2011
DOI: 10.1364/oe.19.005297
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Nonlinear generation of a neat semi-Gaussian laser beam with a transversely varying periodically-poled LiTaO_3 crystal

Abstract: We experimentally demonstrate a compact, all-solid-state 532 nm semi-Gaussian laser beam (SGB) source based on a 1064 nm laser and a transversely varying periodically-poled LiTaO3 (TPPLT) crystal as the laser beam shaper as well as the nonlinear frequency converter. We have used the designed TPPLT crystal to obtain a neat 532nm SGB with the quality of QSGB=1:17.5 by a single-pass second harmonic generation. The dependence of the generated SGB quality on the designed TPPLT parameter and the potential applicatio… Show more

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Cited by 8 publications
(7 citation statements)
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References 24 publications
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“…The SGB has a waist radius of đ‘€ SGB = 20 ”m and a sharp border width of đ‘€ đ” = 1.2 ”m. [13,14] The intensity profile of the SGB in the 𝑧 direction is a semi-Gaussian one. The deceleration principle will be introduced in detail in the following.…”
Section: (B) a Well-collimatedmentioning
confidence: 99%
“…The SGB has a waist radius of đ‘€ SGB = 20 ”m and a sharp border width of đ‘€ đ” = 1.2 ”m. [13,14] The intensity profile of the SGB in the 𝑧 direction is a semi-Gaussian one. The deceleration principle will be introduced in detail in the following.…”
Section: (B) a Well-collimatedmentioning
confidence: 99%
“…Nonlinear photonic crystals, also known as quasi-phase matching (QPM) media, feature a spatial modulation of the second-order nonlinearity of the host materials. [1][2][3][4][5][6][7][8][9] This modulation provides synchronization of phase velocities of optical waves at different DOI: 10.1002/lpor.202000224 frequencies, such that they can efficiently exchange energy. Meanwhile, the spacedependent nonlinearity allows controlling over the wavefront of the nonlinear interacting waves, which has inspired wide applications in novel light sources, nonlinear data processing, etc.…”
Section: Introductionmentioning
confidence: 99%
“…Taking the second harmonic generation (SHG) as an example, the nonlinearity modulation maps the interference between the nonlinear polarization wave (with a doubling of the wave vector of the fundamental beam) and the second harmonic (SH) of required shape, e.g., Bessel, vortex, Airy beam etc. [ 17,19,21 ] The holographic χ (2) nonlinearity patterning has been commonly achieved by either ferroelectric domain inversion (electrical poling), [ 8–10 ] or laser‐induced partial amorphization of the crystal. [ 24,25 ] However, while the original pattern is a continuous in space, the corresponding nonlinearity distribution is of binary character, as in binary computer generated holograms.…”
Section: Introductionmentioning
confidence: 99%
“…Depending on the geometry of interaction, the QPM can be implemented through the schemes of nonlinear Bragg diffraction 15 , Čerenkov-type 16 emission and nonlinear Raman-Nath diffractions 17 . In these NPCs the wavefront shaping often relies on transversely patterned nonlinearity, i.e., χ (2) varies spatially (typically between +| χ (2) | and −| χ (2) |) in a plane perpendicular to the propagation direction of the incident beam 18–20 . In this respect, the transverse χ (2) modulation plays a role analogous to that of spatial variation of refractive index in linear optical media.…”
Section: Introductionmentioning
confidence: 99%