2009 Conference on Lasers &Amp; Electro Optics &Amp; The Pacific Rim Conference on Lasers and Electro-Optics 2009
DOI: 10.1109/cleopr.2009.5292578
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Generating vortex laser beams by converting ince-gaussian laser beams with an astigmatic mode converter

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Cited by 3 publications
(3 citation statements)
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“…Since the repetition rate of pulse trains is 1 MHz, the maximum pulse energy is calculated to be 20.36 μJ and 20.12 μJ. In addition, the maximum peak power is calculated to be 46.3 MW (radial vector beam) and 46.8 MW (azimuthal vector beam), which are two orders of magnitude higher than in previously reported research [11] . As shown in Fig.…”
Section: Resultsmentioning
confidence: 61%
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“…Since the repetition rate of pulse trains is 1 MHz, the maximum pulse energy is calculated to be 20.36 μJ and 20.12 μJ. In addition, the maximum peak power is calculated to be 46.3 MW (radial vector beam) and 46.8 MW (azimuthal vector beam), which are two orders of magnitude higher than in previously reported research [11] . As shown in Fig.…”
Section: Resultsmentioning
confidence: 61%
“…Cylindrical vector beams (CVBs) have attracted enormous scientific attention due to their unique optical properties, such as axially symmetric field amplitude distributions and radial or azimuthal polarization states, which enable imaging resolution below the diffraction limit and interact without the undesirable anisotropy produced by a linearly-polarized light [1][2][3][4][5] . A variety of applications utilizing CVBs have been explored such as high resolution imaging, nanoparticle manipulation, terahertz technology, data storage, and optical communication [6][7][8][9][10][11] . Generally, several typical optical devices, such as astigmatic mode converters (AMCs), liquid-crystal spatial light modulators (SLMs), and forked gratings, have been used as mode converters to transfer spatially homogeneous polarizations (e.g., linear or circular polarization) into spatially inhomogeneous cylindrical vector polarizations [12][13][14][15][16] .…”
Section: Introductionmentioning
confidence: 99%
“…These extra-cavity PILB transformation techniques are based on coherent beam superposition within interferometric instruments [15,16] and beam shaping schemes employing anamorphic optical systems (AOSs) [17,18]. These techniques have been applied to transform Hermite-Gaussian [19,20], Laguerre-Gaussian [18], and Ince-Gaussian [16,21] laser modes. Beam transformations employing anamorphic optical systems are insensitive to vibrations, and are easier to implement when compared to interferometric techniques.…”
Section: Introductionmentioning
confidence: 99%