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authorPrefetch2021-11-18 20:07:12 +0100
committerPrefetch2021-11-18 20:07:12 +0100
commitdc3498fd50121eadbdd3ddac5bf950a16e2b50cb (patch)
treeb48f7f76aaaf4993d36eab276f99a3936b49160e /content/know/concept/dyson-equation/index.pdc
parentc0d352dd0f66b47ee91fb96eaf320f895fa78790 (diff)
Expand knowledge base
Diffstat (limited to 'content/know/concept/dyson-equation/index.pdc')
-rw-r--r--content/know/concept/dyson-equation/index.pdc4
1 files changed, 2 insertions, 2 deletions
diff --git a/content/know/concept/dyson-equation/index.pdc b/content/know/concept/dyson-equation/index.pdc
index be93379..25abe11 100644
--- a/content/know/concept/dyson-equation/index.pdc
+++ b/content/know/concept/dyson-equation/index.pdc
@@ -63,8 +63,8 @@ Let us assume that $\hat{H}_0$ is simple,
such that $G_0$ and $\hat{G}{}_0^{-1}$ can be found without issues
by solving the defining equation above.
-Suppose we now perturb this Hamiltonian with
-a possibly time-dependent operator $\hat{H}_1(\vb{r}, t)$,
+Suppose we now add a more complicated and
+possibly time-dependent term $\hat{H}_1(\vb{r}, t)$,
in which case the corresponding fundamental solution
$G(\vb{r}, \vb{r}', t, t')$ satisfies: