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visualize what chirality physically means |
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| Sep15-07, 03:34 PM | #1 |
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visualize what chirality physically means
My difficultly is in trying to visualize what chirality physically means. In solid state system, people usually ascribed electron of one chirality to be electron in the conduction band while the opposite chirality belongs to an unoccupied state (hole) in the valence band. Can I then say the electron is left handed, while the hole is right handed. Electron spins clockwise while hole spins anti-clockwise. Is this correct?
Is there an example that describe how electron with different chirality can interacts? Is the electron hole interaction forming an exciton an example of this? |
| Sep15-07, 09:04 PM | #2 |
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I think it's necessary to note that my response in http://www.physicsforums.com/showthread.php?t=184042 was for high energy particle physics, not for solid state physics. My knowledge about solid state physics is very limited. I see no reason why and how the chirality I described in my other post (being eigenstates of the projection operators mentioned) would fit to what you seem to say here. It might be (and even seems to me that way) that the term chirality has a different meaning in solid state physics.
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| Sep17-07, 04:35 AM | #3 |
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Zz. |
| Sep17-07, 07:59 PM | #4 |
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visualize what chirality physically means |
| Sep17-07, 08:03 PM | #5 |
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Recognitions:
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I vaguely recall that the "spinor" components are actually with respect to the sublattices in graphene and that the chirality conservation has something to do with the fact that electrons want to stay on the same sublattice they started on...
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| Sep17-07, 08:21 PM | #6 |
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Recognitions:
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| Sep18-07, 05:49 AM | #7 |
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Zz. |
| Sep18-07, 05:52 AM | #8 |
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If we are doing to discuss some exotic property of material science, then I can do that as well. But there's no such thing in the OP. "Chirality in the conduction band" is meaningless until something is defined here. Where exactly is chirality involved in the derivation of the conduction band. That's what I want to know. One may start with the ideal metal if one wish. Zz. |
| Sep18-07, 10:18 AM | #9 |
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| Sep18-07, 10:38 AM | #10 |
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Graphene isn't a "band" material. Very much like Mott-Hubbard insulator, you can't describe graphene using a typical band model, especially when you can have 2D structure that can behave both like a conductor and semiconductor at the same time. This is not the behavior of ordinary material, and certainly not the the typical conduction band what we know. Zz. |
| Sep18-07, 11:49 AM | #11 |
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| Sep18-07, 12:21 PM | #12 |
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Ultrathin graphite, for example, has a rather unusual electronic transport property, such as the anomolous quantum hall effect, something you do not get with a typical semiconductor or metal. This has been used often as the typical sign for non-standard electronic structure. This is despite the fact that you do get Dirac fermions in the vicinity of of the Fermi energy. Zz. |
| Sep18-07, 01:32 PM | #13 |
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But let me drop you another question which might help the discussion. In semiconductor like Si, how does one treat electron and hole in a single Hamiltonian picture? For example in the case of exciton, where electron and hole couples, I will need a Hamiltonian description that includes an electron and hole state. Lets consider a simple effective mass picture. Wouldn't this results in a Hamiltonian matrix like Dirac eqaution with postivie and negative sea of electrons? |
| Sep18-07, 01:40 PM | #14 |
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Zz. |
| Sep18-07, 01:42 PM | #15 |
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quantized---
did you happen to glance at the Wikipedia chirality article? http://en.wikipedia.org/wiki/Chirality_%28physics%29 it is clear and simple AFAICS, though perhaps it wouldn't be responsive to your question (someone else may wish to comment---Wik not always reliable.) |
| Sep18-07, 02:07 PM | #16 |
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| Sep18-07, 02:11 PM | #17 |
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