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| author | Prefetch | 2021-11-12 20:20:05 +0100 |
|---|---|---|
| committer | Prefetch | 2021-11-12 20:20:05 +0100 |
| commit | f2970c55894b3c8d5fd2926a8918d166988109fe (patch) | |
| tree | be07d30a501b84cc3e6a80f70c6f5a729f6b28dc /content/know/concept/interaction-picture | |
| parent | 2a91bdedf299a7fa7b513785d51a63e2f147f37f (diff) | |
Expand knowledge base
Diffstat (limited to 'content/know/concept/interaction-picture')
| -rw-r--r-- | content/know/concept/interaction-picture/index.pdc | 6 |
1 files changed, 4 insertions, 2 deletions
diff --git a/content/know/concept/interaction-picture/index.pdc b/content/know/concept/interaction-picture/index.pdc index 1ce330d..45950ff 100644 --- a/content/know/concept/interaction-picture/index.pdc +++ b/content/know/concept/interaction-picture/index.pdc @@ -40,8 +40,10 @@ With $\hat{H}_S(t)$ the full Schrödinger Hamiltonian. We define the unitary conversion operator: $$\begin{aligned} - \hat{U}(t) - \equiv \exp\!\Big( i \frac{\hat{H}_{0,S} t}{\hbar} \Big) + \boxed{ + \hat{U}(t) + \equiv \exp\!\bigg( i \frac{\hat{H}_{0,S} t}{\hbar} \bigg) + } \end{aligned}$$ The interaction-picture states $\ket{\psi_I(t)}$ and operators $\hat{L}_I(t)$ |