Sum-frequency generation

Sum-frequency generation (SFG) is a second order nonlinear optical process based on the annihilation of two input photons at angular frequencies $\omega _{1}$ and $\omega _{2}$ while, simultaneously, one photon at frequency $\omega _{3}$ is generated.[1] As with any second order $\chi ^{(2)}$ phenomenon in nonlinear optics, this can only occur under conditions where: the light is interacting with matter, which is asymmetric (for example, surfaces and interfaces); the light has a very high intensity (typically from a pulsed laser). Sum-frequency generation is a "parametric process",[2] meaning that the photons satisfy energy conservation, leaving the matter unchanged:

\hbar \omega _{3}=\hbar \omega _{1}+\hbar \omega _{2}

Second-harmonic generation

A special case of sum-frequency generation is second-harmonic generation, in which $\omega _{1}=\omega _{2}$ . In fact, in experimental physics, this is the most common type of sum-frequency generation. This is because in second-harmonic generation, only one input light beam is required, but if $\omega _{1}\neq \omega _{2}$ , two simultaneous beams are required, which can be more difficult to arrange. In practice, the term "sum-frequency generation" usually refers to the less common case in which $\omega _{1}\neq \omega _{2}$ .

Phase-matching

For sum-frequency generation to occur efficiently, a condition called phase-matching must be satisfied:[3]

\hbar k_{3}\approx \hbar k_{1}+\hbar k_{2}

where $k_{1},k_{2},k_{3}$ are the angular wavenumbers of the three waves as they travel through the medium. (Note that the equation resembles the equation for conservation of momentum.) As this condition is satisfied more and more accurately, the sum-frequency generation becomes more and more efficient. Also, as sum-frequency generation occurs over a longer and longer length, the phase-matching must become more and more accurate.

Sum frequency generation spectroscopy

Sum frequency generation spectroscopy uses two laser beams mixed at a surface to generate an output beam with a frequency equal to the sum of the two input frequencies. Sum frequency generation spectroscopy is used to analyze surfaces and interfaces.[4]

References

Akihiro Morita (2 August 2018). Theory of Sum Frequency Generation Spectroscopy. Springer Singapore. ISBN 9789811316074.
Boyd, Nonlinear Optics, page 14
Boyd, Nonlinear optics, page 79
Vidal, Franck; Tadjeddine, Abderrahmane (2005). "Sum-frequency generation spectroscopy of interfaces". Reports on Progress in Physics. 68 (5): 1095–1127. Bibcode:2005RPPh...68.1095V. doi:10.1088/0034-4885/68/5/R03. ISSN 0034-4885.

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[Morita2018-1] Akihiro Morita (2 August 2018). Theory of Sum Frequency Generation Spectroscopy. Springer Singapore. ISBN 9789811316074.

[2] Boyd, Nonlinear Optics, page 14

[3] Boyd, Nonlinear optics, page 79

[VidalTadjeddine2005-4] Vidal, Franck; Tadjeddine, Abderrahmane (2005). "Sum-frequency generation spectroscopy of interfaces". Reports on Progress in Physics. 68 (5): 1095–1127. Bibcode:2005RPPh...68.1095V. doi:10.1088/0034-4885/68/5/R03. ISSN 0034-4885.