Timeline for Spatially localised solution to the Schrödinger equation with potential is a combination of eigenfunctions
Current License: CC BY-SA 4.0
9 events
| when toggle format | what | by | license | comment | |
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| Jul 15 at 18:12 | history | edited | Michael Hardy | CC BY-SA 4.0 |
added 4 characters in body
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| Jul 10 at 23:33 | vote | accept | Earl Jones | ||
| Jun 26 at 4:13 | history | edited | Willie Wong |
edited tags
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| Jun 26 at 4:12 | answer | added | Willie Wong | timeline score: 1 | |
| Jun 25 at 20:57 | comment | added | Dispersion | Additionally, you have your quantifiers wrong I believe. The correct phrasing is that once you fix $\varepsilon$, there exists a compact set $K$ such that your stated inequality holds for all time. | |
| Jun 25 at 20:33 | comment | added | Dispersion | Just a comment to say that usually the $L^2$ norm is referred to as the mass, while the energy is reserved for say the $H^1$ norm. | |
| Jun 25 at 20:06 | history | edited | Earl Jones | CC BY-SA 4.0 |
added 2 characters in body; edited title
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| Jun 25 at 19:57 | history | edited | Daniele Tampieri | CC BY-SA 4.0 |
edited title
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| Jun 25 at 18:29 | history | asked | Earl Jones | CC BY-SA 4.0 |