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About Left: An Arbitrary One-Dimensional Potential V (X) of Range R. Right: The Same Potential With A Regulator Wall Placed at X L
1. Levinson's theorem relates the number of bound states of a potential to the change in phase shift from 0 to infinity energy. It states that the number of bound states is equal to the change in phase shift divided by pi. 2. Resonances occur when a wave packet becomes temporarily trapped in an attractive potential, localized in the region. This can lead to an arbitrarily large positive time delay. 3. A model potential that can produce resonances is one that is infinite for x < 0, -V0 for 0 < x < a, and V1 for x > a, providing an attractive well and positive energy barrier.
Detailed Information
| Author: | ['Sanjid Backer K'] |
|---|---|
| Publication Year: | 2019 |
| Pages: | 10 |
| Language: | English |
| Format: | |
| Price: | FREE |
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