Slowly varying envelope approximation

In physics, the slowly varying envelope approximation (SVEA) refers to the assumption that the envelope of a forward-travelling wave pulse varies slowly in time and space compared to a period or wavelength. This requires the spectrum of the signal to be narrow banded. Which it why it also referred to as the narrow band approximation.

The slowly varying envelope approximation is often used because the resulting equations are in many cases easier to solve than the original equations, reducing the order of—all or some of—the highest-order partial derivatives. But the validity of the assumptions which are made need to be justified.

Example

For example, consider the electromagnetic wave equation:

$\nabla ^{2}E-\mu _{0}\,\epsilon _{0}\,{\frac {\partial ^{2}E}{\partial t^{2}}}=0.$

If k_o and ω_o are the wave number and angular frequency of the (characteristic) carrier wave for the signal E(r,t), the following representation is useful:

$E(\mathbf {r} ,t)=\Re \left\{E_{0}(\mathbf {r} ,t)\,e^{i\,(\mathbf {k} _{0}\,\cdot \,\mathbf {r} -\omega _{0}\,t)}\right\},$

with $\Re \{\cdot \}$ denotes taking the real part of the quantity between brackets.

In the slowly varying envelope approximation (SVEA) it is assumed that E_o(r,t) only varies slowly with r and t. This inherently implies that E_o(r,t) represents waves propagating forward, predominantly in the k_o direction. As a result of the slow variation of E_o(r,t), when taking derivatives, the highest-order derivatives may be neglected:

${\Bigl |}\nabla ^{2}E_{0}{\Bigr |}\ll {\Bigl |}k_{0}\,\nabla E_{0}{\Bigr |}$   and   ${\Bigl |}{\frac {\partial ^{2}E_{0}}{\partial t^{2}}}{\Bigr |}\ll {\Bigl |}\omega _{0}\,{\frac {\partial E_{0}}{\partial t}}{\Bigr |},$   with  $k_{0}=|\mathbf {k} _{0}|.$

Full approximation

Consequently, the wave equation is approximated in the SVEA as:

$2\,i\,\mathbf {k} _{0}\,\cdot \nabla E_{0}+2\,i\,\omega _{0}\,\mu _{0}\,\epsilon _{0}\,{\frac {\partial E_{0}}{\partial t}}-\left(k_{0}^{2}-\omega _{0}^{2}\,\mu _{0}\,\epsilon _{0}\right)\,E_{0}=0.$

It is convenient to choose k_o and ω_o such that they satisfy the dispersion relation:

$k_{0}^{2}-\omega _{0}^{2}\,\mu _{0}\,\epsilon _{0}=0.\,$

This gives the following approximation to the wave equation, as a result of the slowly varying envelope approximation:

$\mathbf {k} _{0}\cdot \nabla E_{0}+\omega _{0}\,\mu _{0}\,\epsilon _{0}\,{\frac {\partial E_{0}}{\partial t}}=0.$

Parabolic approximation

Assume wave propagation is dominantly in the z-direction, and k_o is taken in this direction. The SVEA is only applied to the second-order spatial derivatives in the z-direction and time. If $\scriptstyle \Delta _{\perp }=\partial ^{2}/\partial x^{2}+\partial ^{2}/\partial y^{2}$ is the Laplace operator in the x–y plane, the result is:

$k_{0}{\frac {\partial E_{0}}{\partial z}}+\omega _{0}\,\mu _{0}\,\epsilon _{0}\,{\frac {\partial E_{0}}{\partial t}}-{\tfrac {1}{2}}\,i\,\Delta _{\perp }E_{0}=0.$

Which is a parabolic partial differential equation. This equation has enhanced validity as compared to the full SVEA: it can represents waves propagating in directions significantly different from the z-direction.

See also

• WKB approximation

References

• Butcher, Paul N.; Cotter, David (1991), The elements of nonlinear optics (reprinted ed.), Cambridge University Press, ISBN 0521424240