Timeline for How is Green function in many-body theory introduced?
Current License: CC BY-SA 3.0
8 events
| when toggle format | what | by | license | comment | |
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| Nov 20, 2015 at 11:57 | comment | added | jarm | It seems to me that there is a minus sign mistake, as you have $it(\epsilon - \omega -H)$ in the exponential, and then this becomes $\omega + \epsilon - H$ in the delta function. | |
| S Jul 11, 2015 at 14:48 | history | suggested | Minethlos | CC BY-SA 3.0 |
corrected some typos
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| Jul 11, 2015 at 14:13 | review | Suggested edits | |||
| S Jul 11, 2015 at 14:48 | |||||
| Jun 9, 2015 at 17:13 | vote | accept | Minethlos | ||
| Jun 9, 2015 at 16:02 | comment | added | dolun | See edit $\uparrow$ for more precision. | |
| Jun 9, 2015 at 16:01 | history | edited | dolun | CC BY-SA 3.0 |
+precisions
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| Jun 9, 2015 at 14:40 | comment | added | Minethlos | Thank you for the thorough answer. I understood everything except the second formula. Can you explain why this $\Psi$ is truly a solution of the Schrödinger equation? | |
| Jun 9, 2015 at 10:09 | history | answered | dolun | CC BY-SA 3.0 |