From adeae2e2b68c4867f51f0b2cf1e677b0e7d74248 Mon Sep 17 00:00:00 2001
From: Thomas Bredewoud <t.p.bredewoud@student.tudelft.nl>
Date: Thu, 11 May 2023 14:17:37 +0000
Subject: [PATCH] Update 14_doping_and_devices_solutions.md

---
 docs/14_doping_and_devices_solutions.md | 2 +-
 1 file changed, 1 insertion(+), 1 deletion(-)

diff --git a/docs/14_doping_and_devices_solutions.md b/docs/14_doping_and_devices_solutions.md
index 41a285a..37c4b54 100644
--- a/docs/14_doping_and_devices_solutions.md
+++ b/docs/14_doping_and_devices_solutions.md
@@ -27,7 +27,7 @@ $$ n_e - n_h + n_D - n_A = N_D - N_A $$
 Since $E_G \gg k_B T$, we can only use the law of mass action. 
 But the question offers us another piece of information - we are around $|N_D-N_A| \approx n_i$.
 That means that we are near the transition between extrinsic and intrinsic regimes.
-Because the dopants stop being ionized at very low temperatures (see next exercise), we can neglect $n_D$ and $n_A$ in this exercise, just like in the lecture.
+In this regime we can neglect $n_D$ and $n_A$ in this exercise, just like in the lecture.
 Writing $n_e n_h = n_i^2$ and $n_e - n_h = N_D - N_A$ and solving these together, we obtain
 
 \begin{align} 
-- 
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