge of polarization, and nonspherical particles can result in a change in the polarization of incident radiation. The aim of this dissertation is to investigate the polarizing effects of precipitation in the atmosphere, including the existence of a precipitation signal in the third Stokes parameter, and compare these effects with the current sensitivities of passive wind vector retrieval algorithms. Realistic simulated precipitation profiles give hydrometeor water contents which are input into a vector radiative transfer model. Brightness temperatures are produced within the model using a reverse Monte Carlo method. Results are produced at three frequencies of interest to microwave polarimetry, 10.7 GHz, 18.7 GHz, and 37.0 GHz, for the first 3 components of the Stokes vector.
Ph.D.
School of Electrical Engineering and Computer Science
Engineering and Computer Science
Electrical Engineering PhD
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Mu, Tingkui, Shaun Pacheco, Zeyu Chen, Chunmin Zhang, and Rongguang Liang. "Snapshot linear-Stokes imaging spectropolarimeter using division-of-focal-plane polarimetry and integral field spectroscopy." NATURE PUBLISHING GROUP, 2017. http://hdl.handle.net/10150/622866.

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In this paper, the design and experimental demonstration of a snapshot linear-Stokes imaging spectropolarimeter (SLSIS) is presented. The SLSIS, which is based on division-of-focal-plane polarimetry with four parallel linear polarization channels and integral field spectroscopy with numerous slit dispersive paths, has no moving parts and provides video-rate Stokes-vector hyperspectral datacubes. It does not need any scanning in the spectral, spatial or polarization dimension and offers significant advantages of rapid reconstruction without heavy computation during post-processing. The principle and the experimental setup of the SLSIS are described in detail. The image registration, Stokes spectral reconstruction and calibration procedures are included, and the system is validated using measurements of tungsten light and a static scene. The SLSIS's snapshot ability to resolve polarization spectral signatures is demonstrated using measurements of a dynamic scene.
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Narayan, Chaya. "Polarimetric Stokes Imaging for the Detection of Tumor Margins and Segmentation." University of Akron / OhioLINK, 2013. http://rave.ohiolink.edu/etdc/view?acc_num=akron1386785379.

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Bradley, Christine Lavella, and Christine Lavella Bradley. "SpectroPolarimetric Imaging Observations." Diss., The University of Arizona, 2017. http://hdl.handle.net/10150/624499.

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The capability to map anthropogenic aerosol quantities and properties over land can provide significant insights for climate and environmental studies on global and regional scales. One of the primary challenges in aerosol information monitoring is separating two signals measured by downward-viewing airborne or spaceborne instruments: the light scattered from the aerosols and light reflected from the Earth's surface. In order to study the aerosols independently, the surface signal needs to be subtracted out from the measurements. Some observational modalities, such as multispectral and multiangle, do not provide enough information to uniquely define the Earth's directional reflectance properties for this task due to the high magnitude and inhomogeneity of albedo for land surface types. Polarization, however, can provide additional information to define surface reflection. To improve upon current measurement capabilities of aerosols over urban areas, Jet Propulsion Laboratory developed the Multiangle SpectroPolarimetric Imager (MSPI) that can accurately measure the Degree of Linear Polarization to 0.5%. In particular, data acquired by the ground-based prototype, GroundMSPI, is used for directional reflectance studies of outdoor surfaces in this dissertation. This work expands upon an existing model, the microfacet model, to characterize the polarized bidirectional reflectance distribution function (pBRDF) of surfaces and validate an assumption, the Spectral Invariance Hypothesis, on the surface pBRDF that is used in aerosol retrieval algorithms. The microfacet model is commonly used to represent the pBRDF of Earth's surface types, such as ocean and land. It represents a roughened surface comprised of randomly oriented facets that specularly reflect incoming light into the upward hemisphere. The analytic form of the pBRDF for this model assumes only a single reflection of light from the microfaceted surface. If the incoming illumination is unpolarized, as it is with natural light from the Sun, the reflected light is linearly polarized perpendicular to the plane that contains the illumination and view directions, the scattering plane. However, previous work has shown that manmade objects, such as asphalt and brick, show a polarization signature that differs from the single reflection microfacet model. Using the polarization ray-tracing (PRT) program POLARIS-M, a numerical calculation for the pBRDF is made for a roughened surface to account for multiple reflections that light can experience between microfacets. Results from this numerical PRT method shows rays that experience two or more reflections with the microfacet surface can be polarized at an orientation that differs from the analytical single reflection microfacet model. This PRT method is compared against GroundMSPI data of manmade surfaces. An assumption made regarding the pBRDF for this microfacet model is verified with GroundMSPI data of urban areas. This is known as the Spectral Invariance Hypothesis and asserts that the magnitude and shape of the polarized bidirectional reflectance factor (pBRF) is the same for all wavelengths. This simplifies the microfacet model by assuming some surface parameters such as the index of refraction are spectrally neutral. GroundMSPI acquires the pBRF for five prominent region types, asphalt, brick, cement, dirt, and grass, for day-long measurements on clear sky conditions. Over the course of each day, changing solar position in the sky provides a large range of scattering angles for this study. The pBRF is measured for the three polarimetric wavelengths of GroundMSPI, 470, 660, and 865nm, and the best fit slope of the spectral correlation is reported. This investigation shows agreement to the Spectral Invariance Hypothesis within 10% for all region types excluding grass. Grass measurements show a large mean deviation of 31.1%. This motivated an angle of linear polarization (AoLP) analysis of cotton crops to isolate single reflection cases, or specular reflections, from multiple scattering cases of light in vegetation. Results from this AoLP method show that specular reflections off the top surface of leaves follow the Spectral Invariance Hypothesis.
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Petermann, Jeff C. "Design of a Fully Automated Polarimetric Imaging System for Remote Characterization of Space Materials." University of Akron / OhioLINK, 2012. http://rave.ohiolink.edu/etdc/view?acc_num=akron1329101390.

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Gendre, Luc. "Conception et réalisation d'un polarimètre de Stokes haute cadence à division temporelle utilisant un unique modulateur à cristaux liquides ferroélectriques pour moduler la polarisation." Phd thesis, Université de Haute Alsace - Mulhouse, 2011. http://tel.archives-ouvertes.fr/tel-00713656.

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L'imagerie de polarisation apporte des informations complémentaires à l'imagerie conventionnelle. L'oeil humain n'étant cependant pas sensible à la polarisation de la lumière, l'utilisation d'équipements spécifiques est indispensable. Depuis le XIXème siècle, des scientifiques étudient la polarisation de la lumière: d'abord avec de simples lames polarisantes, puis depuis une vingtaine d'années à l'aide de modulateurs à cristaux liquides (CL). Ces derniers présentent un avantage considérable par rapport aux lames polarisantes: ils permettent des vitesses de modulation de la polarisation de la lumière qui ne peuvent être atteintes avec des lames orientées mécaniquement. Les CL nématiques alignés parallèlement et les CL nématiques en hélice sont les plus répandus aujourd'hui, que ce soit dans des équipements grand public tels que les écrans d'ordinateur, ou dans des équipements professionnels. Ils fonctionnent à des fréquences maximales de l'ordre de 50Hz. La vitesse de fonctionnement de ces CL peut toutefois encore être dépassée en utilisant des CL ferroélectriques, pouvant atteindre le kiloHertz. Ces éléments sont rapportés dans la littérature comme des éléments bistables, donc ne permettant pas de moduler la polarisation incidente de manière accordable, contrairement aux CL nématiques. En d'autres termes, un seul modulateur à CL ferroélectriques ne permet a priori pas d'analyser la totalité de la polarisation. Seulement une fraction de la polarisation linéaire du faisceau incident peut être identifiée.Le présent travail vise à montrer qu'a posteriori des CL ferroélectriques convenablement commandés peuvent être utilisés de manière accordable pour analyser la totalité de la polarisation. Partant d'un modulateur à CL ferroélectriques conventionnel, il est montré dans un premier temps que l'on peut analyser la totalité de la polarisation linéaire dès lors que la commande électrique est adaptée. Puis dans un deuxième temps, en exploitant la dépendance en longueur d'onde du comportement du modulateur, nous démontrons que cet élément optique peut être utilisé pour analyser la totalité de la polarisation du faisceau incident, c'est-à-dire la composante linéaire aussi bien que circulaire. Un polarimètre à division temporelle est développé pour prouver la faisabilité d'un polarimètre n'utilisant qu'un seul et unique modulateur à CL ferroélectriques pour tout élément polarisant. Un défaut a également été mis en évidence dans la restitution de l'information de polarisation avec un polarimètre à division temporelle lors de l'observation d'objets en mouvement. Avec un tel système, l'acquisition des différentes images d'intensités nécessaires à l'estimation de l'information de polarisation se fait séquentiellement. Par conséquent, le mouvement d'un objet dans la scène pendant la phase d'acquisition se répercute sur la séquence d'images d'intensités, ce qui produit des artéfacts lors de l'estimation de la polarisation. Des solutions à ce problème sont proposées.
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Book chapters on the topic "Stokes polarimetry"

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Stenflo, Jan O. "Stokes polarimetry of the Zeeman and Hanle effects." In Observing Photons in Space, 583–98. New York, NY: Springer New York, 2013. http://dx.doi.org/10.1007/978-1-4614-7804-1_33.

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Pham, Thi-Thu-Hien, and Yu-Lung Lo. "Decoupling Six Effective Parameters of Anisotropic Optical Materials Using Stokes Polarimetry." In Optical Measurements, Modeling, and Metrology, Volume 5, 365–70. New York, NY: Springer New York, 2011. http://dx.doi.org/10.1007/978-1-4614-0228-2_44.

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Fleck, B. "Time-Resolved Stokes V Polarimetry of Small-Scale Magnetic Structures on the Sun." In Reviews in Modern Astronomy, 90–103. Berlin, Heidelberg: Springer Berlin Heidelberg, 1991. http://dx.doi.org/10.1007/978-3-642-76750-0_6.

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Calvani, R., R. Caponi, and F. Cisternino. "Real-Time Heterodyne Fibre Polarimetry by Means of Jones and Stokes Vector Detection." In Trends in Optical Fibre Metrology and Standards, 527–39. Dordrecht: Springer Netherlands, 1995. http://dx.doi.org/10.1007/978-94-011-0035-9_27.

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Yan, Wei-Ling, and Wolfgang-Martin Boerner. "Optimal Polarization States Determination of the Stokes Reflection Matrices [ M ¯ p ] $$\left[ {{{\bar M}_p}} \right]$$ for the Coherent Case, and of the Mueller Matrix [M] for the Partially Polarized Case." In Direct and Inverse Methods in Radar Polarimetry, 351–85. Dordrecht: Springer Netherlands, 1992. http://dx.doi.org/10.1007/978-94-010-9243-2_12.

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Lin, Jing-Fung, and Meng-Zhe Lee. "Using Stokes Polarimeter for Linear Birefringence and Dichroism in Ferrofluid." In Conference Proceedings of the Society for Experimental Mechanics Series, 319–26. New York, NY: Springer New York, 2012. http://dx.doi.org/10.1007/978-1-4614-4235-6_44.

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Berg, Matthew J. "Reflection symmetry of a sphere’s internal field and its consequences on scattering: behavior of the Stokes parameters." In Polarimetric Detection, Characterization and Remote Sensing, 31–48. Dordrecht: Springer Netherlands, 2011. http://dx.doi.org/10.1007/978-94-007-1636-0_2.

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Skumanich, A., B. W. Lites, and V. Martinez Pillet. "Vector Spectropolarimetry with the Advanced Stokes Polarimeter (ASP) for Quantitative Solar Magnetometry." In Solar Surface Magnetism, 99–125. Dordrecht: Springer Netherlands, 1994. http://dx.doi.org/10.1007/978-94-011-1188-1_9.

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"Stokes Polarimetry." In Polarized Light, Revised and Expanded. CRC Press, 2003. http://dx.doi.org/10.1201/9780203911587.ch27.

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"Stokes Polarimetry." In Polarized Light, Third Edition, 327–52. CRC Press, 2010. http://dx.doi.org/10.1201/b10436-19.

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Conference papers on the topic "Stokes polarimetry"

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Ushenko, Alexander G., Dimitry N. Burkovets, Serhiy B. Yermolenko, A. D. Arkhelyuk, Vasyl P. Pishak, A. M. Yuzko, Olga V. Pishak, L. A. Plaviuk, A. P. Peresunko, and V. M. Znack. "Stokes polarimetry of biotissues." In International Conference on Correlation Optics, edited by Oleg V. Angelsky. SPIE, 1999. http://dx.doi.org/10.1117/12.370448.

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Angelsky, Oleg V., Alexander G. Ushenko, Vasyl P. Pishak, Dimitry N. Burkovets, Serhiy B. Yermolenko, Olga V. Pishak, and Yuriy A. Ushenko. "Stokes polarimetry of biotissues." In Photonics Prague '99, edited by Miroslav Hrabovsky, Pavel Tomanek, and Miroslav Miler. SPIE, 1999. http://dx.doi.org/10.1117/12.373663.

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Hagen, Nathan. "Analytic statistics for Stokes polarimetry." In Polarization Science and Remote Sensing VIII, edited by Frans Snik and Joseph A. Shaw. SPIE, 2017. http://dx.doi.org/10.1117/12.2273628.

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Denisenko, Vladimir G., Roman Egorov, and Marat S. Soskin. "Stokes polarimetry in singular optics." In SPIE Proceedings, edited by Oleg V. Angelsky. SPIE, 2004. http://dx.doi.org/10.1117/12.558753.

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Olivard, Pascal, Pierre-Yves Gerligand, Bernard Le Jeune, Jack Cariou, and Jean Lotrian. "Stokes-Mueller formalism and Poincare sphere representation applied to studies of monomode optical fibers." In Polarimetry and Ellipsometry, edited by Maksymilian Pluta and Tomasz R. Wolinski. SPIE, 1997. http://dx.doi.org/10.1117/12.271831.

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Savenkov, Sergey N., Yevgeny A. Oberemok, and Alexander S. Klimov. "Analysis of generalized polarimetric measurement equations for Stokes polarimetry techniques." In 2008 Microwaves, Radar and Remote Sensing Symposium (MRRS). IEEE, 2008. http://dx.doi.org/10.1109/mrrs.2008.4669545.

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Castillejos, Y., Geminiano Martínez-Ponce, Azael Mora-Nuñez, and R. Castro-Sanchez. "Multispectral Stokes polarimetry for dermatoscopic imaging." In SPIE/OSJ Biophotonics Japan, edited by Takashige Omatsu, Yoshio Hayasaki, Yusuke Ogura, Yasuyuki Ozeki, and Seigo Ohno. SPIE, 2015. http://dx.doi.org/10.1117/12.2205123.

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Huynen, Jean R. "Stokes matrix parameters and their interpretation in terms of physical target properties." In Polarimetry '90, Huntsville, AL, edited by Russell A. Chipman and John W. Morris. SPIE, 1990. http://dx.doi.org/10.1117/12.22083.

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Shearer, Andrew. "GASP-Galway Astronomical Stokes Polarimeter." In Polarimetry days in Rome: Crab status, theory and prospects. Trieste, Italy: Sissa Medialab, 2009. http://dx.doi.org/10.22323/1.078.0029.

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Bae, Janghwan, David Haefner, Sergey Sukhov, and Aristide Dogariu. "Full Stokes Polarimetry in the Near Field." In Computational Optical Sensing and Imaging. Washington, D.C.: OSA, 2009. http://dx.doi.org/10.1364/cosi.2009.cwa1.

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Reports on the topic "Stokes polarimetry"

1

Tsang, Leung. Effects of Ocean Wind, Foam/Spray and Atmosphere on Four Stokes Parameters in Passive Polarimetric Remote Sensing of the Ocean Based on Numerical Simulations and Analytic Theory. Fort Belvoir, VA: Defense Technical Information Center, September 2003. http://dx.doi.org/10.21236/ada629271.

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