4.8 • 750 Ratings
🗓️ 7 July 2017
⏱️ 45 minutes
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0:00.0 | Oh, wow, oh, oh, wow, oh, wow, oh, wow. |
0:13.0 | Oh, wow. |
0:15.0 | Oh, my. Hello, you're listening to The Science of Everything podcast episode 84, Advanced Quantum Mechanics Part 2. |
0:40.8 | I'm your host, James Fodor. |
0:42.5 | So this episode follows directly from the previous episode, Advanced Quantum Mechanics, part one, |
0:47.8 | which turned out to be longer than I'd expected, so I've split into two episodes. |
0:52.0 | That's definitely recommended pre-listing for this episode. |
0:55.7 | In this show, what I want to talk about are some more advanced ideas in quantum mechanics, |
1:00.0 | including Noethus theorem, particle statistics, perturbation theory, |
1:04.7 | and a little bit about the EPR paradox. |
1:07.1 | So these are some of the more juicy concepts, |
1:10.1 | which require a little bit of background to sort of understand. |
1:13.6 | Hopefully you'll find this interesting, but do be warned that these are some relatively advanced topics, |
1:18.6 | so it may be heavy-going if you don't already have some background in QM, |
1:22.6 | which is why I recommend the previous episode and also the principles of quantum mechanics episodes |
1:28.3 | that I think episode 14 that I did some time back. Okay so let's get into it. |
1:34.3 | In the previous episode I outlined as best as I could without any visual aids |
1:40.3 | the core ideas of Dirac's Brachette formalism of quantum mechanics, and the basic idea of being |
1:46.4 | able to represent an arbitrary quantum system as a superposition of eigenstates, and each |
1:53.1 | eigenstate corresponding to some measurable observable. |
1:57.7 | Now, I'm not directly going to continue on from that, but I'm going to assume that as sort of background in the discussion that follows, and some of the things I talk about will require more than others. But basically, now I'm going to introduce some key ideas that are pertinent to a more advanced study of quantum mechanics, and that are just interesting in their own light. So the first I'm going to talk about is Nertha's theorem. |
2:20.0 | Now, Nertha was a mathematician who was, well, obviously responsible for NERtha's theorem |
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