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-rw-r--r--content/know/concept/dispersive-broadening/index.pdc4
-rw-r--r--content/know/concept/dispersive-broadening/pheno-disp-small.jpgbin0 -> 95385 bytes
2 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,
diff --git a/content/know/concept/dispersive-broadening/pheno-disp-small.jpg b/content/know/concept/dispersive-broadening/pheno-disp-small.jpg
new file mode 100644
index 0000000..8c70eac
--- /dev/null
+++ b/content/know/concept/dispersive-broadening/pheno-disp-small.jpg
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