A SO(3) group, Heisenberg Hamiltonian

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The discussion focuses on the commutation relations of matrices representing the SO(3) group, specifically in the context of Heisenberg Hamiltonians. It is clarified that while 2x2, 3x3, and 4x4 matrices can generate SO(3), the 4x4 matrices may also suggest a connection to SO(4). The invariance of the Heisenberg Hamiltonian, which depends on the spin of the system, raises questions about whether it maintains SO(3) symmetry or reflects a broader SO(n) symmetry. The conversation emphasizes that the dimensionality of the group is linked to the number of independent generators and that the specific representation depends on the system's spin. Ultimately, the nature of the group and its representations is determined by the commutation relations and the dimensionality of the matrices involved.
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We have commutation relation ##[J_j,J_k]=i \epsilon_{jkl}J_l## satisfied for ##2x2##, ##3x3##, ##4x4## matrices. Are in all dimensions these matrices generate ##SO(3)## group? I am confused because I think that maybe for ##4x4## matrices they will generate ##SO(4)## group. For instance for Heisenberg Hamiltonian
H=-\frac{J}{2}\sum_{n,m}\vec{S}_n \cdot \vec{S}_m depending on spin of the sistem is this Hamiltonian always ##SO(3)## invariant or no? Or it is SO(n) symmetry in general?
 
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They together close to form the Lie algebra of the SO(3) group. But SO(3) (and so(3) the Lie algebra) can have various dimensional representations. So yes, it depends on the "spin of the system" which is another way of specifying which irreducible representation of SO(3) (or rather its corresponding spin group) you're considering.

Note: The dimension of the group is number of independent parameters which equates to the number of (linearly) independent generators. Hence here the general group element is: ##G(\Theta) =\exp( i\theta^k J_k)##. The group here is 3 dimensional... but which 3-dim group? That's what the commutator relations determine. Then what dimensional matrices these generators are describes the dimension of the representation.

[Edit] Let me add, for SO(n) the n is the dimension of the fundamental representation, namely the spin 1 or vector representation.
 
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