advanced_tools:fiber_bundles
| Both sides previous revision Previous revision Next revision | Previous revision Next revision Both sides next revision | ||
|
advanced_tools:fiber_bundles [2018/05/03 12:54] 46.229.168.66 ↷ Links adapted because of a move operation |
advanced_tools:fiber_bundles [2018/05/05 12:37] jakobadmin ↷ Links adapted because of a move operation |
||
|---|---|---|---|
| Line 5: | Line 5: | ||
| {{ :advanced_tools:unit-roots-100.gif?nolink|}} | {{ :advanced_tools:unit-roots-100.gif?nolink|}} | ||
| - | Phase factors $e^{i \theta(\vec x,t)}$, like they appear in [[theories:canonical_quantum_mechanics|quantum mechanics]], are just complex numbers with amplitude $1$. Therefore, we can picture them as points on a circle with radius $1$: | + | Phase factors $e^{i \theta(\vec x,t)}$, like they appear in [[theories:quantum_mechanics:canonical|quantum mechanics]], are just complex numbers with amplitude $1$. Therefore, we can picture them as points on a circle with radius $1$: |
| The wave function that describes an electron has a specific phase $\Psi(\vec x,t)= |\Psi(\vec x,t)|e^{i \theta(\vec x,t)}$ at each point $\vec x$ at any given moment $t$. Each such phase $\theta$ can be represented by a dot on the unit circle. | The wave function that describes an electron has a specific phase $\Psi(\vec x,t)= |\Psi(\vec x,t)|e^{i \theta(\vec x,t)}$ at each point $\vec x$ at any given moment $t$. Each such phase $\theta$ can be represented by a dot on the unit circle. | ||
advanced_tools/fiber_bundles.txt · Last modified: 2020/10/28 16:31 by 89.36.76.154
Page Tools
Except where otherwise noted, content on this wiki is licensed under the following license: CC Attribution-Share Alike 4.0 International
