Supercontinuum Generation in Photonic Crystal Fibers John M. Dudley Laboratoire d’Optique P-M Duffieux, Institut FEMTO-ST CNRS UMR 6174 Université de Franche-Comté BESANÇON, France. POWAG 2004 Bath July 12-16 With thanks to … Université Libre de Bruxelles & University of Auckland Stéphane Coen Université de Franche-Comté Laurent Provino, Hervé Maillotte, Pierre Lacourt, Bertrand Kibler, Cyril Billet Université de Bourgogne Guy Millot Georgia Institute of Technology Rick Trebino, Xun Gu, Qiang Cao National Institute of Standards & Technology Kristan Corwin, Nate Newbury, Brian Washburn, Scott Diddams + Ole Bang (COM), Ben Eggleton (OFS & Sydney), Alex Gaeta (Cornell), John Harvey (Auckland), Rüdiger Paschotta (ETH Zurich), Stephen Ralph (Georgia Tech), Philip Russell (Bath), Bob Windeler (OFS) + ACI photonique What exactly are we trying to understand? Ranka et al. Optics Letters 25, 25 2000 Femtosecond Ti:sapphire laser Anomalous GVD pumping grating PCF • Output spectrum What exactly are we trying to understand? Birks et al. Optics Letters 25, 1415 2000 Femtosecond Ti:sapphire laser Anomalous GVD pumping grating TAPER • Output spectrum What exactly are we trying to understand? Ranka et al. Optics Letters 25, 25 2000 Femtosecond Ti:sapphire laser Anomalous GVD pumping PCF • Broadening mechanisms • • • • Spectral structure Evolution of spectrum along the fiber • Output spectrum Stability Flatness …etc… Understand, control, exploit… grating Objectives ● Develop a detailed understanding of ultrashort pulse propagation and supercontinuum (SC) generation in solid-core PCF Concentrate on femtosecond pulse pumping regime – soliton generation dynamics – noise and stability issues ● Appreciate the utility of time-frequency spectrograms for interpreting nonlinear fiber pulse propagation ● Briefly (if time) address mechanisms using longer pulses Introduction (I) ● It has been known since 1970 that ultrashort light pulses injected in a nonlinear medium yield extreme spectral broadening or supercontinuum (SC) generation. ● Multiple physical processes involved – Self- & cross-phase modulation – – Multi-wave mixing Raman scattering …etc… Introduction (II) ● Many previous studies of spectral broadening carried out with conventional fibers since 1971. ● Higher nonlinearity and novel dispersion of PCF has meant that much old physics has been poorly recognised as such. ● There are, however, new features associated with SC generation in PCF based on pumping close to near-IR zero dispersion points. Wavelength (nm) 300 1300 Dn = 770 THz Dn/n0 ~ 2 2000 Dn = 81 THz Dn/n0 ~ 0.5 Pulse propagation in single mode fibers Analysis of single-mode fiber propagation equations yield: scalar approach transverse profile field envelope propagation constant Frequency dependence of b – chromatic dispersion (group velocity)-1 group velocity dispersion (GVD) [ps2/km] [ps / nm·km] Propagation equation (I) Nonlinear Envelope Equation (NEE) co-moving frame dispersion co-moving frame Kerr nonlinearity Raman response self-steepening SPM, FWM, Raman Propagation equation (II) Nonlinear Envelope Equation (NEE) co-moving frame dispersion self-steepening SPM, FWM, Raman Validity to the few-cycle regime has been established Blow & Wood Brabec & Krausz Ranka & Gaeta Karasawa et al. IEEE JQE 25 2665 (1989) Phys. Rev. Lett. 78 3283 (1997) Opt. Lett. 23 534 (1998) IEEE JQE 37 398 (2001) Application to PCF pulse propagation Gaeta Dudley & Coen Opt. Lett. 27 924 (2002) Opt. Lett. 27 1180 (2002) Simulations of SC generation in PCF • We first consider propagation in highly nonlinear PCF with a high air-fill fraction, and a small central “core” diameter 2.5 mm • Treat anomalous dispersion regime pumping l > 780 nm Simulations of SC generation in PCF • We first consider propagation in highly nonlinear PCF with a high air-fill fraction, and a small central “core” diameter 2.5 mm By the way… FREE SOFTWARE for PCF dispersion calculation (multipole method) now available from University of Sydney cudosMOF • Treat anomalous dispersion regime pumping l > 780 nm So…what does a simulation look like? Evolution with propagation distance Complex spectral and temporal evolution in 15 cm of PCF Pulse parameters: 30 fs FWHM, 10 kW peak power, l = 800 nm Temporal evolution Distance (m) Distance (m) Spectral evolution Wavelength (nm) Time (ps) Understanding the details… Solitons Perturbed solitons Raman self-frequency shift Dispersive waves Simplify things : Nonlinear Schrödinger Equation Nonlinear Schrödinger Equation (NLSE): co-moving frame Kerr nonlinearity instantaneous power (W) The NLSE has a number of analytic solutions and scaling rules. Higher-order effects can (sometimes) be treated as perturbations, making the physics clear. Nonlinear Schrödinger Equation Nonlinear Schrödinger Equation (NLSE) co-moving frame Kerr nonlinearity instantaneous power (W) Consider propagation in highly nonlinear PCF: ZDW at 780 nm l = 850 nm b2 = -13 ps2 km-1 g = 100 W-1km-1 T0 = 28 fs (FWHM 50 fs) Fundamental solitons Initial condition = 165 W N=1 Invariant evolution soliton wavenumber Higher-order solitons Initial condition N=3 Periodic evolution = 10 cm Higher-order solitons Initial condition Periodic evolution = 10 cm Soliton decay – soliton fission In the presence of perturbations, a higher order N-soliton is unstable, and will break up into N constituent fundamental 1-solitons …quite a bit of work yields… Soliton decay – soliton fission In the presence of perturbations, a higher order N-soliton is unstable, and will break up into N constituent fundamental 1-solitons Initial condition Raman Higher-order dispersion NLSE + PERTURBATION Selfsteepening Soliton decay – soliton fission In the presence of perturbations, a higher order N-soliton is unstable, and will break up into N constituent fundamental 1-solitons Soliton decay – soliton fission In the presence of perturbations, a higher order N-soliton is unstable, and will break up into N constituent fundamental 1-solitons Physics of the self-frequency shift Dt’ Dt Dl’ Dl FT NN==11 -13 -13 THz THz l t sees seesgain gain 25 fs FWHM 14 THz bandwidth pump pump Soliton decay – soliton fission Illustration : Raman perturbation only ZDW Distance (z/zsol) Distance (z/zsol) Pulse parameters: N = 3, FWHM = 50 fs, P0 = 14.85 kW, zsol = 10 cm Time (ps) Wavelength (nm) Soliton decay – soliton fission Illustration : Raman perturbation only Distance (z/zsol) Pulse parameters: N = 3, FWHM = 50 fs, P0 = 14.85 kW, zsol = 10 cm Time (ps) The spectrogram ● The spectrogram shows a pulse in both domains simultaneously gate pulse pulse variable delay gate Soliton fission in the time-frequency domain ZDW projected axis spectrogram Dispersive wave radiation A propagating 1-soliton in the presence of higher-order dispersion can shed energy in the form of a low amplitude dispersive wave. Phasematching between the propagating soliton and a linear wave. DW b3 > 0 DW > 0 BLUE SHIFT l Wai et al. Opt. Lett. 11 464 (1986) Akhmediev & Karlsson Phys. Rev. A 51 2602 (1995) Dispersive wave radiation A propagating 1-soliton in the presence of higher-order dispersion can shed energy in the form of a low amplitude dispersive wave. Distance (m) Distance (m) Pulse parameters: N = 1 soliton at 850 nm, b3 > 0, no Raman Wavelength (nm) Time (ps) Does that remind you of anything? SC generation – anomalous dispersion pump Signatures of soliton fission and dispersive wave generation in SC generation are now apparent… Temporal evolution Distance (m) Distance (m) Spectral evolution Wavelength (nm) Time (ps) SC generation – anomalous dispersion pump Signatures of soliton fission and dispersive wave generation in SC generation are now apparent… Temporal evolution Distance (m) Distance (m) Spectral evolution Wavelength (nm) Time (ps) SC generation – anomalous dispersion pump DW 115 THz S3 S2 ZDW fine structure S1 Intuitive correlation of time and frequency domains What about the experiments ? Spectrum (20 dB / div.) Experimental Measurements – spectra Experiment Simulation Wavelength (nm) Experimental Measurements – Raman solitons Good comparison between simulations and experiments Simulation Washburn et al. Electron. Lett. 37 1510 (2001) Experiment Experimental Measurements – XFROG XFROG measures the spectrally resolved cross-correlation between a reference field ERef(t) (fs pump pulse at 800 nm) and the field to be characterized E(t) (the SC from 500-1200 nm). The cross-correlation is measured using sum-frequency generation (SFG) by mixing the reference pump pulse with the SC. Experimental Measurements – XFROG Interpretation of experimental XFROG data is facilitated by the numerical results above. Distinct anomalous dispersion regime Raman solitons Low amplitude ultrafast oscillations Gu et al. Dudley et al. Opt. Lett. 27 1174 (2002) Opt. Exp. 10 1251 (2002) Experimental Measurements – XFROG Interpretation of experimental XFROG data is facilitated by the numerical results above. Distinct anomalous dispersion regime Raman solitons Low amplitude ultrafast oscillations Gu et al. Dudley et al. Opt. Lett. 27 1174 (2002) Opt. Exp. 10 1251 (2002) SC generation – normal dispersion pump Four wave mixing ws wp wi w Dudley et al. JOSA B 19, 765-771 (2002) SC generation – anomalous vs normal dispersion pumps Each case would yield visually similar supercontinua but they are clearly very different the difference is in the dynamics ZDW ZDW Propagation with negative dispersion slope For a PCF with a second zero dispersion point, the negative dispersion slope completely changes the propagation dynamics reduced core diameter ~ 1.2 mm Modeled GVD old regime b3 > 0 Harbold et al. Opt. Lett. 27, 1558 (2002) Skyrabin et al. Science 301 1705 (2003) Hillisgøe et al. Opt. Exp. 12, 1045 (2004) Efimov et al. CLEO Paper IML7 (2004) new regime b3 < 0 Propagation with negative dispersion slope For a PCF with a second zero dispersion point, the negative dispersion slope completely changes the propagation dynamics reduced core diameter ~ 1.2 mm Modeled GVD old regime b3 > 0 Harbold et al. Opt. Lett. 27, 1558 (2002) Skyrabin et al. Science 301 1705 (2003) Hillisgøe et al. Opt. Exp. 12, 1045 (2004) Efimov et al. CLEO Paper IML7 (2004) new regime b3 < 0 Suppressing the Raman self-frequency shift Suppressing the Raman self-frequency shift Initial Raman shifting is arrested by dispersive wave generation ZDW Distance (m) Distance (m) Pulse parameters: 50 fs FWHM, 2 kW peak power, l = 1200 nm, N ~ 1.7 Wavelength (nm) Time (ps) Suppressing the Raman self-frequency shift A detailed treatment shows that dispersive wave generation is associated with spectral recoil of the generating soliton. Recoil RED SHIFT ZDW b3 > 0 BLUE SHIFT DW l In the “conventional regime” the Raman shift and spectral recoil are in the same direction and reinforce. Suppressing the Raman self-frequency shift A detailed treatment shows that dispersive wave generation is associated with spectral recoil of the generating soliton. DW b3 < 0 RED SHIFT ZDW Recoil BLUE SHIFT l Around the second ZDW, the Raman shift and spectral recoil are in opposite directions and can thus compensate. Suppressing the Raman self-frequency shift Biancalana et al. Theory of the self frequency shift compensation by the resonant radiation in photonic crystal fibers To appear in Phys Rev E August 2004. SC generation with nanosecond pulses 1 ns input pulses from mchip laser at 1064 nm, 4 m of PCF P = 26 W P = 43 W P = 98 W P = 72 W SC generation with nanosecond pulses Simulations reproduce experiments over a 50 dB dynamic range P = 43 W P = 26 W P = 98 W exp exp exp sim sim sim Supercontinuum stability As early as 2001, experiments reported that supercontinuum generation in PCF could be very unstable. Hollberg et al. IEEE J. Quant. Electron. 37 1502 (2001) Nonlinear spectral broadening processes are very sensitive to technical or quantum noise sources. Nakazawa et al. Phys. Rev. A 39 5768 (1989) The NEE model, extended to include quantum noise sources, can be used to clarify physical origin of instabilities and determine useful parameter regimes for quiet continuum generation. Drummond & Corney J. Opt. Soc. Am. B 18, 139 (2001) Quantifying the supercontinuum coherence 150 fs input pulses, 1 nJ energy at 850 nm, 10 cm of PCF ● We quantify the phase stability in terms of the degree of coherence: Dudley and Coen, Opt. Lett. 27, 1180 (2002) Experimentally accessible Gu et al. Opt. Exp. 11, 2697 (2003). Lu & Knox Opt. Exp. 12, 347 (2004). Giessen et al. Talk today at 15:15 Quantifying the supercontinuum coherence 150 fs input pulses, 1 nJ energy at 850 nm, 10 cm of PCF ● We quantify the phase stability in terms of the degree of coherence: Dudley and Coen, Opt. Lett. 27, 1180 (2002) Experimentally accessible Gu et al. Opt. Exp. 11, 2697 (2003). Lu & Knox Opt. Exp. 12, 347 (2004). Giessen et al. Talk today at 15:15 Conclusions Physics of femtosecond pulse pumped SC generation in PCF with a single ZDW can be understood in terms of well-known physics. More novel effects (higher order dispersion, negative dispersion slope) may have been anticipated theoretically but PCF allows them to be studied through clean experiments. Technological applications require that the physics is understood. Still a lot to do … noise, new SC regimes, more XFROG experiments, polarization-dependent effects…