Modelling Of Broadband Electric Field Propagation In Nonlinear Dielectric Media

We derive unidirectional pulse propagation equations to describe extreme high-intensity and ultra-broadband optical interactions in uniaxial crystals, showing both secondand third-order nonlinear optical susceptivities. Two nonlinearly coupled first order (in the propagation coordinate) equations describe the dynamics and interactions of the ordinary and extraordinary field polarizations, and are valid for arbitrarily wide pulse bandwidth. We exploit this model to predict harmonic and supercontinuum generation in BBO crystals under strong and competing influence of quadratic and cubic susceptivities.

[1]  J. Dudley,et al.  Supercontinuum generation in photonic crystal fiber , 2006 .

[2]  Costantino De Angelis,et al.  Modeling of ultrabroadband and single-cycle phenomena in anisotropic quadratic crystals , 2011 .

[3]  Fredrik Laurell,et al.  Multistep quadratic cascading in broadband optical parametric generation. , 2012, Optics letters.

[4]  Ajit Kumar Ultrashort pulse propagation in a cubic medium including the Raman effect , 2010 .

[5]  F. Wise,et al.  Optical Cherenkov radiation by cascaded nonlinear interaction: an efficient source of few-cycle energetic near- to mid-IR pulses. , 2011, Optics express.

[6]  J Warner,et al.  The effects of phase matching method and of crystal symmetry on the polar dependence of third-order non-linear optical polarization , 1965 .

[7]  K Yamakawa,et al.  0.85-PW, 33-fs Ti:sapphire laser. , 2003, Optics letters.

[8]  F. Krausz Attosecond Physics , 2007, 2007 Conference on Lasers and Electro-Optics - Pacific Rim.

[9]  Carsten Langrock,et al.  Supercontinuum generation in quasi-phase-matched LiNbO3 waveguide pumped by a Tm-doped fiber laser system. , 2011, Optics letters.

[10]  F Baronio,et al.  Ultrabroadband Optical Phenomena in Quadratic Nonlinear Media , 2010, IEEE Photonics Journal.

[11]  Tae Jun Yu,et al.  0.1 Hz 1.0 PW Ti:sapphire laser. , 2010, Optics letters.

[12]  Costantino De Angelis,et al.  Nonlinear envelope equation for broadband optical pulses in quadratic media , 2010, 1001.1874.

[13]  F. Krausz,et al.  Intense few-cycle laser fields: Frontiers of nonlinear optics , 2000 .

[14]  J Warner,et al.  The effects of phase matching method and of uniaxial crystal symmetry on the polar distribution of second-order non-linear optical polarization , 1965 .

[15]  A. Husakou,et al.  Supercontinuum generation of higher-order solitons by fission in photonic crystal fibers. , 2001, Physical review letters.

[16]  F. Wise,et al.  Ultrafast and octave-spanning optical nonlinearities from strongly phase-mismatched quadratic interactions. , 2011, Physical review letters.

[17]  F. Wise,et al.  Limits to compression with cascaded quadratic soliton compressors. , 2008, Optics express.

[18]  G.H.C. New,et al.  Theory of directional pulse propagation , 2005 .

[19]  Carsten Langrock,et al.  Supercontinuum generation in quasi-phasematched waveguides. , 2011, Optics express.

[20]  Binbin Zhou,et al.  Optical Cherenkov radiation in ultrafast cascaded second-harmonic generation , 2010 .

[21]  Fabio Baronio,et al.  Three-wave Trapponic solitons for tunable high-repetition rate pulse train generation , 2008 .

[22]  G Genty,et al.  Nonlinear envelope equation modeling of sub-cycle dynamics and harmonic generation in nonlinear waveguides. , 2007, Optics express.

[23]  Vladimir Lozhkarev,et al.  High-efficiency second-harmonic generation of superintense ultrashort laser pulses. , 2009, Applied optics.

[24]  J V Moloney,et al.  Unidirectional optical pulse propagation equation. , 2002, Physical review letters.

[25]  D. Nikogosyan,et al.  Nonlinear Optical Crystals: A Complete Survey , 2005 .

[26]  Binbin Zhou,et al.  The anisotropic Kerr nonlinear refractive index of the beta-barium borate (β -BaB 2 O 4 ) nonlinear crystal , 2012, 1209.3158.

[27]  Lu Chai,et al.  Multiwatt octave-spanning supercontinuum generation in multicore photonic-crystal fiber. , 2012, Optics letters.

[28]  Paul Kinsler Optical pulse propagation with minimal approximations , 2010 .

[29]  H. H. Chen,et al.  Soliton at the zero-group-dispersion wavelength of a single-model fiber. , 1987, Optics letters.

[30]  P. Petropoulos,et al.  Mid-IR Supercontinuum Generation From Nonsilica Microstructured Optical Fibers , 2007, IEEE Journal of Selected Topics in Quantum Electronics.

[31]  M. Kolesik,et al.  Theory and Simulation of Ultrafast Intense Pulse Propagation in Extended Media , 2012, IEEE Journal of Selected Topics in Quantum Electronics.

[32]  Fabio Baronio,et al.  Parametric frequency conversion of short optical pulses controlled by a CW background. , 2007, Optics express.

[33]  Costantino De Angelis,et al.  From femtosecond infrared to picosecond visible pulses: temporal shaping with high-efficiency conversion. , 2007, Optics letters.

[34]  Michael D. Perry,et al.  High-intensity third-harmonic generation , 2002 .

[35]  J V Moloney,et al.  Nonlinear optical pulse propagation simulation: from Maxwell's to unidirectional equations. , 2004, Physical review. E, Statistical, nonlinear, and soft matter physics.

[36]  Vincent Couderc,et al.  Velocity-locked solitary waves in quadratic media. , 2010, Physical review letters.

[37]  E. M. Lifshitz,et al.  Electrodynamics of continuous media , 1961 .

[38]  C Farrell,et al.  Octave-spanning super-continuum from a silica photonic crystal fiber pumped by a 386 MHz Yb:fiber laser. , 2012, Optics letters.

[39]  Vladislav Ginzburg,et al.  Compact 0.56 Petawatt laser system based on optical parametric chirped pulse amplification in KD*P crystals , 2007 .