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Journal articles on the topic 'Linearly polarized field'

Author: Grafiati

Published: 28 May 2022

Last updated: 30 July 2025

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1

Chen, Cong, Zhensheng Tao, Carlos Hernández-García, et al. "Tomographic reconstruction of circularly polarized high-harmonic fields: 3D attosecond metrology." Science Advances 2, no. 2 (2016): e1501333. http://dx.doi.org/10.1126/sciadv.1501333.

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Bright, circularly polarized, extreme ultraviolet (EUV) and soft x-ray high-harmonic beams can now be produced using counter-rotating circularly polarized driving laser fields. Although the resulting circularly polarized harmonics consist of relatively simple pairs of peaks in the spectral domain, in the time domain, the field is predicted to emerge as a complex series of rotating linearly polarized bursts, varying rapidly in amplitude, frequency, and polarization. We extend attosecond metrology techniques to circularly polarized light by simultaneously irradiating a copper surface with circul

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2

Milošević, Dejan. "Atomic and Molecular Processes in a Strong Bicircular Laser Field." Atoms 6, no. 4 (2018): 61. http://dx.doi.org/10.3390/atoms6040061.

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With the development of intense femtosecond laser sources it has become possible to study atomic and molecular processes on their own subfemtosecond time scale. Table-top setups are available that generate intense coherent radiation in the extreme ultraviolet and soft-X-ray regime which have various applications in strong-field physics and attoscience. More recently, the emphasis is moving from the generation of linearly polarized pulses using a linearly polarized driving field to the generation of more complicated elliptically polarized polychromatic ultrashort pulses. The transverse electrom

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3

Skulkin, Sergey P., Nikolai A. Lysenko, Grigoriy K. Uskov, Nikolai I. Kashcheev, and Ksenia V. Smuseva. "Linearly polarized field of a flat aperture." Physics of Wave Processes and Radio Systems 26, no. 1 (2023): 18–27. http://dx.doi.org/10.18469/1810-3189.2023.26.1.18-27.

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The article analyzes a flat circular aperture and proposes to use a new analytical expression that describes the radiation pattern of an elementary radiator of an antenna aperture depending on time and integration angle. The formula presented in the paper can be applied to any flat section of the aperture without taking into account its shape. A new equation for the antiderivative function of the impulse response of a circular aperture is presented in the form of an elliptic integral of the second kind. It is shown that the theoretically calculated results are in good agreement with numerical

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4

Yachin, V., T. Zinenko, L. Kochetova, P. Mladyonov, and S. Mizrakhy. "POLARIZATION AND FREQUENCY SELECTIVE CHARACTERISTICS OF A CHIRAL METASURFACE COMPOSED OF PERIODICALLY ARRANGED SQUARE DIELECTRIC HELICES." RADIO PHYSICS AND RADIO ASTRONOMY 28, no. 4 (2023): 287–94. http://dx.doi.org/10.15407/rpra28.04.287.

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Subject and Purpose. The present study is concerned with the linearly polarized electromagnetic wave transmission through a chiral metasurface composed of periodically assembled square dielectric helices. We expect that the metasurface of the kind has a wider range of functional capabilities to transform a polarized wave into a cross-polarized one when compared to a similar metasurface composed of metal helices. Methods and Methodology. To find the scattering coefficients of the considered structure, the well-established method of integral functionals is followed. A set of volume integral equa

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5

Zyoud, Samer H., Atef Abdelkader, Ahed H. Zyoud, and Araa Mebdir Holi. "Influence of Magnetic Field on Level of Linearly Polarized Laser Beam Passing through Faraday Crystal." Defect and Diffusion Forum 408 (April 2021): 129–40. http://dx.doi.org/10.4028/www.scientific.net/ddf.408.129.

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Many natural materials have the ability to rotate the polarization level of linearly polarized laser beam and pass through it. This phenomenon is called optical activity. In the event that a light beam (linearly polarized) passes through an optically active material, such as a quartz crystal, and projected vertically on the optical axis, the output beam will be polarized equatorially, and the vibration level will rotate at a certain angle [1], [2], [3]. A number of crystals, liquids, solutions, and vapors rotate the electric field of linearly polarized light that passes through them [4], [5],

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6

Wasiq, Khudaidad, and Mohammad Tayeeb Qurdash. "The Investigating of the Effect of Magnetic Field on a Flint Glass for Optical Isolators Applications." International Journal of Biological, Physical and Chemical Studies 5, no. 2 (2023): 11–16. http://dx.doi.org/10.32996/ijbpcs.2023.5.2.2.

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In this study, the effect of a magnetic field on a Flint Glass for optical isolator applications has been reported. A flint glass and a laser light source with a wavelength of 650nm were used as a medium and a light source, respectively. The magnetic field was produced by applying a current through a coil. The linearly polarized light was passed through the medium in the presence of a magnetic field, and the angle of rotation was measured. The angle of rotation was plotted versus magnetic field strength and fitted linearly. The experimental results showed that the flint glass becomes optically

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7

Hu, Li, Hongxia Dai, Fayin Cheng, and Yuxia Tang. "Controllable and switchable chiral near-fields in symmetric graphene metasurfaces*." Chinese Physics B 30, no. 12 (2021): 127303. http://dx.doi.org/10.1088/1674-1056/ac2e5d.

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A strong chiral near-field plays significant roles in the detection, separation and sensing of chiral molecules. In this paper, a simple and symmetric metasurface is proposed to generate strong chiral near-fields with both circularly polarized light and linearly polarized light illuminations in the mid-infrared region. Owing to the near-field interaction between plasmonic resonant modes of two nanosheets excited by circularly polarized light, there is a strong single-handed chiral near-field in the gap between the two graphene nanosheets and the maximum enhancement of the optical chirality cou

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8

Hummel, E., and M. Dahlem. "The Magnetic Field in Edge-On Galaxies." Symposium - International Astronomical Union 140 (1990): 219–22. http://dx.doi.org/10.1017/s0074180900190035.

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9

Yang, Yi, and Siyuan Huang. "Trapping and rotation of microparticles using a metasurface exciting by linearly polarized beam." Nanomaterials and Nanotechnology 11 (January 1, 2021): 184798042110151. http://dx.doi.org/10.1177/18479804211015107.

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We numerically demonstrate trapping and rotation of particles using a metasurface formed by arranging nanocavities as a right-handed Archimedes’ spiral. Excited by a 90° linearly polarized beam, a focused surface plasmon polariton (SPP) field is formed at the center of the spiral, and the particle can be trapped by the field. While excited by −45° linearly polarized beams, a vortex SPP field carrying orbital angular momentum is formed, and the particles can be trapped and rotated in the clockwise direction at the vortex field.

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10

CH. ZHUKOVSKY, V., P. A. EMINOV, and A. E. GRIGORUK. "RADIATIVE DECAY OF A MASSIVE NEUTRINO IN THE WEINBERG–SALAM MODEL WITH MIXING IN A CONSTANT UNIFORM MAGNETIC FIELD." Modern Physics Letters A 11, no. 39n40 (1996): 3119–26. http://dx.doi.org/10.1142/s0217732396003106.

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Influence of an external magnetic field on the neutrino decay process with emission of a linearly polarized photon is considered. The decay rate is shown to be enhanced as compared to the free case in the broad region where both the nonvanishing neutrino mass and the field make substantial contributions. In the limit of a negligible neutrino mass the emitted photons are totally linearly polarized, which may help in the identification of these photons.

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11

Yuan, Jiadong, Zuyu Li, Yuhan Hong, Yuhang Zhang, Hongzhan Liu, and Zhongchao Wei. "Three-Channel Near-Field Display and Encryption Based on a Polarization Multiplexed Metasurface." Nanomaterials 13, no. 10 (2023): 1638. http://dx.doi.org/10.3390/nano13101638.

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Multichannel metasurfaces are becoming a significant trend in the field of optical encryption due to their excellent manipulation of optical wavefronts. However, existent multichannel metasurfaces for optical encryption mostly implement only two channels in the near-field, or three channels by combining the near- and far-field. In this paper, we propose and simulate a three-channel metasurface that works entirely in the near-field and uses the polarization state of the incident light, left circularly polarized (LCP) light, right circularly polarized (RCP) light, and linearly polarized (LP) lig

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12

Lu, Xiaotian, Kunpeng Xing, Siran Li, Ziyu Gu, and Lei Xin. "Theoretical Research on Large Field-of-View Polarization Imaging Based on Dynamic Vision Sensors." Photonics 12, no. 5 (2025): 426. https://doi.org/10.3390/photonics12050426.

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The combination of dynamic vision sensors (DVSs) and polarization can overcome the limitation of DVSs whereby they can only detect dynamic scenes, and it also has the ability to detect artificial targets and camouflaged targets, and is thus expected to become a new means of remote sensing detection. Remote sensing detection often requires the field-of-view (FOV) and width to be large enough to improve detection efficiency, but when large FOV polarization imaging is performed, the polarization state in the edge FOV and the center FOV will not be consistent, which does not meet the paraxial appr

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13

ARKA, IOANNA, and JOHN G. KIRK. "LINEARLY POLARIZED SUPERLUMINAL WAVES IN PULSAR WINDS." International Journal of Modern Physics: Conference Series 08 (January 2012): 96–101. http://dx.doi.org/10.1142/s2010194512004461.

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Pulsar winds are the ideal environment for the study of non-linear electromagnetic waves. It is generally thought that a pulsar launches a striped wind, a magnetohydrodynamic entropy wave, where plasma sheets carried along with the flow separate regions of alternating magnetic field. But when the density drops below a critical value, or equivalently for distances from the pulsar greater than a critical radius, a strong superluminal wave can also propagate. In this contribution we discuss the conversion of the equatorial striped wind into a linearly polarized superluminal wave, and we argue tha

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14

Lu, Fanfan, Tengxiang Huang, Lei Han, et al. "Tip-Enhanced Raman Spectroscopy with High-Order Fiber Vector Beam Excitation." Sensors 18, no. 11 (2018): 3841. http://dx.doi.org/10.3390/s18113841.

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We investigated tip-enhanced Raman spectra excited by high-order fiber vector beams. Theoretical analysis shows that the high-order fiber vector beams have stronger longitudinal electric field components than linearly polarized light under tight focusing conditions. By introducing the high-order fiber vector beams and the linearly polarized beam from a fiber vector beam generator based on an electrically-controlled acoustically-induced fiber grating into a top-illumination tip-enhanced Raman spectroscopy (TERS) setup, the tip-enhanced Raman signal produced by the high-order fiber vector beams

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15

Hsu, Julia W. P., E. B. McDaniel, and S. C. McClain. "Development of Polarization Modulation Near-Field Scanning Optical Microscope and its Application to Mapping Defect-Induced Birefringence in SrTiO3 Bicrystals." Microscopy and Microanalysis 4, S2 (1998): 314–15. http://dx.doi.org/10.1017/s1431927600021693.

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Photoelastic measurement is a sensitive optical technique to map strain fields in otherwise isotropic materials. To extend this method to the submicron scale, we combine dynamic polarimetry with nearfield scanning optical microscopy (NSOM) and construct a polarization modulation NSOM (PMNSOM). The 670 nm laser light passes first through a linear polarizer (oriented at 90°), and then through a photoelastic modulator (PEM), and finally through a quarter wave plate. The PEM introduces a sinusoidally time varying phase shift δ0sin(2πft) into the +45° polarization component, where the modulation fr

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16

van Duijn, Ernst, and H. G. Muller. "Detachment rates ofH2−in an intense linearly polarized laser field." Physical Review A 59, no. 2 (1999): 1423–33. http://dx.doi.org/10.1103/physreva.59.1423.

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17

Zhou Guo-Quan. "Far-field divergent properties of linearly polarized Laguerre-Gauss beams." Acta Physica Sinica 61, no. 2 (2012): 024208. http://dx.doi.org/10.7498/aps.61.024208.

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18

Saraswat, Kapil, and A. R. Harish. "A polarization and band reconfigurable cross-slot antenna for multiband application." International Journal of Microwave and Wireless Technologies 11, no. 10 (2019): 1054–60. http://dx.doi.org/10.1017/s1759078719000758.

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AbstractA polarization and band reconfigurable cross-slot antenna for multiband applications is presented in this paper. The antenna consists of four p–i–n diodes embedded in the cross-shaped slot in a ground plane and excited by a microstrip feed line. The p–i–n diodes are placed in such a way that they produce multiple bands, with linearly and circularly polarized (CP) radiation. By switching the states of the p–i–n diodes, the sense of rotation of the electric field in CP radiation can be reconfigured. The proposed structure can be configured to produce two bands that radiate linearly polar

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19

Kumar, Rajkishor, Avinash Chandra, Naveen Mishra, and Raghvendra Kumar Chaudhary. "A Frequency Tunable Dielectric Resonator Antenna with Reduction of Cross Polarisation for Wi MAX and Sub 6 GHz 5G Applications." Defence Science Journal 73, no. 4 (2023): 475–86. http://dx.doi.org/10.14429/dsj.73.18180.

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A frequency Tunable (mechanical tuning) Linearly Polarized (TLP) rectangular Dielectric Resonator Antenna(DRA) coupled with a horizontal/vertical-slot and excited with circular-ring type feed is investigated in this article.The frequency tunability (mechanical tuning) is achieved by the rotation of slot at different angles of the proposedstructure. Hence, two linearly polarized antennas have been proposed for different frequency bands such as Wi-MAX and Sub-6 GHz/5G, respectively, using slot variations (named as DRA-1 and DRA-2). TE 11δ mode has been excited in both the DRAs and confirmed by o

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20

GALLAGHER, T. F. "IONIZATION OF RYDBERG ATOMS BY CIRCULARLY POLARIZED MICROWAVE FIELDS." Modern Physics Letters B 05, no. 04 (1991): 259–72. http://dx.doi.org/10.1142/s0217984991000307.

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In circularly polarized microwave fields of frequencies in the vicinity of 10 GHz ionization of Na Rydberg atoms occurs at a field E=1/16n4, up to principal quantum number n=50. This field is equal to the classical field for ionization and the static field required to ionize a Na atom. On the other hand, this field is far below the linearly polarized 10 GHz field required to ionize Na atoms, E=1/3n5. If the problem is transformed to a frame rotating with the microwave field, the field becomes a static field. In this case it is straightforward to calculate the ionization field classically. Howe

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21

Ramanantoanina, Harry, Michał Studniarek, Niéli Daffé, and Jan Dreiser. "Non-empirical calculation of X-ray magnetic circular dichroism in lanthanide compounds." Chemical Communications 55, no. 20 (2019): 2988–91. http://dx.doi.org/10.1039/c8cc09321k.

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22

Safin, Ansar, Sergey Nikitov, Andrei Kirilyuk, Vasyl Tyberkevych, and Andrei Slavin. "Theory of Antiferromagnet-Based Detector of Terahertz Frequency Signals." Magnetochemistry 8, no. 2 (2022): 26. http://dx.doi.org/10.3390/magnetochemistry8020026.

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We present a theory of a detector of terahertz-frequency signals based on an antiferromagnetic (AFM) crystal. The conversion of a THz-frequency electromagnetic signal into the DC voltage is realized using the inverse spin Hall effect in an antiferromagnet/heavy metal bilayer. An additional bias DC magnetic field can be used to tune the antiferromagnetic resonance frequency. We show that if a uniaxial AFM is used, the detection of linearly polarized signals is possible only for a non-zero DC magnetic field, while circularly polarized signals can be detected in a zero DC magnetic field. In contr

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23

Karbstein, Felix, and Elena A. Mosman. "Photon polarization tensor in circularly polarized Hermite- and Laguerre-Gaussian beams." Modern Physics Letters A 33, no. 07n08 (2018): 1850044. http://dx.doi.org/10.1142/s021773231850044x.

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We derive analytical expressions for the photon polarization tensor in circularly polarized Hermite-Gaussian (HG) and Laguerre-Gaussian (LG) beams, complementing the corresponding results for linearly polarized beams obtained recently. As they are based upon a locally constant field approximation of the one-loop Heisenberg–Euler effective Lagrangian for quantum electrodynamics (QED) in constant fields, our results are generically limited to slowly varying electromagnetic fields, varying on spatial (temporal) scales much larger than the Compton wavelength (time) of the electron.

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24

FUKUOKA, DAISUKE, NAOKI TANAKA, KENICHI OTO, et al. "OPTICALLY INDUCED DYNAMIC NUCLEAR SPIN POLARIZATION IN QUANTUM HALL REGIME OBSERVED BY A TIME-RESOLVED KERR ROTATION." International Journal of Modern Physics B 23, no. 12n13 (2009): 2755–59. http://dx.doi.org/10.1142/s0217979209062311.

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The dynamics between electron and nuclear spins in quantum Hall regime is investigated by a time-resolved Kerr rotation (TRKR) spectroscopy carried down in tilted-field geometry. The spin-flip energy varies almost linearly with the applied magnetic field under the nuclear spin depolarizing radio frequency field and the helicity modulation of circularly polarized pump, while the spin-flip energy obtained under a circularly polarized pump deviates from linearly behavior. This deviation is ascribed to the Overhauser shift due to dynamic nuclear spin polarization (DNP). The DNP depends markedly on

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25

Middha, K., V. Thakur, N. Kant, and J. Rajput. "Periodic chirp electron acceleration due to linearly polarized lasers." Journal of Physics: Conference Series 2663, no. 1 (2023): 012050. http://dx.doi.org/10.1088/1742-6596/2663/1/012050.

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Abstract Laser beat wave electron acceleration scheme provides a number of distinct advantages and exciting possibilities in terms of high electron’s energy gain, compact accelerator design, versatility, high repetition rates and fundamental research. In this scheme, two linearly polarized lasers of same amplitude and the frequency have been considered propagating θ and − θ along the z axis with their electric field components in x and z axis respectively. Peak intensity is observed for resultant electric field at the crossing of both lasers at a focal spot. At this focus, constructive interfe

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26

XU, J. J., Q. KONG, Z. CHEN, et al. "Polarization effect of fields on vacuum laser acceleration." Laser and Particle Beams 25, no. 2 (2007): 253–57. http://dx.doi.org/10.1017/s0263034607000092.

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Concerning laser-driven electron acceleration in vacuum, a comparison was made between using circularly polarized (CP) laser field and linearly polarized (LP) field. It has been found that the main advantage for using CP field is that its acceleration channel occupies relatively larger phase space, which can give rise to greater acceleration efficiency. This feature chiefly comes from the difference in the distribution of the longitudinal electric components of these two kinds of fields. One of the disadvantages with CP field is the “energy saturation” phenomenon as the laser intensity is suff

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27

Pengfei, Lan, Lu Peixiang, and Cao Wei. "Spatial Characteristics of Thomson Scattering in a Linearly Polarized Laser Field." Plasma Science and Technology 9, no. 2 (2007): 143–46. http://dx.doi.org/10.1088/1009-0630/9/2/05.

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28

Komarov, V. N. "Motion invariants for a charge in a linearly polarized wave field." Technical Physics 46, no. 1 (2001): 117–18. http://dx.doi.org/10.1134/1.1340896.

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29

Dvornikov, M. S., and A. I. Studenikin. "Neutrino oscillations in the field of a linearly polarized electromagnetic wave." Physics of Atomic Nuclei 64, no. 9 (2001): 1624–27. http://dx.doi.org/10.1134/1.1409503.

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30

Formanek, Martin, Andrew Steinmetz, and Johann Rafelski. "Classical neutral point particle in linearly polarized EM plane wave field." Plasma Physics and Controlled Fusion 61, no. 8 (2019): 084006. http://dx.doi.org/10.1088/1361-6587/ab242e.

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31

Kalinski, Maciej, and J. H. Eberly. "Nonspreading Rydberg wave packets supported by a linearly polarized electromagnetic field." Physical Review A 52, no. 5 (1995): 4285–88. http://dx.doi.org/10.1103/physreva.52.4285.

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32

Collins, L. A., and G. Csanak. "Multiphoton resonances ine+H+scattering in a linearly polarized radiation field." Physical Review A 44, no. 9 (1991): R5343—R5345. http://dx.doi.org/10.1103/physreva.44.r5343.

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33

Kadzhaya, I. M., and G. B. Furman. "Topological phase for spin systems in a linearly polarized RF field." Radiophysics and Quantum Electronics 34, no. 3 (1991): 287–89. http://dx.doi.org/10.1007/bf01066517.

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34

Lin, Zhan-Hong, Jiwei Zhang, and Jer-Shing Huang. "Plasmonic elliptical nanoholes for chiroptical analysis and enantioselective optical trapping." Nanoscale 13, no. 20 (2021): 9185–92. http://dx.doi.org/10.1039/d0nr09080h.

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35

Ren, Yuhu, Jimo Jian, Wenjiang Tan, et al. "Polarization state transition mechanism of light through turbid media by Monte Carlo simulation." Laser Physics 34, no. 2 (2024): 026001. http://dx.doi.org/10.1088/1555-6611/ad1fe9.

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Abstract We study the propagation of polarized light through turbid media with high scattering coefficient (μ s = 50 cm−1) and disclose the physical processes involved in the evolution of Stokes vector. The results show that the components of the Stokes vector can be expressed as the superimposition of the generalized divergence and the generalized curl of the two orthogonal electric field vectors. The components I, Q, and U can be represented as the superimposition of the generalized divergence. The components V can be conveyed as the superimposition of the generalized curl omitting the direc

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36

Кухарь, Е. И., та С. В. Крючков. "Фотоиндуцированное состояние Флоке-изолятора в графеноподобном кристалле". Журнал технической физики 92, № 3 (2022): 337. http://dx.doi.org/10.21883/jtf.2022.03.52128.280-21.

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Floquet spectrum of charge carriers in a 2D crystal with initially displaced Dirac points has been derived. The phase and amplitude dependences of the energy gap induced by elliptically polarized and bichromatic high-frequency fields has been investigated. In contrast to graphene the linearly polarized electric field has been shown to be able to transform the initially semi-metallic state of Dirac crystal into the Floquet-insulator state. The conditions for such a transition are indicated, one of which is the mismatch between the orientation of the field polarization line and the direction of

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37

Eid, D. A. M., and L. Shafai. "Synthesis of line-source feeds for conical reflectors and their performance using dipole arrays." Canadian Journal of Physics 69, no. 6 (1991): 702–11. http://dx.doi.org/10.1139/p91-118.

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The matched feed concept is used to determine the electrical characteristics of a line-source feed for conical-reflector antennas. A linearly polarized plane wave incident on the reflector is used to determine the field distribution along and in the vicinity of the focal axis of the reflector. The co-polar, cross-polar, and axial field components are determined and their dependence on reflector size, cone angle, and radial distance is studied. The results indicate that for a line source of finite diameter, its surface field distribution must contain other field components to generate a linearl

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Degner, Shelee L., and Craig W. Hawryshyn. "Orientation of rainbow trout (Oncorhynchus mykiss) to multiple patches of linearly polarized light." Canadian Journal of Zoology 79, no. 3 (2001): 407–15. http://dx.doi.org/10.1139/z00-221.

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Orientation responses of juvenile rainbow trout (Oncorhynchus mykiss) to two linearly polarized light patches were examined under controlled laboratory conditions. Fish were trained to swim the length of the training tank under a polarized light field created by two linearly polarized stimuli that were oriented either parallel or perpendicular to the length of the tank. Trained fish were released in a circular tank and their angular responses were recorded. For each testing paradigm, the E-vector (electric vector) orientation of one of the two linearly polarized light patches was varied by 15°

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Kotlyar, V. V., A. G. Nalimov, and S. S. Stafeev. "Comparison of backward flow values in the sharp focus of light fields with polarization and phase singularity." Computer Optics 43, no. 2 (2019): 174–83. http://dx.doi.org/10.18287/2412-6179-2019-43-2-174-183.

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Using Jones matrices and vectors, we show that an optical metasurface composed of a set of subwavelength binary diffraction gratings and characterized by an anisotropic transmittance described by a polarization rotation matrix by the angle mφ, where φ is the polar angle, forms an m-th order azimuthally or radially polarized beam when illuminated by linearly polarized light, generating an optical vortex with the topological charge m upon illumination by circularly polarized light. Such a polarization-phase converter (PPC) performs a spin-orbit transformation, similar to that performed by liquid

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Li, Shaobo, Shuming Yang, Fei Wang, Qiang Liu, Biyao Cheng, and Yossi Rosenwaks. "Plasmonic interference modulation for broadband nanofocusing." Nanophotonics 10, no. 16 (2021): 4113–23. http://dx.doi.org/10.1515/nanoph-2021-0405.

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Abstract Metallic plasmonic probes have been successfully applied in near-field imaging, nanolithography, and Raman enhanced spectroscopy because of their ability to squeeze light into nanoscale and provide significant electric field enhancement. Most of these probes rely on nanometric alignment of incident beam and resonant structures with limited spectral bandwidth. This paper proposes and experimentally demonstrates an asymmetric fiber tip for broadband interference nanofocusing within its full optical wavelengths (500–800 nm) at the nanotip with 10 nm apex. The asymmetric geometry consisti

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Mäthger, Lydia M., Kenneth J. Lohmann, Colin J. Limpus, and Kerstin A. Fritsches. "An unsuccessful attempt to elicit orientation responses to linearly polarized light in hatchling loggerhead sea turtles ( Caretta caretta )." Philosophical Transactions of the Royal Society B: Biological Sciences 366, no. 1565 (2011): 757–62. http://dx.doi.org/10.1098/rstb.2010.0212.

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Sea turtles undertake long migrations in the open ocean, during which they rely at least partly on magnetic cues for navigation. In principle, sensitivity to polarized light might be an additional sensory capability that aids navigation. Furthermore, polarization sensitivity has been linked to ultraviolet (UV) light perception which is present in sea turtles. Here, we tested the ability of hatchling loggerheads ( Caretta caretta ) to maintain a swimming direction in the presence of broad-spectrum polarized light. At the start of each trial, hatchling turtles, with their magnetic sense temporar

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Kuri, Deep Kumar, Nilakshi Das, and Kartik Patel. "Collimated proton beams from magnetized near-critical plasmas." Laser and Particle Beams 36, no. 3 (2018): 276–85. http://dx.doi.org/10.1017/s0263034618000307.

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AbstractGeneration of collimated proton beams by linearly and circularly polarized (CP) lasers from magnetized near-critical plasmas has been investigated with the help of three-dimensional (3D) particle-in-cell (PIC) simulations. Due to cyclotron effects, the transverse proton momentum gets significantly reduced in the presence of an axial magnetic field which leads to an enhancement in collimation. Collimation is observed to be highest in case of a linearly polarized (LP) laser in the presence of magnetic field. However, protons accelerated by a right CP laser in the presence of magnetic fie

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Smolyansky, S. A., A. M. Fedotov, and V. V. Dmitriev. "Kinetics of the vacuum e−e+ plasma in a strong electric field and problem of radiation." Modern Physics Letters A 35, no. 03 (2020): 2040028. http://dx.doi.org/10.1142/s0217732320400283.

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We consider a quantum kinetic equation for [Formula: see text] plasma created from vacuum under the action of a strong time-dependent linearly polarized electric field. Simplification of the collision integral for photon emission along the polarization direction of the field is discussed.

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He, Yang, Burabigul Yakup та Mamat Ali Bake. "Linearly Polarized γ Photon Generation from Unpolarized Electron Bunch Interacting with Laser". Applied Sciences 15, № 1 (2025): 481. https://doi.org/10.3390/app15010481.

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Highly polarized high-energy γ photons demonstrate potential application in the efficient detection of strong-field quantum electrodynamics effects. Currently, polarized γ-rays are mostly generated in conventional particle accelerators, which are typically huge and expensive. This study proposes a scheme for generating linearly polarized γ photons from the interaction of a GeV-level unpolarized electron bunch with currently available laser pulses at moderate intensity. We investigate the scheme by considering the electron bunch of various initial energies and various laser intensities using tw

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45

Zurrón-Cifuentes, Óscar, Sergio Martín-Doménech, Ana García-Cabrera, Carlos Hernández-García, and Luis Plaja. "Ultrafast magnetic field induced by anisotropy in carbon nanotubes irradiated by intense laser fields." EPJ Web of Conferences 309 (2024): 07016. http://dx.doi.org/10.1051/epjconf/202430907016.

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We report an unexpected result of the anisotropy of the nonlinear optical response of carbon nanotubes, inherent to their chirality. Using a model based on the resolution of the semiconductor Bloch equations, we theoretically demonstrate that, upon irradiation with an intense linearly polarized laser pulse along the axial direction, chiral nanotubes exhibit an oscillating azimuthal current that is absent in achiral species. This current induces a magnetic field parallel to the axis of the nanotube that radiates like a loop antenna.

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Грачев, А. И. "Вращение атомно-молекулярной частицы, находящейся в поле линейно поляризованной световой волны и постоянном электрическом или магнитном поле". Письма в журнал технической физики 48, № 18 (2022): 28. http://dx.doi.org/10.21883/pjtf.2022.18.53395.19281.

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Rotation mechanisms of an atomic-molecular particle being into the linearly polarized light field and applied static electric or magnetic fields are for the first time shortly analyzed. Exerting of the particle torque is based on the dynamic molecular Hall effect, distinctive features of which are able to expand the resource of the optical-mechanical manipulation by molecular objects.

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Gavrilenko, V. P., and E. Oks. "Nonexistence of a “local suppression” in the ionization of hydrogen atoms by a low-frequency laser field of arbitrary strength." Canadian Journal of Physics 89, no. 8 (2011): 849–55. http://dx.doi.org/10.1139/p11-064.

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Further development of an analytical model for the tunneling ionization of atoms using a low-frequency laser field of arbitrary strength, including the strong-field region, is presented. The model uses a very accurate approximation of the true ionization barrier–potential in the Schrödinger equation by the effective parabolic barrier–potential based on the algorithm suggested by Miller and Good and later employed by Kulyagin and Taranukhin (KT) for calculating the ionization rate, W(F), of hydrogen atoms from the ground state by a linearly polarized laser field. We point out and eliminate a nu

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Gui, Jaime, José L. Leiva, Aurora Andújar, Jaap Groot, Joan L. Pijoan, and Jaume Anguera. "Linearly Polarized Antenna Boosters versus Circularly Polarized Microstrip Patch Antennas for GPS Reception in IoT Devices." Energies 15, no. 24 (2022): 9623. http://dx.doi.org/10.3390/en15249623.

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GPS has become an attractive feature for geolocalization enabling asset tracking IoT devices. GPS satellite antennas radiate RHCP (right-hand circularly polarized) electromagnetic waves; thus, the typical antenna at the receiver is also RHCP. However, when the orientation of the receiving device is random, linear polarization antennas operate better in terms of TTFF (time to first fix). Through field measurements (urban and field) and considering different positions of the device in a vehicle, an RHCP microstrip patch antenna and a linear non-resonant antenna element called an antenna booster

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FURIS, MADALINA, TODD BARRICK, PATRICK ROBBINS, et al. "EXCITON SPIN STATES IN NANOCRYSTAL QUANTUM DOTS REVEALED BY SPIN-POLARIZED RESONANT PHOTOLUMINESCENCE AND RAMAN SPECTROSCOPY." International Journal of Modern Physics B 18, no. 27n29 (2004): 3769–74. http://dx.doi.org/10.1142/s0217979204027438.

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We performed spin-polarized resonant Raman and resonant photoluminescence excitation spectroscopy (also known as "fluorescence line narrowing") on ZnS -capped CdSe nanocrystal quantum dots in high magnetic fields to 33 Tesla and temperatures down to 1.7K, which allows detailed investigation of the excitonic spin states. In these experiments, spin-polarized electrons and holes are resonantly injected by circularly polarized light into colloidal quantum dots of specific size, using a narrowband tunable dye laser and a fiber-coupled probe that is specially-designed for use in high-field magnets.

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Repjar, A. G., A. C. Newell, and M. H. Francis. "Accurate determination of planar near-field correction parameters for linearly polarized probes." IEEE Transactions on Antennas and Propagation 36, no. 6 (1988): 855–68. http://dx.doi.org/10.1109/8.1189.

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