Where Does the Nonlinear Optics Wave Equation Come From?

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Discussion Overview

The discussion revolves around the derivation of the nonlinear optics wave equation, specifically the equation involving the electric field E and the nonlinear polarization PNL. Participants seek clarification on the origins of this equation and its components, exploring theoretical aspects of nonlinear optical phenomena.

Discussion Character

  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant cites a textbook stating that time-varying polarization is crucial for nonlinear optical phenomena and presents the wave equation without derivation.
  • Another participant suggests consulting Boyd's book for further information on the topic.
  • Several participants attempt to clarify the notation and formatting of the equation, with one providing a corrected version of the equation as it appears in the original post.
  • A participant mentions that the derivation of the wave equation is similar to the usual derivation but includes a nonlinear polarization term, noting assumptions made during the process.
  • There is a discussion about potential technical issues with displaying the equation correctly on different operating systems and browsers.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the derivation of the wave equation, and there are multiple viewpoints regarding the assumptions and methods involved in its formulation.

Contextual Notes

Assumptions regarding the divergenceless nature of the electric field are mentioned, though this assumption may not hold strictly true in all contexts.

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.
 
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See Boyd's book, section 2.
 
Can't offer help, but I think this is what the equation in the OP is supposed to be:

\nabla^2E - \frac{n^2}{c^2} \ \frac{d^2 E} {dt^2} <br /> = \frac{1}{\epsilon c^2} \ \frac{d^2P^{NL}}{dt^2}
 
Redbelly98 said:
Can't offer help, but I think this is what the equation in the OP is supposed to be:

\nabla^2E - \frac{n^2}{c^2} \ \frac{d^2 E} {dt^2} <br /> = \frac{1}{\epsilon c^2} \ \frac{d^2P^{NL}}{dt^2}

thats exactly it - i think maybe cause I am on a mac? or maybe cause I'm using firefox? I'll see if my linux machine does a better job.
 
You can click on the equation I wrote to see the correct LaTex code. For example, superscripts in LaTex are made using the "^" character, not the [noparse][/noparse] tags.

Other users with macs have been able to write LaTex equations.
 
It's pretty much the usual derivation of the wave equation, except with a nonlinear polarization term kept along for the ride. That is, take the cross product of Faraday's law, substitute in Ampere's Law, and simplify. You have to also assume that the E field is divergenceless (which is not strictly true here, but is what people do nonetheless).
 

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