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Diffstat (limited to 'source/know/concept/dispersive-broadening')
| -rw-r--r-- | source/know/concept/dispersive-broadening/index.md | 3 |
1 files changed, 2 insertions, 1 deletions
diff --git a/source/know/concept/dispersive-broadening/index.md b/source/know/concept/dispersive-broadening/index.md index 9642737..55a31e6 100644 --- a/source/know/concept/dispersive-broadening/index.md +++ b/source/know/concept/dispersive-broadening/index.md @@ -62,7 +62,8 @@ 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 $$\gamma = 0$$: -{% include image.html file="simulation-full.png" width="100%" alt="Dispersive broadening simulation results" %} +{% include image.html file="simulation-full.png" width="100%" + alt="Dispersive broadening simulation results" %} The **instantaneous frequency** $$\omega_\mathrm{GVD}(z, t)$$, which describes the dominant angular frequency at a given point in the time domain, |