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ω1+ω2=ω3 (or 1/λ1+1/λ2=1/λ3 in wavelength)

It combines two low energy (or low frequency) photons into a high energy photon.

For example:1064nm+1064nm→532nm

Optical Parametric Generation (OPG) is an inverse process of sum Frequency Generation. It splits one high-frequency photon (pumping wavelength, lp) into two low-frequency photons (signal, ls, and idler wavelength, li). If two mirrors are added to from a cavity as shown in fig. 7, an Optical Parametric Oscillator (OPO) is established. For a fixed pump wavelength, an infinite number of sigal and idler wavelengths can be generated by tilting a crystal. Therefore, OPO is an excellent source for generating wide tunable range coherent radiation. KTP and LINbO3 are good crystal for OPO and Optical Parametic Amplifier (OPA)Applications.

ω1-ω2=ω3(or 1/λ1+1/λ2=1/λ3 in wavelength)

It combines two high energy photons into a low energy photon.

For example:532nm-810nm→1550nm

The frequency conversion processes include frequency doubling (which is a special case of sum frequency generation), sum frequency generation (SFG), differential-frequency generation (DFG) and optical parametric generation (OPG) which are demonstrated in the following equations:

Frequency Conversion

Sum Frequenby Generation (SFG)

Differential-Frequency Generation (DFG)  

Optocal Parametric Generatiom (OPG)


ωp-ωs=ωi(or 1/λp=1/λs+1/λi in wavelength)

It splits one high energy photon into two low energy photons.

For example:532nm→810nm+1550nm

Second Harmonic Generation(SHG)

Frequency Doubling is a special case of sum frequency generation if the two input wavelengths are the same.



Third Harmonic Generation(THG)


Optical Parametric Oscillation

IN order to obtain high conversion efficiency, the phase vectors of input beams and generated beams have to be matched:

ΔK=k3-k2-k1=2p(n3/l3-n2/l2-n1/l1)=0 (For sum frequency generation)

Where:ΔK is phase mismatching, ki is phase vector at li and ni is refractive index atli.

In low power case, the relationship between conversion efficiency and phase mismatching is:



It is clear that the conversion efficiency will drop dramatically if ΔK increases. The phase-matching can be obtained by angle tilting, temperature tuning or other methods. The angle tilting is mostly used to obtain phase-matching as shown. If the angle between optical axis and beam propagation (q) is not equal to 90 deg. or 0 deg., we call it Critical phase-matching (CPM). Otherwise, 90deg. non-critical phase-matching (NCPM) is for q=90deg. and 0 deg. NCPM is for q=0deg.

Two types of phase-matching are classsified in consideration of polarization of lasers. If the polarizations of two input beams (for sum frequency) are parallel to each other., it is type I phase-matching. If the polarizations are perpendicular to each other, it is called type II phase-matching.

If a laser light propagates in the direction with angle Δq to phase matching direction, the conversion efficiency will reduce dramatically. We define the acceptance angle (Δq) as full angle at half maximum (FAHM), where q=0 deg. is phase-matching direction. For example, the acceptance angle of BBO for type I frequecny  doubling of Nd:YAG at 1064nm is about 1mrad-cm. therefore, if a Nd:YAG laser has beam dibergence of 3mrad for frequency-doubling, over half of the input power is useless. In this case, LBO may be better because of its larger acceptance angle, about 8 mrad-cm. For NCMP, the acceptance angle is normally much bigger than that for CPM, for example, 52 mrad-cm(1/2) for type I NCPM LBO.
In addtion, you have to consider the Spectral acceptance (Δl) of crystal and the spectral bandwidth of your laser; crystal temperature acceptance (ΔT)and the temperature change of environment.

Crystal Acceptance

Due to the birefringence of NLO crystals, the extraordinary wave (ne)will experience Poynting vector walk-off as shown. If the beam size of input beam will be separated at walk-offangle(ρ) in the crystal and it will cause low conversion efficiency. Therefore, for focused beam or intracavity doubling, the walk-off is a main limitation to high conversion efficiency.



For NLO processes of ultrafast lasers such as Ti:Sapphire and Dye lasers with femtosecond (fs) pulse width, the main limitation to conversion efficiency is group velocity mismatching(GVM). The GVM is caused by group velocity dispersion of NLO crystal. For frequency doubling a Ti:sapphire laser at 800nm, for example, the inverse group velocities (1/VG)of BBO are respectively 1/VG=56.09ps/cm at 800nm and 1/VG=58.01ps/cm at 400nm and GVM=1.92ps/cm. That means an 1mm long BBO crystal will make 192fs separation between the pulses at two wavelengths. Therefore, for an 100fs Ti:sapphire laser, we normally recommend a 0.5mm long BBO crystal (with 96 fs separation) in order to obtain high effciency without dramatic pulse broadening.

Group Velocity Mismatching

Frequency Tripling is an example of Sum Frequency Generation where.