Categories: Fiber optics, Optics, Physics.

# Dispersive broadening

In optical fibers, **dispersive broadening** is a linear effect
where group velocity dispersion (GVD) “smears out” a pulse in the time domain
due to the different group velocities of its frequencies,
since pulses always have a nonzero width in the $\omega$-domain.
No new frequencies are created.

A pulse envelope $A(z, t)$ inside a fiber must obey the nonlinear Schrödinger equation, where the parameters $\beta_2$ and $\gamma$ respectively control dispersion and nonlinearity:

$\begin{aligned} 0 = i \pdv{A}{z} - \frac{\beta_2}{2} \pdvn{2}{A}{t} + \gamma |A|^2 A \end{aligned}$We set $\gamma = 0$ to ignore all nonlinear effects, and consider a Gaussian initial condition:

$\begin{aligned} A(0, t) = \sqrt{P_0} \exp\!\bigg(\!-\!\frac{t^2}{2 T_0^2}\bigg) \end{aligned}$By Fourier transforming in $t$, the full analytical solution $A(z, t)$ is found to be as follows, where it can be seen that the amplitude decreases and the width increases with $z$:

$\begin{aligned} A(z,t) = \sqrt{\frac{P_0}{1 - i \beta_2 z / T_0^2}} \exp\!\bigg(\! -\!\frac{t^2 / (2 T_0^2)}{1 + \beta_2^2 z^2 / T_0^4} \big( 1 + i \beta_2 z / T_0^2 \big) \bigg) \end{aligned}$To quantify the strength of dispersive effects, we define the dispersion length $L_D$ as the distance over which the half-width at $1/e$ of maximum power (initially $T_0$) increases by a factor of $\sqrt{2}$:

$\begin{aligned} T_0 \sqrt{1 + \beta_2^2 L_D^2 / T_0^4} = T_0 \sqrt{2} \qquad \implies \qquad \boxed{ L_D \equiv \frac{T_0^2}{|\beta_2|} } \end{aligned}$This phenomenon is illustrated below for our example of a Gaussian pulse with parameter values $T_0 = 1\:\mathrm{ps}$, $P_0 = 1\:\mathrm{kW}$, $\beta_2 = -10 \:\mathrm{ps}^2/\mathrm{m}$ and $\gamma = 0$:

The **instantaneous frequency** $\omega_\mathrm{GVD}(z, t)$,
which describes the dominant angular frequency at a given point in the time domain,
is found to be as follows for the Gaussian pulse,
where $\phi(z, t)$ is the phase of $A(z, t) = \sqrt{P(z, t)} \exp(i \phi(z, t))$:

This expression is linear in time, and depending on the sign of $\beta_2$, frequencies on one side of the pulse arrive first, and those on the other side arrive last. The effect is stronger for smaller $T_0$: this makes sense, since shorter pulses are spectrally wider.

The interaction between dispersion and self-phase modulation
leads to many interesting effects,
such as modulational instability
and optical wave breaking.
Of great importance is the sign of $\beta_2$:
in the **anomalous dispersion regime** ($\beta_2 < 0$),
lower frequencies travel more slowly than higher ones,
and vice versa in the **normal dispersion regime** ($\beta_2 > 0$).

## References

- O. Bang,
*Numerical methods in photonics: lecture notes*, 2019, unpublished.