Can Spin Comutation Relations be Simplified by Using Average Spin Values?

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Petar Mali
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[tex][\hat{S}^+_{n},\hat{S}^-_{m}]=2S_n^z\delta_{n,m}[/tex]

where [tex]n,m[/tex] are position vectors of spins. Why if we have

[tex]\langle\hat{S}^z\rangle\approx S[/tex] we can use

[tex][\hat{S}^+_{n},\hat{S}^-_{m}]\approx 2S\delta_{n,m}[/tex]?

where [tex]S[/tex] is value of the spin, for example [tex]\frac{1}{2}[/tex].
 
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Its an approximation. And we know that

[tex] \langle [\hat{S}^+_{n},\hat{S}^-_{m}]\rangle \approx 2S\delta_{n,m}[/tex]
So it does not appear implausible.
 
Yes ok. I don't have problem with

[tex]\langle [\hat{S}^+_{n},\hat{S}^-_{m}]\rangle \approx 2S\delta_{n,m}[/tex]

but where [tex]\langle... \rangle[/tex] disappear?

Why I can use this approximation?

[tex] [\hat{S}^+_{n},\hat{S}^-_{m}]\approx 2S\delta_{n,m}[/tex]
 
If relation [tex] <br /> [\hat{S}^+_{n},\hat{S}^-_{m}]\approx 2S\delta_{n,m}<br /> [/tex]

is correct than

we can define

[tex]\hat{S}^-_n \rightarrow \sqrt{2S}\hat{B}_n^+[/tex]

[tex]\hat{S}^+_n\rightarrow \sqrt{2S}\hat{B}_n[/tex]

which is Bloch approximation but I don't see some reasons for

[tex] <br /> [\hat{S}^+_{n},\hat{S}^-_{m}]\approx 2S\delta_{n,m}<br /> [/tex]
 
Petar Mali said:
Why I can use this approximation?
You can always use whatever approximation you like. The question is whether it is good or bad. This depends on the system you use it for. A point about which you didn't tell us anything.
 
Well I have some magnetic ordered system. For example ferromagnet or antiferromagnet and have some spin hamiltonian. I want to replace operators [tex]\hat{S}^{\pm},\hat{S}^z[/tex] with some functions of Bose operators. Temperatures are low.
 
Well, what you could try is to express the hamiltonian in terms of [tex]\hat{B}_n^+[/tex] and
[tex] \hat{S}^-_n - \sqrt{2S}\hat{B}_n^+[/tex]
considering terms containing the difference as a perturbation. Maybe you can show that they only lead to small corrections in the limit you are considering?