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1975
DOI: 10.1007/bf00631587
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Rotation of laser beam polarization in acousto-optic devices

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Cited by 30 publications
(10 citation statements)
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“…The basic parameters for the changes are electrooptical coefficients [3,4], acoustooptical parameters [5], magnetooptical susceptibilities [6]. The use of the piezooptical operation was just done for some of the materials like nanofilms [7], glasses [8], nanocrystals [9] etc.…”
Section: Introductionmentioning
confidence: 99%
“…The basic parameters for the changes are electrooptical coefficients [3,4], acoustooptical parameters [5], magnetooptical susceptibilities [6]. The use of the piezooptical operation was just done for some of the materials like nanofilms [7], glasses [8], nanocrystals [9] etc.…”
Section: Introductionmentioning
confidence: 99%
“…44,45 Furthermore, manual and acoustooptical polarization-swept fs light sources can help determine the detailed content within the subsurface of tissues. 46,47 Polarization signature of tissues, such as skin and cartilage, has added an additional contrast mechanism to intensity-based investigation and has allowed differentiation of normal and morphologically variant tissues. 9,28,48 For instance, variations of collagen fiber organization and orientation in normal cartilage were revealed and differentiated from degenerated cartilage using polarization-sensitive SHG and ratio of intensities of two orthogonally polarization-resolved SHG signals.…”
Section: Basis Of Shg Origin In Biological Mediamentioning
confidence: 99%
“…Although tremendous progress in the exploration of enhancing the local electric field enhancement and improving the absorption, achieving strong local electric field enhancements (| E loc |/| E 0 | > 100) and near-perfect absorption (> 99%) simultaneously still remains a challenge, which will benefit a wide range of applications including plasmonic sensors, photocatalytic water splitting, SERS, and SEIRA. On the other hand, except for the polarization switching reported by Yang et al [ 1 ], most traditional polarization-selective devices, such as waveplates and polarizers based on electro-optical effects, are either static or operating with only gigahertz switching speeds, which are limited by the required electronics [ 45 , 46 ]. Thus, for the phenomena or applications of EIT effect, Fano resonance, and plasmonic nanoantennas based on a plasmonic metasurface, most of previously reported works usually suffer from these serious and urgent problems: (i) the broadening of plasmonic resonances owing to large optical losses in metals [ 5 ]; (ii) unadjustable operating wavelength of EIT effect or Fano resonances [ 35 ]; (iii) the challenge of achieving strong local electric field enhancements (| E loc |/| E 0 | > 100) and near-perfect absorption (> 99%) simultaneously [ 8 ]; (iv) generally, only gigahertz switching speeds of polarization-selective devices operating in visible or NIR region [ 1 ].…”
Section: Introductionmentioning
confidence: 99%