diff options
author | Prefetch | 2022-02-01 11:23:35 +0100 |
---|---|---|
committer | Prefetch | 2022-02-01 11:23:35 +0100 |
commit | 43c5b696aaf421dec7aee967002999d9145da35e (patch) | |
tree | 418dd75bb385a8922b9484883ae0d42124239c94 /content/know/concept/interaction-picture/index.pdc | |
parent | 88537b82784f71104c3a2771330c9e492f57fb03 (diff) |
Expand knowledge base
Diffstat (limited to 'content/know/concept/interaction-picture/index.pdc')
-rw-r--r-- | content/know/concept/interaction-picture/index.pdc | 3 |
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} |