Timeline for Derivation of the quadratic form of the Dirac equation
Current License: CC BY-SA 3.0
13 events
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May 16, 2020 at 10:01 | history | edited | Qmechanic♦ |
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May 16, 2020 at 9:39 | answer | added | Cuntista | timeline score: 4 | |
Dec 2, 2013 at 13:21 | history | tweeted | twitter.com/#!/StackPhysics/status/407499735642439680 | ||
Dec 2, 2013 at 11:42 | answer | added | Trimok | timeline score: 4 | |
Dec 2, 2013 at 6:13 | history | edited | jinawee |
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Dec 2, 2013 at 6:12 | comment | added | mikefallopian | so after a bit of algebra I get $\sigma^{\mu\nu} \left( i \hbar \partial_{\nu} - \frac{e}{c} A_{\nu} \right) \left( i \hbar \partial_{\mu} - \frac{e}{c} A_{\mu} \right) = \frac{i \hbar e}{2c} \sigma^{\mu \nu}F_{\mu \nu}$, which leads me to be off by a factor of 2 in the end. Also, the sign of the first term is still wrong... | |
Dec 2, 2013 at 5:54 | comment | added | mikefallopian | Oh of course, I see what you're getting at. $\sigma^{\mu \nu}=-\sigma^{\nu \mu}$, so the diagonal terms of the expansion vanish | |
Dec 2, 2013 at 5:43 | comment | added | joshphysics | Re-examine your "well-certainly..." assertion; recall that $\sigma^{\mu\nu}$ is proportional to the commutator of $\gamma$ matrices. | |
Dec 2, 2013 at 5:38 | comment | added | mikefallopian | Well certainly $\sigma^{\mu\nu}$ should be symmetric but I'm not sure how that helps. Also, I looked more closely at my work and the sign of the $\left(i \hbar \partial - \frac{e}{c} A \right)^2$ term appears to come out to be opposite what I'd expect. | |
Dec 2, 2013 at 5:35 | history | edited | mikefallopian | CC BY-SA 3.0 |
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Dec 2, 2013 at 4:01 | review | First posts | |||
Dec 2, 2013 at 5:18 | |||||
Dec 2, 2013 at 4:00 | comment | added | Zo the Relativist | What do you know about the symmetry of $\sigma^{\mu\nu}$? What does this tell you about which of those terms in your expansion should vanish? | |
Dec 2, 2013 at 3:44 | history | asked | mikefallopian | CC BY-SA 3.0 |