Critical Phase Matching
Critical phase matching (also called angle phase matching) is a technique for obtaining phase matching of some nonlinear process (usually nonlinear frequency conversion) in a birefringent crystal. The interacting beams are aligned at some angle(s) to the axes of the index ellipsoid. In almost all cases, there are one or two waves linearly polarized along one axis of the index ellipsoid (ordinary beam), while another one or two waves are polarized at some variable angle with the plane spanned by the other two axes (extraordinary beams). Adjustment of the propagation angle affects the refractive index of the extraordinary beam (called extraordinary refractive index), whereas the ordinary index stays constant. For some angular position, phase matching may be achieved, i.e., the phase mismatch vanishes. Effectively this means that the birefringence exactly cancels the phase mismatch which would result from chromatic dispersion. Note that this would not be possible if all involved beams had the same polarization direction, since one would have no effect of the birefringence.
As an example, Figure 1 shows the beam direction and the polarization directions for phase-matched second-harmonic generation (frequency doubling) in LBO based on the type I scheme with polarizations oo-e in the XY plane. This means that beam propagates within the XY plane, the fundamental polarization is ordinary (o, here in the Z direction) and the second-harmonic polarization is extraordinary (e, with an angle φ to the Y axis). Figure 2 shows the required parameters. For example, for a pump wavelength of 800 nm the phase-matching angle φ would have to be 31.6°, and the effective nonlinearity would be 0.72 pm/V. The walk-off angle of the second-harmonic beam (not shown in the diagram) would be 16.5 mrad.
The attribute “critical” comes from the fact that this technique (in contrast to noncritical phase matching) is relatively sensitive to misalignment of the beams. There is only a finite range of beam angles (the acceptance angle, also called angular phase-matching bandwidth) where critical phase matching works; in the example above, it is 0.67 mrad for a 1 cm long crystal. This also implies that the beam divergence must be limited, and that often forces one to use beams with a large beam radius. Efficient nonlinear conversion then requires a higher peak power.
A related problem is the spatial walk-off between ordinary and extraordinary beams, which limits the effective interaction length and may affect both the conversion efficiency and the beam quality. With sufficiently high optical powers, walk-off effects can be minimized by using a short nonlinear crystal and/or large beam diameters.
Nonlinear crystals are often cut such that critical phase matching is possible for close to normal incidence on the input surface. It may be less convenient to use a crystal which needs a substantially non-normal incidence, e.g. because it was designed for use with noncritical phase matching.
A major advantage of critical phase matching is that the crystal temperature can often be close to room temperature, so that a crystal oven is not required. One may only need to stabilize the crystal temperature near room temperature, e.g. using a Peltier element. That also minimizes the required warm-up time.
The above mentioned limitations of critical phase matching can be severe in some cases, but get less relevant in cases where beams with a high peak power are converted.
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