First demonstration of an NLO effect First demonstration of SHG: The Data Laser demonstrated in 1960 (Maiman) The actual published results… P.A. Franken, et al, Physical Review Letters 7, p. 118 (1961) The second harmonic Focused 3kW of pulsed red light (694.3 nm) from a Ruby laser onto a quartz crystal and observed some UV light (347.15 nm) coming out (SHG). Input beam Note that the very weak spot due to the second harmonic is missing. It was removed by an overzealous Physical Review Letters editor, who thought it was a speck of dirt. At that time the conversion efficiency was 1 in 108. Dr. L. Bradley Why is the conversion efficiency so low? Generation of light at the new frequencies is not just a question of having a high intensity beam or the size of the susceptibility Dr. L. Bradley SHG To see the implication of this lets look at the specific example of SHG Conditions: Do we have the whole story? Under what conditions do we achieve the maximum conversion? Coupled Wave Equations The issue of phase-matching? There must be a relationship between the frequencies ω1, ω2 and ω3 in order to drive an oscillation at ω3 ω1=ω2 = ω E(ω1)=E(ω2 )=E(ω) ω3=ω1 + ω2=2ω E(ω3)=E(2ω) The amplitude of each field depends on the amplitude of the other fields as they propagate. They are coupled through the nonlinear susceptibility. And there is a term dependent on their relative propagation speeds, i.e their phase relationship. Dr. L. Bradley Dr. L. Bradley Maximum I2ω SHG ⎛ Δkl ⎞ Sin 2 ⎜ ⎟ 1 ε 2ω ⎡ 2 2 2 μ 4 ⎤ ⎝ 2 ⎠ I 2ω = E0ω ⎥ ω d l ⎢ 2 ε 2ω 2 μ ⎣ ⎦ ⎛ Δkl ⎞ ⎟ ⎜ I2ω ∝ Iω2 ∝ Eω4 ⎝ 2 ⎠ ⎛ Δkl ⎞ Sin 2 ⎜ ⎟ ⎝ 2 ⎠ =1 2 ⎛ Δkl ⎞ ⎜ ⎟ ⎝ 2 ⎠ Δkl =0 2 Δk = 0 Intensity of the second harmonic signal generated is proportional to the square of the input intensity at ω The Dr. L. Bradley Maximum 2nd harmonic intensity will be achieved when Δk=0 Dr. L. Bradley 1 But isn’t this conservation of momentum? Conservation Laws for Photons in NLO Energy must be conserved: r r hkout = hkin r r r hk2ω = hkω + hkω r r k2ω = 2kω And light of this frequency will have the corresponding wavevector: or r r k2ω − 2kω = Δk = 0 Dr. L. Bradley ω1 + ω 2 + ω3 − ω 4 + ω5 = ω0 is the k-vector of the induced light c λ = ωo nω o c Momentum must be conserved: r r r p p = p1 + p2 kp is the wavevector of the induced polarization, and it may not correspond to the kvector of the induced light E h p = = = hk c λ r r r hk p = hk1 + hk 2 r r r k p = k1 + k2 Satisfying these two relations simultaneously is called "phase-matching." Dr. L. Bradley Phase matching condition for SHG Δk = 0 = k2ω − 2kω k2ω = 2kω Momentum : r r r r r r k p = k1 + k 2 + k 3 − k 4 + k 5 2πnω r k p = ko ? Satisfying these two relations simultaneously is called "phase-matching." Thanks to Rick Trebino http://www.physics.gatech.edu/gcuo/UltrafastOptics/index.html 2πnωo ω2= ω1 energy Energy : nωo ωo kω o = Phase Matching Condition More general picture - multiphoton kω o = hωout = hω1 + hω 2 ωout = ω1 + ω 2 2ωn2ω = kω = , k 2ω = c c λ 2ω (n2ω − nω ) Δk = k2ω − 2kω = =0 c n2ω = nω ω0=2ω1 ω1 ωnω Dr. L. Bradley y 2k1 k1 k1 Dr. L. Bradley What is this telling us? Coherence length Applied E field induces polarization field which travels at the same speed in the medium as the incident field ->The resulting oscillating dipoles emit radiation. Only when the radiation from each dipole adds constructively (are in phase) will a propagating EM wave be generated. The distance it takes for the charge polarization wave and the radiated light to get 1800 out of phase is the coherence length – if crystal length = odd multiple of lc no light 2nd harmonic light will be emitted lc Unless the light generated is travelling at the same speed as the charge polarization wave, light radiated from one part of the crystal will not be in phase with light radiated from another part, and they will destructively interfere at some point Phase-matching must be considered in all nonlinear-optical problems. Dr. L. Bradley Dr. L. Bradley 2 Coherence length Coherence length When z=lc lc = lc = π Δk = lc is a measure of the maximum crystal length that is useful in producing 2nd harmonic power If the crystal is longer the 2nd harmonic waves will interfere and the efficiency will be very low. This distance is typically <10-2 cm. Z/lc πc 2ω (n2ω − nω ) 1 πc λ0 = ω 2(n2ω − nω ) 4(n2ω − nω ) Dr. L. Bradley Achieving phase matching Have interference described by the factor Phase matching condition ⎛ Δkl ⎞ Sin 2 ⎜ ⎟ ⎝ 2 ⎠ 2 ⎛ Δkl ⎞ ⎜ ⎟ ⎝ 2 ⎠ Δk = 0 = k2ω − 2kω k2ω = 2kω this from ever happening! Dr. L. Bradley Phase-matching Second-Harmonic Generation using Birefringence Birefringent materials have different refractive indices for different polarizations. “Ordinary” and “extraordinary” refractive indices can be different by up to ~0.1 for SHG crystals. We can now satisfy the phase-matching condition. Use the extraordinary polarization for ω and the ordinary for 2ω. Refractive index n2ω = nω Unfortunately, dispersion prevents I2ω ∝ l2, so phase matching is crucial to be able to use longer crystals no (2ω ) = ne (ω ) ω Frequency 2ω ω Frequency 2ω Dr. L. Bradley SHG crystal Input beam Input beam no Birefringence Light created in real crystals Closer to phase-matching: ne ne depends on propagation angle, so we can tune for a given ω. Some crystals have ne < no, so the opposite polarizations work. Dr. L. Bradley Far from phase-matching: Refractive index ⎛ Δkz ⎞ Sin 2 ⎜ ⎟ 2 ⎝ 2 ⎠ I 2ω ( z ) ∝ I ω 2 ⎛ Δk ⎞ ⎜ ⎟ ⎝ 2 ⎠ Δkz π Max when = 2 2 Output beam The molecular "spring constant" can be different for different directions. SHG crystal Output beam Note that SH beam is brighter as phase-matching is achieved. Dr. L. Bradley Dr. L. Bradley 3 Birefringence Birefringence Angle tuning The x- and y-polarizations can see different refractive index curves. Or can also use temperature tuning – not shown Dr. L. Bradley Tuning With birefringence can even tune the refractive index as a function of angle Dr. L. Bradley Crystals 1 Cos 2θ Sin 2θ = + 2 ne2 (θ ) n02 ne 1 (n ) ω 2 0 = Cos 2θ m (n ) 2ω 2 0 + Sin 2θ m (n ) 2ω 2 e matched direction at an angle of approx 350 to the optic axis. Usually divided into 2 groups – depending on whether the crystal structure remains unchanged under inversion Centrosymmetric e.g. NaCl Inversion of any ion about the central Na+ ion leaves the structure unchanged. Index Non-centrosymmetric e.g. ZnS zinc blende class, GaAs, CdTe Dr. L. Bradley Crystal Symmetry Dr. L. Bradley d Due to crystal symmetry there are no 2nd order polarization effects in centrosymmetric media. Dr. L. Bradley NB lack of uniformity in textbooks Dr. L. Bradley 4 A couple of examples from the laser called FRED, want to generate very low lab UV wavelength (high energy photons) laser to investigate novel wideband gap materials e.g. ZnO for optoelectronic (polariton lasers, efficient white lights) and medical applications. No easy source available at these wavelengths < 300 nm So we use SHG. Light at 488 nm, easily produced by a standard Ar+ laser is converted to 244 nm See only 6-7% conversion efficiency but it is the only way! Intra cavity conversion Using a BBO crystal – transparent from 200 nm to 2000 nm To get appreciable conversion requires large power densities (W/m2) at the fundamental 2 Usually not available from CW lasers I 2ω ∝ I ω BUT can place the NL crystal in the laser resonantor From your laser physics: the intensity inside the cavity exceeds its value outside by (1-R)-1, R is the mirror reflectivity. For R~1 the enhancement is large, so more efficient conversion is achieved. Dr. L. Bradley Intracavity SHG Conversion Dr. L. Bradley Photon energy level representation – energy conservation Ar+ laser Under the proper conditions with the proper mirrors, can extract the total available power at 2ω IR laser ω (λ= 1064 nm), 2ω (λ = 532 nm) Dr. L. Bradley Some experimental results NL crystal ω3 ω1 ω1 ω3=ω1+ ω2 ω2 ω2 BBO UV laser ω (λ= 488 nm), 2ω (λ = 244 nm) The intracavity intensity is >100 kW/m2 The phase matching is achieved via the birefringence ω light propagates as the ordinary ray, 2ω as the extraordinary ray Frequency Sum P = ε 0 χ (2) E1 E2 Second Harmonic Generation ω1= ω2 ω3=2ω1 P = ε 0 χ (2) E12 ω1 ω1 ω3 Dr. L. Bradley Expt: Frequency Sum 2nd A new material for nonlinear effects: PPLN Can achieve phasematching over long lengths, e.g. 8 cm Highly efficient, but very temperature dependent Working at optical telecommunications wavelengths 1521 nm 1527 nm 1532 nm 763.2 nm 763.5 nm Dr. L. Bradley Dr. L. Bradley 5 Induced polarization for nonlinear optical effects Frequency Difference ω1 NL crystal ω2 ω3=ω1- ω2 ω1 ω2 ω3 P = ε 0 χ (2) E1 E2* For every photon created at the difference frequency ω3 a photon at frequency ω1 must be destroyed and a photon at ω2 created. Incoming photon at ω1 excites the atom to the highest virtual level, incoming photon at ω2 stimulates the emission of a photon at ω2 and for energy conservation a photon at ω3 is also emitted. ⇒ Amplification of the input light at ω2 Optical Parametric Amplification Dr. L. Bradley Arrows pointing upward correspond to absorbed photons and contribute a factor of their field, Ei; arrows pointing downward correspond to emitted photons and contribute a factor the complex conjugate of their field: P = ε 0 χ (5) E1 E2 E3 E4* E5 r r r r P ( n ) (Ω = ω1 + ω 2 + ... + ω n ) = ε 0 χ ( n ) (− Ω, ω1 , ω 2 ,..., ω n )E(ω1 ) E(ω2 ) ...E(ωn ) Ω is the resulting frequency Dr. L. Bradley Difference-Frequency Generation: Optical Parametric Generation, Amplification, Oscillation Difference-frequency generation takes many useful forms. ω1 ω3 ω2 = ω3 − ω1 ω1 ω3 Parametric Down-Conversion (Difference-frequency generation) ω1 ω1 ω3 ω2 ω2 Optical Parametric Generation (OPG) "idler" By convention: ωsignal > ωidler ω1 ω3 ω2 mirror Optical Parametric Amplification (OPA) "signal" mirror Optical Parametric Oscillation (OPO) Dr. L. Bradley 6
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