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--- classes:2009:fall:phys4101.001:lec_notes_0911 [2009/09/14 19:19] – yk
+++ classes:2009:fall:phys4101.001:lec_notes_0911 [2009/09/23 22:43] (current) – yk
@@ Line 1: / Line 1: @@
-===== Sept 11 (Fri) =====
+===== Sept 11 (Fri) Probability interpretation =====
 ** Responsible party: Schrödinger's Dog**
@@ Line 50: / Line 50: @@
 Then, <math>\lim_{\Delta t\rightarrow 0} \frac{\int_{-\infty}^{\infty} f(x+\Delta x,t+\Delta t) dx - \int_{-\infty}^{\infty} f(x,t) dx}{\Delta t} = \lim_{\Delta t\rightarrow 0} \frac{\int_{-\infty}^{\infty} \frac{\partial f(x,t)}{\partial t}\Delta t dx + \frac{\partial f(x,t)}{\partial x}\Delta x dx}{\Delta t} = \int_{-\infty}^{\infty} \frac{\partial f(x,t)}{\partial t} dx + \Delta x[f(x,t)]_{-\infty}^{\infty}</math>.  Provided that <math>f(x,t)</math> is a normalizable function, the last term should be zero.
+==Schrodinger's Dog==
+Thanks Yuichi, this makes a lot more sense!
 ==End of lecture==
 S.D.: I wasn't really clear on the last proof, but feel that it isn't a important detail. Besides that, the rest of the lecture was great!
+**To go back to the lecture note list, click [[lec_notes]]**\\
+**previous lecture note: [[lec_notes_0909]]**\\
+**next lecture note: [[lec_notes_0914]]**\\