diff options
Diffstat (limited to 'source/know/concept/heisenberg-picture')
| -rw-r--r-- | source/know/concept/heisenberg-picture/index.md | 3 |
1 files changed, 1 insertions, 2 deletions
diff --git a/source/know/concept/heisenberg-picture/index.md b/source/know/concept/heisenberg-picture/index.md index 54bf397..3ffe29a 100644 --- a/source/know/concept/heisenberg-picture/index.md +++ b/source/know/concept/heisenberg-picture/index.md @@ -118,7 +118,7 @@ This result is arguably more intuitive than the Schrödinger picture, because it allows us to think about observables (i.e. operators) in a more classical way. For example, inserting the position $$\hat{X}$$ and momentum $$\hat{P} = - i \hbar \: \idv{}{\hat{X}}$$ -gives the following Newton-style relations: +gives the following Newton-style relations (details omitted): $$\begin{aligned} \dv{\hat{X}}{t} @@ -130,7 +130,6 @@ $$\begin{aligned} = - \dv{V(\hat{X})}{\hat{X}} \end{aligned}$$ -Where the commutators have been treated as known. These equations would not be valid in the Schrödinger picture, unless we took their expectation value to get [Ehrenfest's theorem](/know/concept/ehrenfests-theorem/). |