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| author | Prefetch | 2021-09-22 15:33:15 +0200 |
|---|---|---|
| committer | Prefetch | 2021-09-22 15:33:15 +0200 |
| commit | bb79f9b1beee85f2290f3bed9b62eacaca445602 (patch) | |
| tree | f0bde207897aa6514d91371baa92b9e00c727cb1 /content/know/concept/time-dependent-perturbation-theory/index.pdc | |
| parent | 42d409fa774efb8206ae5c701d5cbcc4ae1d9cad (diff) | |
Expand knowledge base
Diffstat (limited to 'content/know/concept/time-dependent-perturbation-theory/index.pdc')
| -rw-r--r-- | content/know/concept/time-dependent-perturbation-theory/index.pdc | 5 |
1 files changed, 4 insertions, 1 deletions
diff --git a/content/know/concept/time-dependent-perturbation-theory/index.pdc b/content/know/concept/time-dependent-perturbation-theory/index.pdc index b16e3ee..1fbd9ce 100644 --- a/content/know/concept/time-dependent-perturbation-theory/index.pdc +++ b/content/know/concept/time-dependent-perturbation-theory/index.pdc @@ -181,7 +181,10 @@ which can cause confusion when comparing literature. In any case, the probability oscillates as a function of $t$ with period $T = 2 \pi / (\omega_{ma} \!-\! \omega)$, -so after one period the particle is certain to be back in $\ket{a}$. +so after one period the particle is back in $\ket{a}$, +and after $T/2$ the particle is in $\ket{b}$. +See [Rabi oscillation](/know/concept/rabi-oscillation/) +for a more accurate treatment of this "flopping" behaviour. However, when regarded as a function of $\omega$, the probability takes the form of |