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Journal articles on the topic 'Linear dichroism'

Author: Grafiati

Published: 4 June 2021

Last updated: 15 June 2025

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1

Chang, Huibin, Matthew A. Marcus, and Stefano Marchesini. "Analyzer-free linear dichroic ptychography." Journal of Applied Crystallography 53, no. 5 (2020): 1283–92. http://dx.doi.org/10.1107/s160057672001002x.

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Linear dichroism is an important tool to characterize the transmission matrix and determine the crystal or orbital orientation in a material. In order to achieve high-resolution mapping of transmission properties, the linear-dichroism scattering model in ptychographic imaging is introduced, and an efficient two-stage reconstruction algorithm is developed. Using the proposed algorithm on a uniaxial material, the dichroic transmission matrix can be recovered without an analyzer by using ptychography measurements with as few as three different polarization angles, with the help of an empty region to remove phase ambiguities.

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2

Kuball, Hans-Georg. "Circular Dichroism and Linear Dichroism." Zeitschrift für Physikalische Chemie 212, Part_1 (1999): 118–19. http://dx.doi.org/10.1524/zpch.1999.212.part_1.118.

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3

Polavarapu, Prasad L., and Gang-Chi Chen. "Polarization-Division Interferometry: Far-Infrared Dichroism." Applied Spectroscopy 48, no. 11 (1994): 1410–18. http://dx.doi.org/10.1366/0003702944028119.

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We report the first far-infrared dichroism measurements using a polarization-division interferometer (PDI) developed in our laboratory. This interferometer uses a free-standing wire-grid beamsplitter made of tungsten wires. In conjunction with a linear polarizer in front of the source and two roof-top mirrors (one in each arm of the interferometer), the PDI divides the input beam into two orthogonal linear polarization components, recombines them for interference at the beamsplitter, and directs the output beam at 90° to the direction of the input beam. Light exiting the interferometer is manipulated with far-infrared lenses, to avoid polarization distortions that are inherent to the reflecting surfaces of the mirrors. The performance of the PDI is evaluated by measuring the linear dichroism of oriented PVF2 [poly(vinylidenefluoride) and circular dichroism of α-pinene, camphor, and 3-methylcyclohexanone. The dichroic multiplex advantage (ability to measure dichroism in the entire far-infrared region from a single measurement) and throughput advantage are demonstrated. These measurements establish the utility of the PDI in measuring transmission and linear dichroism spectra simultaneously without the need for any additional components. Additional developments appear necessary to establish the circular dichroism measurements when the magnitudes are less than one part in one thousand.

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4

Polavarapu, Prasad L., Gang-Chi Chen, and Stephen Weibel. "Development, Justification, and Applications of a Mid-Infrared Polarization-Division Interferometer." Applied Spectroscopy 48, no. 10 (1994): 1224–35. http://dx.doi.org/10.1366/0003702944027381.

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We report the development of a polarization-division interferometer (PDI) for the mid-infrared region. This interferometer uses a self-designed beamsplitter constructed in-house from a BaF2 polarizer and a matching substrate. In conjunction with a linear polarizer in front of the source and two roof-top mirrors, one in each arm of the interferometer, the PDI divides the input beam into two orthogonal linear polarization components, recombines them for interference at the beamsplitter, and directs the output beam at 90° to the direction of the input beam. Light exiting the interferometer is manipulated entirely with lenses, to avoid polarization distortions that are inherent to the reflecting surfaces of the mirrors. Details of the instrumental design for this mid-infrared PDI are presented. The performance of the PDI is evaluated by measuring the circular dichroism of α-pinene and camphor and the linear dichroism of oriented polypropylene and polystyrene. These measurements establish the utility of the PDI to measure transmission, circular dichroism, and linear dichroism spectra simultaneously without need for any additional components. The dichroic multiplex advantage (ability to measure dichroism in the entire mid-infrared region from a single measurement) and throughput advantage are demonstrated.

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5

Sharma, Vishakha, Yogita Kalra, and Ravindra Kumar Sinha. "Chiral perovskite based metasurface for linear and circular dichroism." Journal of Optics 26, no. 12 (2024): 125103. http://dx.doi.org/10.1088/2040-8986/ad80a7.

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Abstract Chiral metasurfaces provide ultracompact devices for polarization modification and detection. In this paper, high linear dichroism (LD) and dual band circular dichroism (CD) using superstructural chiral structure with inbuilt resonance cavities based on metal perovskite metal layer is proposed. Under circularly polarised incident waves, the metasurface exhibits a dual-band CD with a maximum value of 0.81. On the other hand, the suggested design also accomplishes efficient LD of 0.95. Additionally, independent control over each resonance wavelength may be attained by modifying parameters inside each resonance cavities. This will significantly contribute to the advancement of tunable dichroic devices and flat polarization optical components in optical integrated systems.

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6

Garab, Győző, and Herbert van Amerongen. "Linear dichroism and circular dichroism in photosynthesis research." Photosynthesis Research 101, no. 2-3 (2009): 135–46. http://dx.doi.org/10.1007/s11120-009-9424-4.

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7

Pellow, Robert, and Martin Vala. "Magnetic circular dichroism and magnetic linear dichroism of randomly oriented linear molecules." Molecular Physics 68, no. 4 (1989): 893–901. http://dx.doi.org/10.1080/00268978900102611.

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8

Lippitsch, M. E., M. Riegler, F. R. Aussenegg, et al. "Linear Dichroism Spectroscopy of Retinal with Picosecond Time Resolution." Zeitschrift für Naturforschung C 40, no. 11-12 (1985): 880–85. http://dx.doi.org/10.1515/znc-1985-11-1222.

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Abstract For the first time linear dichroism spectroscopy has been extended to the picosecond time regime. 11-cis retinal, all-trans retinal and 1,8-diphenyl-1,3,5,7-octatetraene (DPOT) are incorporated into polyethylene films and oriented by stretching the films. By measuring picosecond transient absorption spectra polarized parallel and perpendicular to the stretching direction and calculating the dichroic ratio we get informations about the molecular geometry in excited singlet and triplet states. The results may have relevance to vision.

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9

Pagni, R. M. "Circular Dichroism and Linear Dichroism (Rodger, Alison; Norden, Bengt)." Journal of Chemical Education 75, no. 9 (1998): 1095. http://dx.doi.org/10.1021/ed075p1095.

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10

LYLE, PAUL A., and WALTER S. STRUVE. "DYNAMIC LINEAR DICHROISM IN CHROMOPROTEINS." Photochemistry and Photobiology 53, no. 3 (1991): 359–65. http://dx.doi.org/10.1111/j.1751-1097.1991.tb03641.x.

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11

Ade, H., and B. Hsiao. "X-ray Linear Dichroism Microscopy." Science 262, no. 5138 (1993): 1427–29. http://dx.doi.org/10.1126/science.262.5138.1427.

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12

Margulies, L., N. Friedman, M. Sheves, et al. "Linear dichroism study of retinoids." Tetrahedron 41, no. 1 (1985): 191–95. http://dx.doi.org/10.1016/s0040-4020(01)83485-2.

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13

Hillebrecht, F. U., H. B. Rose, Ch Roth, and E. Kisker. "Linear magnetic dichroism in photoemission." Journal of Magnetism and Magnetic Materials 148, no. 1-2 (1995): 49–52. http://dx.doi.org/10.1016/0304-8853(95)00145-x.

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14

Louis-Dorr, Valérie, Karim Naoun, Paul Allé, Anne-Marie Benoit, and Antoine Raspiller. "Linear dichroism of the cornea." Applied Optics 43, no. 7 (2004): 1515. http://dx.doi.org/10.1364/ao.43.001515.

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15

Cheng, Xi, Maxim B. Joseph, James A. Covington, Timothy R. Dafforn, Matthew R. Hicks, and Alison Rodger. "Continuous-channel flow linear dichroism." Analytical Methods 4, no. 10 (2012): 3169. http://dx.doi.org/10.1039/c2ay25513h.

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16

Johansson, Lennart B.-Å. "Analysis and application of linear dichroism on membranes. Description of a linear-dichroism spectrometer." Journal of the Chemical Society, Faraday Transactions 1: Physical Chemistry in Condensed Phases 81, no. 6 (1985): 1375. http://dx.doi.org/10.1039/f19858101375.

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17

Gladskikh I. A., Dadadzhanov D. R., Zakoldaev R. A., and Vartanyan T. A. "Laser-induced linear dichroism in planar self-organized silver nanostructures." Optics and Spectroscopy 130, no. 9 (2022): 1153. http://dx.doi.org/10.21883/eos.2022.09.54837.3649-22.

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A method for obtaining metallic plasmonic nanostructures with linear dichroism, based on the method of burning out constant spectral dips, is proposed. Isotropic granular silver films obtained by physical vapor deposition in vacuum were irradiated with linearly polarized laser radiation in the spectral region of the plasmon resonance of their constituent nanoparticles. As a result of irradiation, the silver nanostructures change their sizes and shapes, and the films acquire a pronounced linear dichroism. Both the magnitude and the spectrum of linear dichroism depend on the state of the isotropic film before irradiation, which can be changed by heat treatment. For the unannealed films the dichroism does not change the sign over the entire spectral range studied and corresponds to the expected increase in the depth of the spectral dip for the light polarized parallel to the laser radiation polarization plane. For the annealed films, which consist of more distinctly formed and better separated nanoparticles, the dichroism value is greater, and the spectrum turns out to be sign-changing. The appearance of linear dichroism after laser irradiation is due to the differences in the change in the shape and size of the initially anisotropic nanoparticles that make up an isotropic film as a whole, depending on their orientation relative to the polarization plane of the laser beam. Keywords: plasmon resonance, silver nanostructures, linear dichroism, laser radiation.

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18

Norden, Bengt, Mikael Kubista, and Tomas Kurucsev. "Linear dichroism spectroscopy of nucleic acids." Quarterly Reviews of Biophysics 25, no. 1 (1992): 51–170. http://dx.doi.org/10.1017/s0033583500004728.

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This review will consider solution studies of structure and interactions of DNA and DNA complexes using linear dichroism spectroscopy, with emphasis on the technique of orientation by flow. The theoretical and experimental background to be given may serve, in addition, as a general introduction into the state of the art of linear dichroism spectroscopy, particularly as it is applied to biophysical problems.

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19

ROSE, H. B., T. KINOSHITA, CH ROTH, F. U. HILLEBRECHT, and E. KISKER. "INFLUENCE OF PHOTOELECTRON DIFFRACTION ON MAGNETIC LINEAR DICHROISM." Surface Review and Letters 04, no. 05 (1997): 915–18. http://dx.doi.org/10.1142/s0218625x97001036.

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We studied the influence of photoelectron diffraction on magnetic linear dichroism and spin polarization in Co and Fe 3p photoemission excited by linearly polarized synchrotron radiation. We find a strong variation of the magnetic linear dichroism with emission direction. The spin polarization related to the spin–orbit interaction varies in a similar manner. This angular variation closely tracks that of the magnetic dichroism. In contrast, the exchange-induced spin polarization (-12+2)% does not vary appreciably with emission angle. These findings suggest that the main cause for the observed effects is the angular momentum character of the photoelectron wave.

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20

Ingemey, R. A., G. Strohe, and W. S. Veeman. "Dynamic Infrared Linear Dichroic Spectra of Prestretched Polypropylene." Applied Spectroscopy 50, no. 11 (1996): 1360–65. http://dx.doi.org/10.1366/0003702963904746.

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DIRLD (dynamic infrared linear dichroic) spectra of prestretched isotactic polypropylene have been recorded. The line shape features in the in-phase spectra are described on the basis of frequency shifts and absorption amplitude variations during the stretching cycle. Details such as the dichroism of the bands, direction of the shift, and changes in the absorption intensities must be considered to explain signs and shapes of the DIRLD bands. Evidence for chain reorientations under stress has not been found. The general principle of frequency shifts and changes in absorption intensities as the origin of DIRLD bands is demonstrated by spectral simulations.

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21

Kaerkitcha, N., and T. Sagawa. "Amplified polarization properties of electrospun nanofibers containing fluorescent dyes and helical polymer." Photochemical & Photobiological Sciences 17, no. 3 (2018): 342–51. http://dx.doi.org/10.1039/c7pp00413c.

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Well-aligned nanofibers containing cationic fluorescent dyes and anionic chiral polymers prepared via electrospinning exhibit an enhanced circular dichroism, which is mainly caused by linear dichroism and linear birefringence.

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22

Polavarapu, Prasad L., Zhengyu Deng, and Gang-Chi Chen. "Polarization-Division Interferometry: Time-Resolved Infrared Vibrational Dichroism Spectroscopy." Applied Spectroscopy 49, no. 2 (1995): 229–36. http://dx.doi.org/10.1366/0003702953963797.

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We report the first direct measurements of time-resolved Fourier transform infrared vibrational dichroism (TR/FT-IR/VD). The central component for these measurements is a polarization-division interferometer (PDI). This interferometer uses an in-house-designed beamsplitter constructed in-house from a BaF2 polarizer and a matching substrate. In conjunction with a linear polarizer in front of the source and two rooftop mirrors, one in each arm of the interferometer, the PDI divides the input beam into two orthogonal linear polarization components, recombines them for interference at the beamsplitter, and directs the output beam at 90° to the direction of input beam. The signals measured as a function of the moving mirror position in the PDI represent the linear/circular dichroism interferograms, whose cosine/sine Fourier transforms yield linear/circular dichroism spectra. Time-resolved dichroism interferograms were measured with the use of this PDI with the asynchronous external perturbation method. Microsecond time-resolved linear dichroism spectra of a nematic liquid crystal, under the influence of bipolar electric field oscillating at 2 kHz, were measured and presented as the first examples.

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23

Matsuo, Koichi, Hirofumi Namatame, Masaki Taniguchi, and Kunihiko Gekko. "3P014 Membrane-Induced Conformations of Proteins Characterized by Vacuum-Ultraviolet Circular-Dichroism and Flow Linear-Dichroism(01A. Protein: Structure,Poster)." Seibutsu Butsuri 53, supplement1-2 (2013): S214. http://dx.doi.org/10.2142/biophys.53.s214_2.

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24

Rustam, Ya, B. Bakhodir, M. Ikbol, and N. Shokhrukh. "ON THE THEORY OF ONE-PHOTON ABSORPTION OF POLARIZED LIGHT IN NARROW-GAP CRYSTALS. TAKING INTO ACCOUNT THE EFFECT OF COHERENT SATURATION." EurasianUnionScientists 5, no. 1(82) (2021): 56–59. http://dx.doi.org/10.31618/esu.2413-9335.2021.5.82.1235.

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In the article, from a microscopic point of view, the linear-circular dichroism of one-photon between band absorption of light in the Kane approximation in narrow-gap crystals is investigated. The linear-circular dichroism of one-photon absorption of polarized light is calculated taking into account the effect of coherent saturation in photoexcited charge carriers. The matrix elements of one-photon interband optical transitions and the corresponding linear-circular dichroism and the spectral dependence of the light absorption coefficient are calculated.

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25

Dimitrov, Stephan I., Ivan V. Smirnov, and Vladimir L. Makarov. "Optical Anisotropy of Chromatin. Flow Linear Dichroism and Electric Dichroism Studies." Journal of Biomolecular Structure and Dynamics 5, no. 5 (1988): 1135–48. http://dx.doi.org/10.1080/07391102.1988.10506454.

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26

Stifler, Cayla A., Nina Kølln Wittig, Michel Sassi, et al. "X-ray Linear Dichroism in Apatite." Journal of the American Chemical Society 140, no. 37 (2018): 11698–704. http://dx.doi.org/10.1021/jacs.8b05547.

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27

Krichevtsov, B. B. "Linear nonreciprocal dichroism in boracite Co3B7O13I." Journal of Experimental and Theoretical Physics Letters 74, no. 3 (2001): 159–63. http://dx.doi.org/10.1134/1.1410221.

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28

van der Laan, G., and E. Arenholz. "Anisotropic X-ray magnetic linear dichroism." European Physical Journal Special Topics 169, no. 1 (2009): 187–90. http://dx.doi.org/10.1140/epjst/e2009-00991-x.

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29

Petriashvili, Gia, Ridha Hamdi, Maria Penelope De Santo, Ramla Gary, and Riccardo Barberi. "Light-controllable linear dichroism in nematics." Applied Optics 54, no. 28 (2015): 8293. http://dx.doi.org/10.1364/ao.54.008293.

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30

Grum-Grzhimailo, A. N., and N. M. Kabachnik. "Linear magnetic dichroism in fluorescence spectra." Physics Letters A 264, no. 2-3 (1999): 192–97. http://dx.doi.org/10.1016/s0375-9601(99)00800-2.

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31

Brunetti, A., M. Vladimirova, S. Cronenberger, D. Scalbert, M. Nawrocki, and J. Bloch. "Linear dichroism in a GaAs microcavity." Superlattices and Microstructures 41, no. 5-6 (2007): 429–33. http://dx.doi.org/10.1016/j.spmi.2007.03.025.

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32

van der Laan, Gerrit. "Non-reciprocal X-ray linear dichroism." Journal of Synchrotron Radiation 8, no. 3 (2001): 1059–60. http://dx.doi.org/10.1107/s0909049501000899.

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33

Bulheller, B. M., and J. D. Hirst. "DichroCalc--circular and linear dichroism online." Bioinformatics 25, no. 4 (2009): 539–40. http://dx.doi.org/10.1093/bioinformatics/btp016.

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34

Bulheller, Benjamin M., Alison Rodger, and Jonathan D. Hirst. "Circular and linear dichroism of proteins." Physical Chemistry Chemical Physics 9, no. 17 (2007): 2020. http://dx.doi.org/10.1039/b615870f.

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35

Hillebrecht, F. U., H. B. Rose, T. Kinoshita, et al. "Photoelectron Diffraction in Magnetic Linear Dichroism." Physical Review Letters 75, no. 15 (1995): 2883–86. http://dx.doi.org/10.1103/physrevlett.75.2883.

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36

Cheng, Bo, Yuxiao Zou, and Guofeng Song. "Full Stokes Mid-Wavelength Infrared Polarization Photodetector Based on the Chiral Dielectric Metasurface." Photonics 11, no. 6 (2024): 571. http://dx.doi.org/10.3390/photonics11060571.

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Conventional imaging techniques can only record the intensity of light while polarization imaging can record the polarization of light, thus obtaining a higher dimension of image information. We use the COMSOL software to numerically propose a circular polarization photodetector composed of the dislocated 2-hole Si chiral metasurfaces controlling the circular polarization lights and the HgCdTe (MCT) photodetector chip to detect the intensity of light signals. The chiral metasurfaces can be equated to a significant radiation source of the Z-type current density under the right circularly polarized incidence conditions, which explains the large circular dichroism (CD) of absorption of 95% in chiral photodetectors. In addition, the linear dichroism (LD) of the linear polarization pixel is 0.62, and the extinction ratio (ER) is 21 dB. The full Stokes pixel using the six-image-element technique can almost measure arbitrary polarization information of light at 4 μm operation wavelength. Our results highlight the potential of circular dichroic metasurfaces as photonic manipulation platforms for miniaturized polarization detectors.

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37

Olesiak-Banska, Joanna, Magdalena Waszkielewicz, and Marek Samoc. "Two-photon chiro-optical properties of gold Au25 nanoclusters." Physical Chemistry Chemical Physics 20, no. 38 (2018): 24523–26. http://dx.doi.org/10.1039/c8cp05256e.

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38

Brotin, Thierry, Jacek Waluk, Jean-Pierre Desvergne, Henri Bouas-Laurent, and Josef Michl. "ELECTRONIC ABSORPTION PROPERTIES OF SYMMETRICAL DIALKOXYANTHRACENES. LINEAR DICHROISM AND MAGNETIC CIRCULAR DICHROISM." Photochemistry and Photobiology 55, no. 3 (1992): 335–47. http://dx.doi.org/10.1111/j.1751-1097.1992.tb04246.x.

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39

Seixas, Leandro. "Enhanced linear dichroism of flattened-edge black phosphorus nanoribbons." Journal of Physics: Condensed Matter 34, no. 22 (2022): 225701. http://dx.doi.org/10.1088/1361-648x/ac5d18.

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Abstract Black phosphorus is a material with an intrinsic anisotropy in electronic and optical properties due to its puckered honeycomb lattice. Optical absorption is different for incident light with linear polarization in the armchair and zigzag directions (linear dichroism). These directions are also used in the cuts of materials to create black phosphorus nanoribbons. Edges of nanoribbons usually have small reconstruction effects, with minor electronic effects. Here, we show a reconstruction of the armchair edge that introduces a new valence band, which flattens the puckered lattice and increases the linear dichroism extrinsically in the visible spectrum. This enhancement in linear dichroism is explained by the polarization selection rule, which considers the parity of the wave function to a reflection plane. The flattened-edge reconstruction originates from the inversion of chirality of the P atoms at the edges and significantly alters the entire optical absorption of the material. The flattened edges have potential applications in pseudospintronics, photodetectors and might provide new functionalities in optoelectronic and photonic devices.

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40

Koev, M. S. "Propagation of privileged waves in longitudinally inhomogeneous medium with linear birefringence and dichroism." Semiconductor Physics Quantum Electronics and Optoelectronics 17, no. 4 (2014): 403–7. http://dx.doi.org/10.15407/spqeo17.04.403.

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41

Fu, Juxia, and Stephen G. Urquhart. "Linear Dichroism in the X-ray Absorption Spectra of Linearn-Alkanes." Journal of Physical Chemistry A 109, no. 51 (2005): 11724–32. http://dx.doi.org/10.1021/jp053016q.

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42

McCarthy, Lauren A., Kyle W. Smith, Xiang Lan, et al. "Polarized evanescent waves reveal trochoidal dichroism." Proceedings of the National Academy of Sciences 117, no. 28 (2020): 16143–48. http://dx.doi.org/10.1073/pnas.2004169117.

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Matter’s sensitivity to light polarization is characterized by linear and circular polarization effects, corresponding to the system’s anisotropy and handedness, respectively. Recent investigations into the near-field properties of evanescent waves have revealed polarization states with out-of-phase transverse and longitudinal oscillations, resulting in trochoidal, or cartwheeling, field motion. Here, we demonstrate matter’s inherent sensitivity to the direction of the trochoidal field and name this property trochoidal dichroism. We observe trochoidal dichroism in the differential excitation of bonding and antibonding plasmon modes for a system composed of two coupled dipole scatterers. Trochoidal dichroism constitutes the observation of a geometric basis for polarization sensitivity that fundamentally differs from linear and circular dichroism. It could also be used to characterize molecular systems, such as certain light-harvesting antennas, with cartwheeling charge motion upon excitation.

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43

Mizokawa, Takashi. "Photoemission Linear Dichroism Reveals Cubic Wave Functions." JPSJ News and Comments 12 (January 15, 2015): 08. http://dx.doi.org/10.7566/jpsjnc.12.08.

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44

Sato, K., Y. Ueji, K. Okitsu, et al. "Hard X-ray Magnetic Linear Dichroism Imaging." Transactions of the Magnetics Society of Japan 2, no. 4 (2002): 238–39. http://dx.doi.org/10.3379/tmjpn2001.2.238.

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45

Blechschmidt, J., D. C. Kleb, and H. J. Weber. "Strain-induced linear dichroism in YBa2Cu3O7- deltafilms." Superconductor Science and Technology 7, no. 11 (1994): 801–4. http://dx.doi.org/10.1088/0953-2048/7/11/004.

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46

Chen, Q., D. J. Frankel, C. W. Lee, and N. V. Richardson. "Linear dichroism electron scattering from chiral surfaces." Chemical Physics Letters 349, no. 3-4 (2001): 167–71. http://dx.doi.org/10.1016/s0009-2614(01)01170-8.

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47

Ito, Y., M. van Veenendaal, R. E. Cook, N. Menon, B. D. Armstrong, and D. J. Miller. "Nanometer Scale Magnetic Linear Dichroism by EELS." Microscopy and Microanalysis 9, S02 (2003): 314–15. http://dx.doi.org/10.1017/s1431927603441573.

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48

Mishra, S. R., T. R. Cummins, G. D. Waddill, et al. "Linear dichroism and resonant photoemission in Gd." Journal of Magnetism and Magnetic Materials 198-199 (June 1999): 647–49. http://dx.doi.org/10.1016/s0304-8853(98)01104-4.

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49

Zeybek, O., N. P. Tucker, S. D. Barrett, H. A. Dürr, and G. van der Laan. "Magnetic linear dichroism in gadolinium 4f satellites." Journal of Magnetism and Magnetic Materials 198-199 (June 1999): 650–52. http://dx.doi.org/10.1016/s0304-8853(98)01174-3.

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50

Cherepkov, N. A., and G. Schönhense. "Linear Dichroism in Photoemission from Oriented Molecules." Europhysics Letters (EPL) 24, no. 2 (1993): 79–85. http://dx.doi.org/10.1209/0295-5075/24/2/001.

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