Where Does the Nonlinear Optics Wave Equation Come From?

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SUMMARY

The nonlinear optics wave equation is derived from the interaction of electric fields and polarization in nonlinear optical media. The equation is expressed as: . This formulation incorporates a nonlinear polarization term, which is essential for describing the behavior of light in such media. The derivation involves applying Faraday's law and Ampere's law while assuming a divergenceless electric field.

PREREQUISITES
  • Understanding of Maxwell's equations, particularly Faraday's law and Ampere's law.
  • Familiarity with the concept of polarization in electromagnetic fields.
  • Knowledge of nonlinear optics and its applications.
  • Basic proficiency in LaTeX for formatting equations.
NEXT STEPS
  • Study the derivation of the wave equation in nonlinear optics from Boyd's book, specifically section 2.
  • Learn about the implications of nonlinear polarization in optical phenomena.
  • Explore the mathematical techniques for solving the nonlinear wave equation.
  • Investigate the use of LaTeX for accurately formatting and presenting scientific equations.
USEFUL FOR

Researchers, physicists, and students in optics and photonics, particularly those focusing on nonlinear optical phenomena and wave propagation in complex media.

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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