DanSandberg
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From a textbook - The reason why the polarization plays a key role in the description of nonlinear optical phenomena is that a time-varying polarization can act as the source of new components of the electromagnetic field... the wave equation in nonlinear optical media often has the form:
\nabla 2 E - \frac{n<sup>2</sup>}{c<sup>2</sup>} \frac{d<sup>2</sup>E}{dt<sup>2</sup>} = \frac{1}{\epsilon c<sup>2</sup>}\frac{d<sup>2</sup>P<sup>NL</sup>}{dt<sup>2</sup>}
This equation is given with no derivation or justification. Can someone explain where this comes from?
EDIT: I'm having a really hard time getting the equation to come out correctly on the website. Its nabla to the second power operating on the electric field E minus the second time derivative of E times n squared over c squared (where n is the linear refractive index and c is the speed of light) equal to 1 over epsilon c squared times the second time derivative of the polarization. I'll try to uplaod a photo of the equation.
\nabla 2 E - \frac{n<sup>2</sup>}{c<sup>2</sup>} \frac{d<sup>2</sup>E}{dt<sup>2</sup>} = \frac{1}{\epsilon c<sup>2</sup>}\frac{d<sup>2</sup>P<sup>NL</sup>}{dt<sup>2</sup>}
This equation is given with no derivation or justification. Can someone explain where this comes from?
EDIT: I'm having a really hard time getting the equation to come out correctly on the website. Its nabla to the second power operating on the electric field E minus the second time derivative of E times n squared over c squared (where n is the linear refractive index and c is the speed of light) equal to 1 over epsilon c squared times the second time derivative of the polarization. I'll try to uplaod a photo of the equation.