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classes:2009:fall:phys4101.001:q_a_1118 [2009/11/18 23:37] – gebrehiwet | classes:2009:fall:phys4101.001:q_a_1118 [2009/11/30 09:00] (current) – x500_bast0052 | ||
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===Esquire (Age of No Ideas)=== | ===Esquire (Age of No Ideas)=== | ||
I have no idea what an eigenspinor physically represents. | I have no idea what an eigenspinor physically represents. | ||
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+ | ==Devlin== | ||
+ | Neither do I. | ||
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===Green Suit 11/17=== | ===Green Suit 11/17=== | ||
This is what I found on Wikipedia: | This is what I found on Wikipedia: | ||
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===David Hilbert' | ===David Hilbert' | ||
Do you mean ψ or χ? | Do you mean ψ or χ? | ||
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+ | ===David Hilbert' | ||
+ | As far as I can tell, a and b are always given or just some constants, so you can use [4.139] as well as the corresponding eigenvalue for whatever operator you're looking at. It is done in example 4.2 in the book for < | ||
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====Schrodinger' | ====Schrodinger' | ||
χ | χ | ||
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====Pluto 4ever 11/18 5:30PM==== | ====Pluto 4ever 11/18 5:30PM==== | ||
Does the value of the quantum number s depend on m, or is it completely independent of the other terms and deals with purely spin alone? | Does the value of the quantum number s depend on m, or is it completely independent of the other terms and deals with purely spin alone? | ||
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+ | ===The Doctor 11/19 12:02AM=== | ||
+ | Equation 4.137 should solve the question. | ||
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+ | I looks like s is a fixed value for a particular particle while m can change depending on the state of that particle. | ||
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+ | ==David Hilbert' | ||
+ | Usually I think of s as being like a constant for each particle; all electrons have spins of 1/2, photons have spin of 1, and so on for every particle. Then when you measure it, spin can be up or down, so the < | ||
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