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Optical Parametric Devices David Hanna Optoelectronics Research Centre University of Southampton Lectures at Friedrich Schiller University, Jena July/August.

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Presentation on theme: "Optical Parametric Devices David Hanna Optoelectronics Research Centre University of Southampton Lectures at Friedrich Schiller University, Jena July/August."— Presentation transcript:

1 Optical Parametric Devices David Hanna Optoelectronics Research Centre University of Southampton Lectures at Friedrich Schiller University, Jena July/August 2006

2 Outline of lecture series: Optical parametric Devices Lecture1: Optical parametric devices: an overview Lecture2: Optical parametric amplification and oscillation: Basic principles Lecture3: Ultra-short pulse parametric devices Lecture4: The role of Quasi-Phase Matching in parametric devices, PLUS Brightness enhancement via parametric amplification

3 Lecture 1 Optical Parametric Devices: an overview David Hanna Optoelectronics Research Centre University of Southampton Lectures at Friedrich Schiller University, Jena July/August 2006

4 Peter Alden Franken

5 Optical parametric amplification 3 – wave interactions input ω 2, wave is amplified (parametric amplification) Energy conservation, ћω 1, ћω 2 annihilated, ћω 3 created SFG DFG ћω 3 annihilated, ћω 2, ћω 1 created

6 10 -8 photon conversion efficiency, 10 -6 %, 3x10 -10 %/W 2006 Capability: ~1000%/W→13 orders in 45 years

7 Parametric gain: key information needed  Magnitude of gain, and its dependence on crystal length, pump intensity, crystal nonlinearity  Gain bandwidth, ie range of signal wavelengths that experience amplification For significant gain, need phase-matching k 3 = k 1 + k 2 n 3 ω 3 = n 1 ω 1 +n 2 ω 2 (co-linear)


9 Parametric amplification and parametric noise Input pump spontaneously generates pairs of photons ћω 1, ћω 2 (parametric noise) which are then amplified. Transparent nonlinear (χ (2) ) dielectric Pump Signal Signal (amplified) Idler (generated) Amplified noise > > > > ω3ω3 ω2ω2 ω1ω1 ω2ω2 > ω3ω3 > > ω1ω1 ω2ω2 > >


11 Optical parametric oscillation Doubly-resonant oscillator (DRO) Singly-resonant oscillator (SRO) Pump Signal Idler Signal Idler

12 Parametric gain vs laser gain  Gain peak can be tuned, by tuning the phase-match condition (change tilt of crystal, or temperature, or QPM grating period). Very wide signal-idler tuning is possible.  Gain is produced at two wavelengths – two outputs. Choice of resonator (DRO or SRO).  Coherent relation between interacting waves; restriction on relative direction of the waves. No analogue of side-pumped laser. Finite range of allowed pump wave directions can amplify single signal wave. Multimode pump can be used.  brightness enhancement

13 Parametric gain vs laser gain  Gain only present while pump is present. No storage of gain/energy No equivalent of Q-switching. Few OPO round trips if nsec Q-switched pump pulses are used.  Gain is determined by peak pump intensity: very high gain with intense ultrashort pump pulses.  No energy exchange with nonlinear medium – only exchange between the interacting waves. No heat input to the medium

14 Parametric devices Oscillators:SRO or DRO, pump: single-pass, double-pass or resonated, cw or pulsed. long pulse (many round trips), or train of short pulses, SPOPO (synchronously pumped OPO) OP Amplifier:input signal provided OP Generator:no input signal, output generated by amplification from parametric noise Pump Signal Idler > > >

15 Synchronously-pumped OPO Mode-locked pump: pulse separation matches round trip of OPO Signal and idler output pulse train  OPO gain corresponds to the peak power of the pump pulse  Crystal length must be short enough so that group velocity dispersion does not separate pump, signal and idler pulses in the crystal. > > > > > N.L.Xtal

16 Attractions of SPOPO  Low threshold average power  Synchronised outputs at two wavelengths (e.g. for CARS)  Very high gain possible, can oscillate even with very high idler loss  Very high efficiency, e.g. makes the tandem OPO practical

17 Quasi-Phase-Matching Proposed Armstrong, Bloembergen, Ducuing, Pershan, Phys Rev 27,1918,(1962)

18 Periodic-poling scheme (e.g. as in PPLN)  -   -   -  Period = 2 l c 1 st order phase-matching lclc 2 l c period E SH after each l c is  / 2 smaller than for perfect phase-matching over the same length of medium. So, effective nonlinear coefficient reduced by  / 2. 2lc2lc lclc 4lc4lc 3lc3lc E SH 2lc2lc lclc 3lc3lc 4lc4lc Phase-matched Quasi- phase- matched

19 Some benefits of QPM Access materials having too low a birefringence for phase-matching, e.g. LiTaO 3, GaAs Ability to phase-match any frequencies in the transparency range, freedom to choose ideal pump for an OPO Non-critical (90°) phase-matching, allows tight (confocal) focussing Access to largest nonlinear coefficient, e.g. d 33 in LiNbO 3

20 Periodically Poled Lithium Niobate Crystal Acknowledgements to Peter Smith, Corin Gawith and Lu Ming ORC, University of Southampton

21 Frequency-conversion efficiency and parametric gain in PPLN (Waveguide enhancement by lλ/2nw 2 ~10 2 -10 3 ; >1000%/ Wcm 2 ) Parametric gain, 1µm → 2µm, ~0.25% / Wcm (PPLN) 2µm → 4µm, ~0.5% / Wcm (GaAs) SHG,1064nm → 532nm or Parametric gain 532nm → 1064nm ~2%/ Wcm (d eff = 17pm/V) SHG conversion efficiency, confocal focus ( l = b = 2π w o 2 n 1 /λ) (ω 1 → 2ω 1 ) ~ 16π 2 P(ω 1 )d 2 eff l /cє 0 n 1 n 2 λ 1 3

22 Minimum pump power/energy for 1µm – pumped PPLN parametric devices cw SRO ~1-3W Nanosecond-pumped OPO ~5 µJ Synchronously-pumped OPO ~100pJ (~10 mW @ 100 MHz) Optical parametric generator ~100nJ (fs/ps) ~100µJ (1 nsec) 130 dB gain All power/energy values scale as (d 2 /n 2 λ 3 ) -1

23 CW singly-resonant OPOs in PPLN  First cw SRO: Bosenberg et al. O.L., 21, 713 (1996) 13w NdYAG pumped 50mm XL, ~3w threshold, >1.2w @ 3.3µm  Cw single-frequency: van Herpen et al. O.L., 28, 2497 (2003) Single-frequency idler, 3.7 → 4.7 µm, ~1w → 0.1w  Direct diode-pumped: Klein et al. O.L., 24, 1142 (1999) 925nm MOPA diode, 1.5w thresh., 0.5w @ 2.1µm (2.5w pump)  Fibre-laser-pumped: Gross et al. O.L., 27, 418 (2002) 1.9w idler @ 3.2µm for 8.3w pump

24 Some results from PPLN ps/fs parametric devices ●Low threshold SPOPO; 7.5 mW (av), 1047nm pump, 4ps, @120 MHz 21mW, pumped by Yb fibre laser ●High gain devices (at mode-locked rep. rate) Widely-tuned SPOPO, idler >7µm OPCPA, 40 dB gain, mJ output OPG operated at 35 MHz, ~0.5W signal ●High average power femtosecond SPOPO 19W (av) signal @ 1.45 µm, 7.8W @ 3.57 µm

25 SPOPO facts and figures  Average output power > 20 W  Shortest pulses13 fs  Tuning range0.45 – 9.7 micron  Efficiency (diode  laser  OPO)25%  Slope efficiency>100% (170% observed)

26 PPLN Waveguide Optical Parametric Generator ~2ps, 200pJ, (100W) pump @ 780nm gives ~100dB gain @1550nm 10dB needs a pump Power of 1W XieXie Xie et al JOSA B, 21, 1397, (2004)

27 Two spatial-mode waveguide parametric amplifier OPG threshold: 300pJ, 2ps @ 780nm Xie & Fejer, Optics Letters, 31, 799, (2006)

28 OPCPA Optical Parametric Chirped Pulse Amplification Butkus et al Applied Physics B, 79, 693 (2004)

29 The OPCPA march towards Petawatts Dubietis et al IEEE J Sel Topics in QE,12, 163, (2006)

30 Brightness Enhancement via Parametric Amplification Although parametric amplification requires a high-brightness pump, this does not imply a perfect, diffraction-limited pump. A range of pump wave angles (modes) can effectively pump a SINGLE signal wave (mode). So the amplified signal wave can be brighter than the input pump. ▼ Brightness Enhancement (and no heat input)

31 Angular acceptance of pump I ΔkL = π sets limit to θ Next: relate Δk to θ Angular acceptance: determined by the phase-mismatch, Δk, that can be tolerated kpkp ksks kpkp kiki kiki ΔkΔk ΔkΔk θ

32 Concluding remarks Χ (2) Parametric processes now have the pump sources they need and deserve. Χ (2) Parametric devices are very versatile cw to femtosecond UV to TeraHertz mW→TW→PW Absence(?) of heat generation in active medium is of growing interest. Caveat: There is not an abundance of suitable χ (2) nonlinear media.

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