From 20e7c96c35b922252e17fd5fc9ff0407d9bd30ca Mon Sep 17 00:00:00 2001
From: Prefetch
Date: Mon, 1 Mar 2021 11:45:21 +0100
Subject: Optimize images

---
 content/know/concept/dispersive-broadening/index.pdc | 4 +++-
 1 file changed, 3 insertions(+), 1 deletion(-)

(limited to 'content/know/concept/dispersive-broadening/index.pdc')

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,
-- 
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