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1.
J Phys Condens Matter ; 29(8): 084004, 2017 Mar 01.
Article in English | MEDLINE | ID: mdl-28092628

ABSTRACT

We introduce a generalization of the adiabatic frequency conversion method for an efficient conversion of ultrashort pulses in the full nonlinear regime. Our analysis takes into account dispersion as well as two-photon processes and Kerr effect, allowing complete analysis of any three waves with arbitrary phase mismatched design and any nonlinear optical process. We use this analysis to design an efficient and robust second harmonic generation, the most widely used nonlinear process for both fundamental and applied research. We experimentally show that such design not only allows for very efficient conversion of various of ultrashort pulses, but is also very robust to variations in the parameters of both the nonlinear crystal and the incoming light. These include variation of more than 100 °C in the crystal temperature, a wide bandwidth of up to 75 nm and a chirp variation of 300 fs to 3.5 ps of the incoming pulse. Also, we show the dependency of the adiabatic second harmonic generation design on the pump intensity and the crystal length. Our study shows that two photon absorption plays a critical role in such high influence nonlinear dynamics, and that it must be considered in order to achieve agreement with experimental results.

2.
Opt Lett ; 31(9): 1292-4, 2006 May 01.
Article in English | MEDLINE | ID: mdl-16642089

ABSTRACT

The signal and idler beams from a picosecond, synchronously pumped optical parametric oscillator (OPO) provide the two colors necessary for coherent anti-Stokes Raman scattering (CARS) microscopy. The OPO provides a continuously tunable frequency difference between the two beams over a broad range of Raman shifts (100-3700 cm(-1)) by varying the temperature of a single nonlinear crystal. The near-infrared output (900-1300 nm) allows for deep penetration into thick samples and reduced nonlinear photodamage. Applications of this light source to in vivo cell and ex vivo tissue imaging are demonstrated.


Subject(s)
Image Enhancement/instrumentation , Lasers , Lighting/instrumentation , Spectrum Analysis, Raman/instrumentation , Tomography, Optical Coherence/instrumentation , Animals , Ear, External/cytology , Equipment Design , Equipment Failure Analysis , Image Enhancement/methods , Mice , Scattering, Radiation , Spectrum Analysis, Raman/methods , Tomography, Optical Coherence/methods
3.
Opt Express ; 12(22): 5562-76, 2004 Nov 01.
Article in English | MEDLINE | ID: mdl-19484119

ABSTRACT

The details of two soliton collision processes were investigated in detail in a 1 cm long periodically poled KTP crystal for the case when the solitons were excited by inputting only the fundamental beam. The effects on the collision outcomes of the distance of the collision into the sample, collision angle and phase mismatch were measured for different relative phases between the input beams. At small angles (around 0.4 degrees ) fusion, repulsion and energy transfer processes were observed, while at the collision angles approaching 3.2 degrees the two output soliton beams were essentially unaffected by the interaction. The phase mismatch was varied from 3.5 to -1.5pi for the 0.4 degrees collision angle case. The output solitons separation at pi input phase difference showed strongly asymmetric behavior with phase mismatch. In general, the measurements indicate a decrease in the interaction strength with increasing phase mismatch. All collision processes were performed in the vicinity of a non-critical phase matching.

4.
Opt Lett ; 28(21): 2103-5, 2003 Nov 01.
Article in English | MEDLINE | ID: mdl-14587829

ABSTRACT

The reflection of bulk quadratic solutions incident onto a quadratically nonlinear interface in periodically poled potassium titanyl phosphate was observed. The interface consisted of the boundary between two quasi-phase-matched regions displaced from each other by a half-period. At high intensities and small angles of incidence the soliton is reflected.

5.
Opt Lett ; 28(16): 1451-3, 2003 Aug 15.
Article in English | MEDLINE | ID: mdl-12943088

ABSTRACT

Theoretical predictions and experimental observations show that a weak harmonic seed beam can control the process of generating multiple quadratic solitons in periodically poled KTiOPO4 by inputting only a fundamental beam. This all-optical switching does not depend on the relative phase of the input beams, an unusual property for such coherent solitons.

6.
Phys Rev E Stat Nonlin Soft Matter Phys ; 67(4 Pt 2): 046616, 2003 Apr.
Article in English | MEDLINE | ID: mdl-12786518

ABSTRACT

We report the experimental observation of the formation of multiple optical quadratic solitons in a process mediated by the amplification of minute asymmetries in the diffraction properties of the input light. Experiments were conducted in phase-matched second-harmonic generation in a bulk crystal of periodically poled potassium titanyl phosphate pumped at 1064 nm. The different mechanisms that influence the process were investigated numerically, and the pulsed nature of the pump light was found to play a key role in the observed light distributions.

7.
Opt Lett ; 28(8): 640-2, 2003 Apr 15.
Article in English | MEDLINE | ID: mdl-12703926

ABSTRACT

The evolution of fundamental beams into quadratic spatial solitons was investigated in a periodically poled bulk KTiOPO4 crystal near and at phase matching. Various soliton properties, such as trapping efficiency as a function of phase mismatch, poling-induced walk-off, and the effects of pulse width, beam width, and input beam quality, were measured. Effects attributed to the presence of cubic nonlinearities were also observed.

8.
Opt Express ; 11(11): 1328-37, 2003 Jun 02.
Article in English | MEDLINE | ID: mdl-19466001

ABSTRACT

The properties of the multi-quadratic-soliton generation process have been investigated both theoretically and experimentally near and on phase-match in non-critically-phase-matched, periodically poled, potassium titanyl phosphate (PPKTP). It was found that multi-soliton generation occurs primarily due to asymmetry in the input beam and at phase-matching. The number of solitons generated depended on the input intensity in a non-trivial way.

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