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authorPrefetch2022-02-01 11:23:35 +0100
committerPrefetch2022-02-01 11:23:35 +0100
commit43c5b696aaf421dec7aee967002999d9145da35e (patch)
tree418dd75bb385a8922b9484883ae0d42124239c94 /content/know/concept/interaction-picture/index.pdc
parent88537b82784f71104c3a2771330c9e492f57fb03 (diff)
Expand knowledge base
Diffstat (limited to 'content/know/concept/interaction-picture/index.pdc')
-rw-r--r--content/know/concept/interaction-picture/index.pdc3
1 files changed, 2 insertions, 1 deletions
diff --git a/content/know/concept/interaction-picture/index.pdc b/content/know/concept/interaction-picture/index.pdc
index 45950ff..89aff58 100644
--- a/content/know/concept/interaction-picture/index.pdc
+++ b/content/know/concept/interaction-picture/index.pdc
@@ -197,7 +197,8 @@ $$\begin{aligned}
\mathcal{T} \bigg\{ \bigg( \int_{t_0}^{t} \hat{H}_{1,I}(t') \dd{t'} \bigg)^n \bigg\}
\end{aligned}$$
-Here, we recognize the Taylor expansion of $\exp$,
+This construction is occasionally called the **Dyson series**.
+We recognize the well-known Taylor expansion of $\exp\!(x)$,
leading us to a final expression for $\hat{K}_I$:
$$\begin{aligned}