Relevant bibliographies by topics / Right hand circularly polarized

Contents

  1. Journal articles
  2. Dissertations / Theses
  3. Books
  4. Book chapters
  5. Conference papers
  6. Reports

Academic literature on the topic 'Right hand circularly polarized'

Author: Grafiati
Published: 4 June 2021
Last updated: 9 February 2022

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Journal articles on the topic "Right hand circularly polarized"

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Guo, Mengchao, Kan Zhou, Xiaokun Wang, Haiyan Zhuang, Dongming Tang, Baoshan Zhang, and Yi Yang. "Research of the impact of coupling between unit cells on performance of linear-to-circular polarization conversion metamaterial with half transmission and half reflection." International Journal of Modern Physics B 32, no. 10 (April 13, 2018): 1850124. http://dx.doi.org/10.1142/s0217979218501242.

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In this paper, the impact of coupling between unit cells on the performance of linear-to-circular polarization conversion metamaterial with half transmission and half reflection is analyzed by changing the distance between the unit cells. An equivalent electrical circuit model is then built to explain it based on the analysis. The simulated results show that, when the distance between the unit cells is 23 mm, this metamaterial converts half of the incident linearly-polarized wave into reflected left-hand circularly-polarized wave and converts the other half of it into transmitted left-hand circularly-polarized wave at 4.4 GHz; when the distance is 28 mm, this metamaterial reflects all of the incident linearly-polarized wave at 4.4 GHz; and when the distance is 32 mm, this metamaterial converts half of the incident linearly-polarized wave into reflected right-hand circularly-polarized wave and converts the other half of it into transmitted right-hand circularly-polarized wave at 4.4 GHz. The tunability is realized successfully. The analysis shows that the changes of coupling between unit cells lead to the changes of performance of this metamaterial. The coupling between the unit cells is then considered when building the equivalent electrical circuit model. The built equivalent electrical circuit model can be used to perfectly explain the simulated results, which confirms the validity of it. It can also give help to the design of tunable polarization conversion metamaterials.
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Khandelwal, Mukesh Kumar, Binod Kumar Kanaujia, Santanu Dwari, Sachin Kumar, and Anil Kumar Gautam. "Triple band circularly polarized compact microstrip antenna with defected ground structure for wireless applications." International Journal of Microwave and Wireless Technologies 8, no. 6 (March 12, 2015): 943–53. http://dx.doi.org/10.1017/s1759078715000288.

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Asymmetric slits loaded irregular shaped microstrip patch antenna with three different ground structures is proposed. All three antennas show triple band characteristics. First antenna with regular ground plane resonates at 1.95, 2.4, and 4.90 GHz with good radiation characteristics and shows right-hand circular polarization at 1.95 GHz. 18.75% of compactness is achieved with triple band characteristics. Further, same patch is used with different defected ground structures. Second antenna resonates at 1.85, 2.4, and 4.85 GHz with suppressed cross-polarization level and antenna shows right-hand circular polarization at 1.85 and 4.85 GHz. Compactness is further improved to the value of 22.91%. The third antenna resonates at 1.95, 2.4, and 4.85 GHz with better gain and radiation characteristics and antenna shows right-hand circular polarization at 1.95 and 2.4 GHz. The small frequency ratio f2/f1 is achieved and the value of f2/f1 is 1.29 and 1.23 for second and third configuration, respectively. Proposed structures show right-hand circularly polarized with suppressed left-hand circularly polarized radiations and suitable for fixed mobile wireless communication applications. All structures are analyzed using Ansoft HFSS v.14 based on finite element method and measured results satisfy the simulated results.
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Farahani, Mohammadmahdi, Mohammad Akbari, Mourad Nedil, Abdel-Razik Sebak, and Tayeb A. Denidni. "Millimeter-Wave Dual Left/Right-Hand Circularly Polarized Beamforming Network." IEEE Transactions on Antennas and Propagation 68, no. 8 (August 2020): 6118–27. http://dx.doi.org/10.1109/tap.2020.2986678.

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Vaidya, Avinash R., Rajiv K. Gupta, Sanjeev K. Mishra, and Jayanta Mukherjee. "Right-Hand/Left-Hand Circularly Polarized High-Gain Antennas Using Partially Reflective Surfaces." IEEE Antennas and Wireless Propagation Letters 13 (2014): 431–34. http://dx.doi.org/10.1109/lawp.2014.2308926.

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Röhricht, B., P. Eschle, S. Dangel, and R. Holzner. "Nonlinear Behavior of Circularly Polarized Laser Beams Propagating through Sodium Vapor." Zeitschrift für Naturforschung A 48, no. 5-6 (June 1, 1993): 621–23. http://dx.doi.org/10.1515/zna-1993-5-602.

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Abstract A variety of surprising effects arise from the nonlinear light-matter interaction of circularly polarized laser light propagating through sodium vapor. We present experimental evidence for an asymmetry in the absorption of left hand and right hand circularly polarized light as well as for the creation of a collimated light beam of apposite polarization within the light-matter interaction region. Both effects are not yet explained by common theories.
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Mjølhus, E., and T. Hada. "Oblique stability of circularly polarized MHD waves." Journal of Plasma Physics 43, no. 2 (April 1990): 257–68. http://dx.doi.org/10.1017/s002237780001477x.

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The stability of finite-amplitude weakly dispersive circularly polarized MHD wave trains with respect to oblique modulations is investigated. The mathematical model is a multi-dimensional extension of the DNLS equation. We have found that the right-hand-polarized wave, which is stable with respect to parallel modulations, is unstable with respect to certain oblique modulations for most primary wavenumbers.
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Nalimov, A. G., and E. S. Kozlova. "Inversion of the longitudinal component of spin angular momentum in the focus of a left-handed circularly polarized beam." Computer Optics 44, no. 5 (October 2020): 699–706. http://dx.doi.org/10.18287/2412-6179-co-761.

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It has been shown theoretically and numerically that in the sharp focus of a circularly polarized optical vortex, the longitudinal component of the spin angular momentum vector is inverted. Moreover, if the input light to the optical system is left-hand circularly polarized, it has been shown to be right-hand polarized in the focus near the optical axis. Since this effect occurs near the focus where a backward energy flow takes place, such an inversion of the spin angular momentum can be used to detect the backward energy flow.
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Etemadpour, R., and N. Sepehri Javan. "Effect of super-thermal ions and electrons on the modulation instability of a circularly polarized laser pulse in magnetized plasma." Laser and Particle Beams 33, no. 2 (April 8, 2015): 265–72. http://dx.doi.org/10.1017/s0263034615000117.

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AbstractThe modulation instability of a circularly polarized laser pulse in a magnetized non-Maxwellian plasma is investigated. Based on a relativistic fluid model, the nonlinear interaction of an intense circularly polarized laser beam with a non-Maxwellian magnetized plasma is described. Nonlinear dispersion relation and growth rate of the instability for left- and right-hand polarizations are derived. The effect of temperature, external magnetic field, value of Kappa and state of polarization on the growth rate are analyzed. It is shown that the growth rate increases with increase in the magnetic field for the right-hand polarization and inversely it decreases for the left-hand one. Also it is observed that existence of super-thermal particles causes the decrease in the growth.
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Akgol, Oguzhan, Olcay Altintas, Emin Unal, Muharrem Karaaslan, and Faruk Karadag. "Linear to left- and right-hand circular polarization conversion by using a metasurface structure." International Journal of Microwave and Wireless Technologies 10, no. 1 (November 10, 2017): 133–38. http://dx.doi.org/10.1017/s1759078717001192.

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By using a metasurface (MS) structure, a linearly polarized wave is converted to circularly polarized waves. Both right- and left-handed circular polarizations (RHCPs and LHCP) are obtained by a simple configuration in the proposed structure which consists of 16 unit cells arranged in a 4 × 4 layout. Each unit cell contains five horizontal and parallel strips embedded in a rectangular frame in which a single diagonal strip is placed from one corner to the opposed one. It is shown that the orientation of the diagonal line determines the handedness of the converted signal to be either LHCP or RHCP. In order to show the working conditions of the MS structure, scattering parameters are found for both co-polarized and cross-polarized responses. Axial ratio, an indicator for polarization conversion, is then obtained by dividing cross-polar response to co-polar response to demonstrate the transformation. The structure works for horizontally and vertically polarized linear waves in a wide band frequency range which is approximately 510 MHz. Since the suggested MS model is composed of a simple geometry for polarization conversion, it can be easily adjusted in any desired frequency bands for a variety of applications from the defence industry to medical, education, or communication areas.
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Karamzadeh, Saeid, Vahid Rafiei, and Hasan Saygin. "Development and Miniaturized of Circularly Polarization Diversity at Cavity Backed SIW Antenna for X-Band Application." Frequenz 73, no. 9-10 (September 25, 2019): 317–20. http://dx.doi.org/10.1515/freq-2018-0230.

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Abstract In this work circularly polarization diversity has been achieved by utilizing two Schottky diodes on low profile cavity-backed substrate integrated waveguide (CBSIW). In comparison with other studies in the literature, the size of antenna has been reduced to 0.54λg × 0.76λg by helping a 50-Ohm coaxial feed line. The impedance bandwidth, axial ratio bandwidth and antenna gain are improved to 10.02 %, 5.2 % and 7.68dBi, respectively. In addition, the proposed antenna can generate either a left-hand circularly polarized (LHCP) or a right-hand circularly polarized (RHCP) radiation. The developed antenna was fabricated and tested and the achieved results were in good agreement with the simulated one.
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Dissertations / Theses on the topic "Right hand circularly polarized"

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Dvořák, Petr. "Štěrbinová anténa." Master's thesis, Vysoké učení technické v Brně. Fakulta elektrotechniky a komunikačních technologií, 2014. http://www.nusl.cz/ntk/nusl-221052.

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This thesis discusses Slot antennas that are based in gap waveguide technology, which allows them to work with high frequency signals. It contains theoretical findings about antennas and waveguides, which are later used in the design. The practical section of this thesis concentrates on designing a specific gap waveguide for 10 and 24 GHz frequencies, starting with modeling and parameter optimalization. This gap waveguide is then used as a base for slot antenna design. The final antenna is designed for frequency of 10 GHz, for both linear and right-handed circular polarizations. With right-handed circular polarization, the achieved band was approximately 1.41 GHz, while the gain was 7,6 dB.
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Boyer, Laura L. "Carrier-phase wrap-up caused by rotating a global positioning system antenna and its effect on measurements." Ohio : Ohio University, 1999. http://www.ohiolink.edu/etd/view.cgi?ohiou1175890688.

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陳晉揚. "Right Hand Circularly Polarized Antenna Designs for Global Navigation Satellite System Applications." Thesis, 2019. http://ndltd.ncl.edu.tw/handle/xm88n4.

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碩士
逢甲大學
電機工程學系
107
This Thesis proposes two circularly polarized (CP) antenna designs (Antenna I and Antenna II) for GNSS applications. The overall size of proposed Antenna I is 52.8×48.4×0.063 mm3. The operating band can cover GPS L1 Band, Galileo E1 Band and Beidou B1 Band. The design of Antenna I utilize a loop antenna and have applied a perturbed element into the loop to excite two electric fields with 90 degrees phase difference, thereby exciting a good CP radiation. The simulated 10-dB impedance bandwidth of proposed Antenna I was 8.7% (1.485–1.623 GHz), and the measured one was 9.1% (1.48–1.624 GHz). The simulated and measured 3-dB axial ration (AR) bandwidths were 2.5% (1.558–1.592 GHz) and 2.2% (1.555–1.591 GHz), respectively. The Antenna I design was printed on a thin flexible substrate with thickness of only 0.063 mm by applying the Laser Direct Structuring (LDS) printing technology, so that it can exhibit the advantages such as light weight, low profile and ease in manufacturing. Therefore, it is suitable for GNSS applications that require very light weight antenna. The proposed Antenna II is also an antenna design with CP radiation, and it is for operating in the GPS L1 Band. The proposed Antenna II is a modified version of Antenna I. The antenna size is 52.5×52.5×0.76 mm3, and it is placed 10 mm above a 100×100 mm2 ground plane. Compared with proposed Antenna I, the proposed Antenna II has further introduced a pair of truncated corners at the two diagonal corners of the loop in order to improve the CP performances, as well as maintaining its CP radiation even under the interference of a large metal surface beneath it. Here, a T-matching structure is placed at the feeding point for achieving better impedance matching. The simulated 10-dB impedance bandwidth of Antenna II was 2.2% (1.557–1.593 GHz), and the measured one was 2.4% (1.553–1.591 GHz). The simulated and measured 3-dB AR bandwidths were 0.8% (1.57–1.583 GHz) and 0.9% (1.565–1.57 GHz). The simulated and measured peak realized gains at center frequency (1.575 GHz) were 7.4 dBic and 7.6 dBic, respectively. Lastly, the proposed Antenna II is suitable for GNSS application that has large metal surface/ground, such as the roof of a vehicle.
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Books on the topic "Right hand circularly polarized"

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Kimura, T., and Y. Otani. Magnetization switching due to nonlocal spin injection. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198787075.003.0021.

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This chapter discusses and presents a schematic illustration of nonlocal spin injection. In this case, the spin-polarized electrons are injected from the ferromagnet and are extracted from the left-hand side of the nonmagnet. This results in the accumulation of nonequilibrium spins in the vicinity of the F/N junctions. Since the electrochemical potential on the left-hand side is lower than that underneath the F/N junction, the electron flows by the electric field. On the right-hand side, although there is no electric field, the diffusion process from the nonequilibrium into the equilibrium state induces the motion of the electrons. Since the excess up-spin electrons exist underneath the F/N junction, the up-spin electrons diffuse into the right-hand side. On the other hand, the deficiency of the down-spin electrons induces the incoming flow of the down-spin electrons opposite to the motion of the up-spin electron.
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Mir-Hosseini, Ziba. Islam, Gender, and Democracy in Iran. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198788553.003.0010.

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Since the 1979 Revolution that brought clerics into power, the struggle for women’s rights in Iran has conventionally been framed as a polarized conflict between “Islamist” and “secularist” ideologies. This view has masked the real battle, which has been between despotism and patriarchy, on the one hand, and democracy, pluralism, and gender equality, on the other. An unintended consequence of the revolutionaries’ merger of religious and political authority has been a growing popular understanding of this struggle. This chapter examines the shifting dynamics of relations between theology, gender, and politics in the Iranian Islamic state, which, in the aftermath of the 2009 presidential election, gave birth to a rights movement with women at the forefront. By then, the traditional cultural value of namus (sexual honor) for many Iranians was outweighed by the notion of haqq (rights), especially the right to vote and to have one’s vote counted.
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Book chapters on the topic "Right hand circularly polarized"

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Cao, Tan Minh, Hong Son Vu, Thi Duyen Bui, and Minh Thuy Le. "Left Hand and Right Hand Circularly Polarized Antenna for 5G Devices." In Lecture Notes of the Institute for Computer Sciences, Social Informatics and Telecommunications Engineering, 119–27. Cham: Springer International Publishing, 2021. http://dx.doi.org/10.1007/978-3-030-77424-0_10.

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Manoj Kumar, K., and A. Bharathi. "Single-Feed Right-Hand Circularly Polarized Microstrip Antenna with Endfire Radiation." In Lecture Notes in Networks and Systems, 51–58. Singapore: Springer Singapore, 2020. http://dx.doi.org/10.1007/978-981-15-3172-9_5.

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Weik, Martin H. "right-hand polarized electromagnetic wave." In Computer Science and Communications Dictionary, 1494. Boston, MA: Springer US, 2000. http://dx.doi.org/10.1007/1-4020-0613-6_16390.

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Newnham, Robert E. "Optical activity and enantiomorphism." In Properties of Materials. Oxford University Press, 2004. http://dx.doi.org/10.1093/oso/9780198520757.003.0032.

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When plane-polarized light enters a crystal it divides into right- and lefthanded circularly polarized waves. If the crystal possesses handedness, the two waves travel with different speeds, and are soon out of phase. On leaving the crystal, the circularly polarized waves recombine to form a plane polarized wave, but with the plane of polarization rotated through an angle αt. The crystal thickness t is in mm, and α is the optical activity coefficient expressed in degrees/mm. The polarization vector of the combined wave can be visualized as a helix, turning α ◦/mm path length in the optically-active medium. Because of the low symmetry of a helix, optical activity is not observed in many high symmetry crystals. Point groups possessing a center of symmetry are inactive. In relating α to crystal chemistry it is convenient to divide optically-active materials into two categories: Those which retain optical activity in liquid form, and those which do not. It has long been known that optically-active solutions crystallize to give optically-active solids. This follows from the fact that molecules lacking mirror or inversion symmetry can never crystallize in a pattern containing such symmetry elements. Thus one way of obtaining optically-active materials is to begin with optically-active molecules, as in Rochelle salt, tartaric acid and cane sugar. Few of these crystals are very stable, however, and the optical activity coefficients are usually small, typically 2◦/mm. The same is true of many inorganic solids, though they are seldom optically active in the liquid state. For NaClO3 and MgSO4·7H2O, α is about 3◦/mm. Quartz and selenium, however, have coefficients an order of magnitude larger, showing the importance of helical structures to optical activity. Both compounds crystallize as right- and left-handed forms in space groups P312 and P322, with helices spiraling around the trigonal screw axes. Quartz contains nearly regular SiO4 tetrahedra with Si–O distances of 1.61 Å. Levorotatory quartz belongs to space group P312 and contains right-handed helices; enantiomorphic dextrorotatory quartz crystallizes in P322. Trigonal selenium also contains helical chains.
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Rodger, Alison, and Matthew A. Ismail. "Introduction to circular dichroism." In Spectrophotometry and Spectrofluorimetry. Oxford University Press, 2000. http://dx.doi.org/10.1093/oso/9780199638130.003.0008.

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Circular dichroism (CD) is the ideal technique for studying chiral molecules in solution. It is uniquely sensitive to the asymmetry of the system. These features make it particularly attractive for biological systems. CD is by definition the difference in absorption, A, of left and right circularly polarized light (CPL): . . . CD = Ae − Ar . . . . . . 1 . . . CPL has the electric field vector of the electromagnetic radiation retaining constant magnitude in time but tracing out a helix about the propagation direction. Following the optics convention we take the tip of the electric field vector of right CPL to trace out a right-handed helix in space at any instant of time (1, 2). CD spectra can in principle be measured with any frequency of electromagnetic radiation. In practice, most CD spectroscopy involves the ultraviolet-visible (UV-visible) regions of the spectrum and electronic transitions, though increasing progress is being made with measuring the CD spectra of vibrational transitions using infrared radiation. We shall limit our consideration to electronic CD spectroscopy since the practical considerations for vibrational CD differ from those for electronic CD. For randomly oriented samples, such as solutions, a net CD signal will only be observed for chiral molecules (ones that cannot be superposed on their mirror images (3)). Oriented samples of achiral molecules, such as crystals, will also give a CD spectrum unless the optical axis of the sample aligns with the propagation direction of the radiation. However, such spectra are seldom useful. CD is now a routine tool in many laboratories. The most common applications include proving that a chiral molecule has indeed been synthesized or resolved into pure enantiomers and probing the structure of biological macromolecules, in particular determining the α-helical content of proteins. Figure 3 gives an example of a CD spectrum. The key points to remember are that a CD signal is observed only at wavelengths where the sample absorbs radiation, i.e. under absorption bands, and the signal may be positive or negative depending on the handedness of the molecules in the sample and the transition being studied.
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Conference papers on the topic "Right hand circularly polarized"

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Singh, Abhishek, Olivier Pajona, Sebastian Rowson, Jeff Shamblin, Mehak Garg, and Jaakko Kyllonen. "Miniaturized right hand circularly polarized antenna for GPS applications." In 2015 IEEE 4th Asia-Pacific Conference on Antennas and Propagation (APCAP). IEEE, 2015. http://dx.doi.org/10.1109/apcap.2015.7374380.

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Kawakami, H., T. Haga, M. Ishikawa, and M. Nagatsuka. "Characteristics of 5-element right-hand circularly polarized ring loop antenna." In 2006 IEEE Antennas and Propagation Society International Symposium. IEEE, 2006. http://dx.doi.org/10.1109/aps.2006.1710648.

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Nakagawa, Yukata, Takeshi Higashino, and Minoru Okada. "Multiple Regression For Rainfall Estimation Using Right/Left-hand Circularly Polarized Signals." In 2020 IEEE 9th Global Conference on Consumer Electronics (GCCE). IEEE, 2020. http://dx.doi.org/10.1109/gcce50665.2020.9291977.

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Farahani, Mohammadmahdi, Mansoor Dashti Ardakani, Mohammad Akbari, Tayeb A. Denidni, and Abdel-Razik Sebak. "Hedgehog Waveguide Phase Adjustment of Dual Left/Right-Hand Circularly-Polarized Antenna." In 2020 IEEE International Symposium on Antennas and Propagation and North American Radio Science Meeting. IEEE, 2020. http://dx.doi.org/10.1109/ieeeconf35879.2020.9330482.

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Umeda, Norihiro, Sho Wakayama, Shinsuki Arakawa, Atsuo Takayanagi, and Hiroyuki Kohwa. "Fast birefringence measurement using right and left hand circulary polarized laser." In International Symposium on Polarization Analysis and Applications to Device Technology, edited by Toru Yoshizawa and Hideshi Yokota. SPIE, 1996. http://dx.doi.org/10.1117/12.246195.

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Denton, Suzanna, and Paul Zavidniak. "Analysis of a right-hand circular polarized conventional antenna system for high altitude airborne cellular base stations." In SAS2008 - IEEE Sensors Applications Symposium. IEEE, 2008. http://dx.doi.org/10.1109/sas13374.2008.4472967.

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Jahagirdar, D. R., and K. Sambasiva Rao. "Novel wideband high gain Right Hand Circular Polarized (RHCP) 2×4 Array Antenna at L-Band for data link applications." In 2016 Asia-Pacific Microwave Conference (APMC). IEEE, 2016. http://dx.doi.org/10.1109/apmc.2016.7931466.

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Hashemi, Mohammed Reza M., and Tatsuo Itoh. "Circularly polarized composite right/left-handed leaky-wave antenna." In 2010 IEEE International Conference on Wireless Information Technology and Systems (ICWITS). IEEE, 2010. http://dx.doi.org/10.1109/icwits.2010.5612258.

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Khorasaninejad, Mohammadreza, and Kenneth B. Crozier. "Separating Left- from Right-Circularly Polarized Light with a Dielectric Metamaterial." In CLEO: Science and Innovations. Washington, D.C.: OSA, 2014. http://dx.doi.org/10.1364/cleo_si.2014.sf1o.2.

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Ding, Dawei, Dawei Li, Zhuang Li, and Lixia Yang. "Compact Circularly-Polarized Microstrip Antenna for Hand-Held RFID Reader." In 2019 8th Asia-Pacific Conference on Antennas and Propagation (APCAP). IEEE, 2019. http://dx.doi.org/10.1109/apcap47827.2019.9472059.

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Reports on the topic "Right hand circularly polarized"

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Venkataraman, C. T., J. C. Lang, C. S. Nelson, G. Srajer, D. R. Haeffner, and S. D. Shastri. A high energy phase retarder for the simultaneous production of right- and left-handed circularly polarized x-rays. Office of Scientific and Technical Information (OSTI), September 1997. http://dx.doi.org/10.2172/642741.

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