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-rw-r--r--source/know/concept/dispersive-broadening/index.md4
-rw-r--r--source/know/concept/dispersive-broadening/pheno-disp-small.jpgbin95385 -> 0 bytes
-rw-r--r--source/know/concept/dispersive-broadening/pheno-disp.jpgbin285990 -> 0 bytes
-rw-r--r--source/know/concept/dispersive-broadening/simulation-full.pngbin0 -> 670730 bytes
-rw-r--r--source/know/concept/dispersive-broadening/simulation-half.avifbin0 -> 30415 bytes
-rw-r--r--source/know/concept/dispersive-broadening/simulation-half.jpgbin0 -> 137095 bytes
-rw-r--r--source/know/concept/dispersive-broadening/simulation-half.pngbin0 -> 183226 bytes
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8 files changed, 1 insertions, 3 deletions
diff --git a/source/know/concept/dispersive-broadening/index.md b/source/know/concept/dispersive-broadening/index.md
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--- a/source/know/concept/dispersive-broadening/index.md
+++ b/source/know/concept/dispersive-broadening/index.md
@@ -59,9 +59,7 @@ 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 $$\gamma = 0$$:
-<a href="pheno-disp.jpg">
-<img src="pheno-disp-small.jpg" style="width:100%">
-</a>
+{% 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,
diff --git a/source/know/concept/dispersive-broadening/pheno-disp-small.jpg b/source/know/concept/dispersive-broadening/pheno-disp-small.jpg
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