# Physical meaning of Phase matching

Can anyone help me understand what exactly is meant by phase matching? I want to know whether momentum can be conserved only under phase matching condition or phase matching condition ensures momentum conservation. How does momentum conservation ensure efficient transfer of energy between waves? How is phase matching related to various matrix elements of susceptibility? I have been struggling with these fundamental questions for a long time.

• uh, you linked a google search? – anon01 Apr 4 '16 at 16:42
• momentum conservation is true whether or not a phase matching condition is met. You may want to ask a single, specific question about phase matching to get a good answer. – anon01 Apr 4 '16 at 16:44
• "Momentum is conserved, as is necessary for phase-matching" (en.wikipedia.org/wiki/Quasi-phase-matching) Please explain this. Thanks – Aswin Alex Apr 4 '16 at 17:53
• You'll get a better answer if you tell us what the context is, what you know, and what confuses you. In nonlinear optics, you generally want your field to build up. For that, the two waves have to have the same phase. If not, there will be alternating growth and reduction of the field, resulting in almost no output. – garyp Apr 4 '16 at 19:43
• I want to understand the interaction between the various waves inside a non-linear crystal with a space-time picture. Is phase matching a condition which will sustain an efficient transfer of energy between waves throughout the non-linear crystal? Should momentum be conserved at each instant of time everywhere inside the crystal? If yes, is this the reason why phase matching requirement is imposed for efficient transfer of energy? – Aswin Alex Apr 5 '16 at 4:56

For sum frequency generation ($\omega_1+\omega_2=\omega_3$) $\Delta\phi=\phi_3-\phi_2-\phi_1$. If $\Delta\phi=-\pi/2$ the energy transfer will occur from $\omega_3$ to $\omega_2$ and $\omega_1$ making photon split. If $\Delta\phi=+\pi/2$ the energy transfer will occur from $\omega_1$ and $\omega_2$ to $\omega_3$ making photon merger.
Between the two cases the efficiency of one of the two process will decrease. If the phase matching relation tells you that $\phi_3=\pi/2+\phi_1+\phi_2$. The phase $\phi_1$ and $\phi_2$ are given by your optical sources at $\omega_1$ and $\omega_2$. But if you add a signal at $\omega_3$ to stimulate the nonlinear process it will deteriorate the efficiency if $\phi_3$ is not exactly the phase given by the phase matching condition.