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Diffstat (limited to 'content/know/concept/dispersive-broadening/index.pdc')
| -rw-r--r-- | content/know/concept/dispersive-broadening/index.pdc | 4 |
1 files changed, 3 insertions, 1 deletions
diff --git a/content/know/concept/dispersive-broadening/index.pdc b/content/know/concept/dispersive-broadening/index.pdc index 7342295..f053eb6 100644 --- a/content/know/concept/dispersive-broadening/index.pdc +++ b/content/know/concept/dispersive-broadening/index.pdc @@ -64,7 +64,9 @@ 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 $\gamma = 0$: -<img src="pheno-disp.jpg"> +<a href="pheno-disp.jpg"> +<img src="pheno-disp-small.jpg"> +</a> The **instantaneous frequency** $\omega_\mathrm{GVD}(z, t)$, which describes the dominant angular frequency at a given point in the time domain, |