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Do the Creation Operator and Spin Projection Operator Commute? |
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| Dec20-12, 04:04 AM | #1 |
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Do the Creation Operator and Spin Projection Operator Commute?
I have bumped into a term
[itex]a^\dagger \hat{O}_S | \psi \rangle[/itex] I would really like to operate on the slater determinant [itex]\psi[/itex] directly, but I fear I cannot. Is there any easy manipulation I can perform? |
| Dec21-12, 01:05 AM | #2 |
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where you got that and is that O something expressible in terms of gamma matrices?
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| Dec21-12, 03:16 AM | #3 |
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What is a spin projection operator? The things that come to mind are single body operators, and you have a many body wavefunction. If it's something like the total Z component of the spin, then as a many body operator it would be written as \sum_i (n_up - n_down), which is a combination of creation/annihilation operators ... take your operator and express it in terms of particle creation/annihilation operators and then you can work out the commutation relation.
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| Dec21-12, 04:14 AM | #4 |
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Recognitions:
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Do the Creation Operator and Spin Projection Operator Commute?
Spin projection operators are used e.g. in quantum chemistry. A single Slater determinant is in general not an eigenstate of spin, but such an eigenstate can be obtained using a projection operator.
If ##a^\dagger## adds an electron in a spin orbital, the new state will in general be a combination of states with with new spin S-1/2 and S+1/2. In general you can write the spin projected state as a sum of determinants again and then act with ##a^\dagger## on each of it. |
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