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authorPrefetch2022-01-30 11:27:00 +0100
committerPrefetch2022-01-30 11:27:00 +0100
commit88537b82784f71104c3a2771330c9e492f57fb03 (patch)
tree0d5ddb6adaf9e55892f4e7b79adf1e22cf0aee10 /content/know/concept/kubo-formula/index.pdc
parent8a9fb5fef2a97af3274290e512816e1a4cac0c02 (diff)
Expand knowledge base, remove comments
Diffstat (limited to 'content/know/concept/kubo-formula/index.pdc')
-rw-r--r--content/know/concept/kubo-formula/index.pdc5
1 files changed, 1 insertions, 4 deletions
diff --git a/content/know/concept/kubo-formula/index.pdc b/content/know/concept/kubo-formula/index.pdc
index f5430da..1df4780 100644
--- a/content/know/concept/kubo-formula/index.pdc
+++ b/content/know/concept/kubo-formula/index.pdc
@@ -5,6 +5,7 @@ publishDate: 2021-09-23
categories:
- Physics
- Quantum mechanics
+- Perturbation
date: 2021-09-23T16:21:51+02:00
draft: false
@@ -54,9 +55,6 @@ $$\begin{aligned}
&\approx \bigg( 1 + \frac{i}{\hbar} \int_{t_0}^t \hat{H}_{1,I}(t') \dd{t'} \bigg) \hat{A}_I(t)
\bigg( 1 - \frac{i}{\hbar} \int_{t_0}^t \hat{H}_{1,I}(t') \dd{t'} \bigg)
\\
- %&= \bigg( \hat{A}_I + \frac{i}{\hbar} \int_{t_0}^t \hat{H}_{1,I}(t') \hat{A}_I \dd{t'} \bigg)
- %\bigg( 1 - \frac{i}{\hbar} \int_{t_0}^t \hat{H}_{1,I}(t') \dd{t'} \bigg)
- %\\
&\approx \hat{A}_I(t)
- \frac{i}{\hbar} \int_{t_0}^t \hat{A}_I(t) \hat{H}_{1,I}(t') \dd{t'}
+ \frac{i}{\hbar} \int_{t_0}^t \hat{H}_{1,I}(t') \hat{A}_I(t) \dd{t'}
@@ -102,7 +100,6 @@ describing the response of $\expval*{\hat{A}}$ to first order in $\hat{H}_1$:
$$\begin{aligned}
\boxed{
\delta\expval*{\hat{A}}(t)
- %= - \frac{i}{\hbar} \int_{t_0}^\infty \Theta(t \!-\! t') \expval{\comm{\hat{A}_I(t)}{\hat{H}_{1,I}(t')}}_0 \dd{t'}
= \int_{t_0}^\infty C^R_{A H_1}(t, t') \dd{t'}
}
\end{aligned}$$