Self-focusing and self-defocusing by cascaded second-order effects in KTP

We monitor the induced phase change produced by a cascaded chi((2)):chi((2)) process in KTP near the phase-matching angle on a picosecond 1.06-microm-wavelength beam using the Z-scan technique. This nonlinear refraction is observed to change sign as the crystal is rotated through the phase-match ang...

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Veröffentlicht in:Optics letters 1992, Vol.17 (1), p.28-30
Hauptverfasser: DESALVO, R, HAGAN, D. J, SHEIK-BAHAE, M, STEGEMAN, G, VAN STRYLAND, E. W, VANHERZEELE, H
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container_end_page 30
container_issue 1
container_start_page 28
container_title Optics letters
container_volume 17
creator DESALVO, R
HAGAN, D. J
SHEIK-BAHAE, M
STEGEMAN, G
VAN STRYLAND, E. W
VANHERZEELE, H
description We monitor the induced phase change produced by a cascaded chi((2)):chi((2)) process in KTP near the phase-matching angle on a picosecond 1.06-microm-wavelength beam using the Z-scan technique. This nonlinear refraction is observed to change sign as the crystal is rotated through the phase-match angle in accordance with theory. This theory predicts the maximum small-signal effective nonlinear refractive index of n(eff)(2) congruent with +/-2 x 10(-14) cm(2)/W (+/-1 x 10(-11) esu) for an angle detuning of +/-5 degrees from phase match for this 1-mm-thick crystal with a measured d(eff) of 3.1 pm/V. For a fixed phase mismatch, this n(eff)(2) scales linearly with length and as d(eff)(2) however, for the maximum n(eff)(2) the nonlinear phase distortion becomes sublinear with irradiance for phase shifts near pi/4.
doi_str_mv 10.1364/ol.17.000028
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Fundamental areas of phenomenology (including applications)
Nonlinear optics
Optics
Physics
title Self-focusing and self-defocusing by cascaded second-order effects in KTP
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