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Thanks for your package!
I suggest to add a spin irreducible operator $\hat{S}=\sum_{\sigma\sigma'}f^\dagger_\sigma\vec{\sigma}f_{\sigma'}=(-S^{+}/\sqrt{2},S^{z},S^{-}/\sqrt{2})$ in a spinful fermionic system with U(1) charge and SU(2) spin symmetry. This could be beneficial as we consider magnetic properties in electronic systems.
With Wigner–Eckart theorem, we have
where the quantum number are labeled as $(q_n; S, S_z)$ and $C^{1/2}_{1/2,1}$ is the CG coefficients with dimension $=2\times 3 \times 2.$
The other two equations about $S^{z}$ and $S^{+}$ are equivalent with this one because the reduced matrix element $\langle 0;1/2|S^{0;1}|0;1/2\rangle$ is independent of quantum number $S_z$.
Here, we have $\langle 0,1/2|S^{0;1}|0;1/2\rangle = \sqrt{3}/2$ .
We can construct the spin irreducible operator $\hat{S}$ as
#S operator
P = Vect[fℤ₂ ⊠ SU2Irrep ⊠ U1Irrep]((0,0,-1)=>1, (1,1//2,0)=>1, (0,0,1)=>1)
V = Vect[fℤ₂ ⊠ SU2Irrep ⊠ U1Irrep]((0, 1, 0) =>1)
S =TensorMap(zeros, ComplexF64, P ← P ⊗ V)
blocks(S)[fℤ₂(1) ⊠SU2Irrep(1//2) ⊠U1Irrep(0)].=sqrt(3)/2#S^2 operator@planar S²[-1; -2] := S[-1; 12] * S'[12; -2]
Thank you again for your nice package!
Sincerely yours
Yong-Yue Zong
The text was updated successfully, but these errors were encountered:
Thanks for the suggestion! I am definitely very happy to add this, would you have a suggestion for a good name? In hindsight, naming these functions with a single letter is probably not very future-proof, as S could be many different things...
How about Sₑ$\to\hat{S}$ , Sₑ²$\to\hat{S}^2$ and Sₑ_exchange$\to\hat{S}_i \cdot \hat{S}_j$? Where e has considered the style in MPSKitModels that indicates a spin 1/2 fermionic system and Sₑ can be used to distinguish from the spin operators such as Sˣ, S⁺, S_exchange in spin systems.
Hi Lukas,
Thanks for your package!$\hat{S}=\sum_{\sigma\sigma'}f^\dagger_\sigma\vec{\sigma}f_{\sigma'}=(-S^{+}/\sqrt{2},S^{z},S^{-}/\sqrt{2})$ in a spinful fermionic system with U(1) charge and SU(2) spin symmetry. This could be beneficial as we consider magnetic properties in electronic systems.
I suggest to add a spin irreducible operator
With Wigner–Eckart theorem, we have
where the quantum number are labeled as$(q_n; S, S_z)$ and $C^{1/2}_{1/2,1}$ is the CG coefficients with dimension $=2\times 3 \times 2.$ $S^{z}$ and $S^{+}$ are equivalent with this one because the reduced matrix element $\langle 0;1/2|S^{0;1}|0;1/2\rangle$ is independent of quantum number $S_z$ .$\langle 0,1/2|S^{0;1}|0;1/2\rangle = \sqrt{3}/2$ .
The other two equations about
Here, we have
We can construct the spin irreducible operator$\hat{S}$ as
Thank you again for your nice package!
Sincerely yours
Yong-Yue Zong
The text was updated successfully, but these errors were encountered: