Su(2), so(3) and their representations

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SUMMARY

The discussion centers on the relationship between the representations of the special orthogonal group SO(3) and the special unitary group SU(2). It is established that every representation of SO(3) can be derived from a representation of SU(2) through a group homomorphism R:SU(2)→SO(3). The matrices corresponding to the j=1 representation of both groups are not identical due to the nature of the groups, but they are related through the Lie algebras su(2) and so(3). The mapping R is a linear isometry that connects the complex 2×2 hermitian matrices to the 3-dimensional vector space over the reals, confirming the structural relationship between these groups.

PREREQUISITES
  • Understanding of group theory, specifically Lie groups and Lie algebras.
  • Familiarity with representations of groups, particularly SU(2) and SO(3).
  • Knowledge of complex matrices and hermitian forms.
  • Basic concepts of linear algebra, including isometries and vector spaces.
NEXT STEPS
  • Study the properties of Lie groups and their representations, focusing on SU(2) and SO(3).
  • Explore the concept of group homomorphisms and their implications in representation theory.
  • Investigate the role of Pauli spin matrices in quantum mechanics and their connection to SU(2).
  • Learn about the double cover properties of groups, particularly in the context of SL(4,C) and SO(6,C).
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This discussion is beneficial for mathematicians, physicists, and students specializing in theoretical physics, particularly those interested in quantum mechanics, representation theory, and the mathematical foundations of symmetry in physics.

Lapidus
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I try to understand the statement "Every representation of SO(3) is also a representation of SU(2)".

Does that mean that all the matrices of an integer-spin rep of SU(2) are identical to the matrices of the corresponding spin rep of SO(3)?

Say, the j=1 rep of SU(2) has three 3x3 matrices, so has the j=1 rep of SO(3). Are the matrices for SU(2) identical to those for SO(3)? But their are different groups, so that can't be right.

Or are the matrices identical only for the Lie algebras su(2), so(3)? THANK YOU
 
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There's a group homomorphism ##R:SU(2)\to SO(3)##. So if ##\Pi:SO(3)\to GL(V)## is a representation of ##SO(3)##, then ##\Pi\circ R## is a representation of ##SU(2)##.

The map ##R## isn't an isomorphism. It fails to be injective, but has the property that ##R(-\lambda)=R(\lambda)## for all ##\lambda\in SU(2)##.

This is a sketch of how to find the map ##R##:

Every complex 2×2 hermitian matrix ##x## can be written in the form
$$x=\begin{pmatrix}x_3 & x_1-ix_2\\ x_1+ix_2 & -x_3\end{pmatrix} =\sum_{i=1}^3 x_i \sigma_3.$$ The ##\sigma_i## are the Pauli spin matrices. The set ##H## of all such matrices is a 3-dimensional vector space over ##\mathbb R## (not ##\mathbb C##). We can define an inner product on ##H## by ##\langle x,y\rangle=\operatorname{Tr}(x^*y)## for all ##x,y\in H##. The map ##x\mapsto(x_1,x_2,x_3)## is an isometric isomorphism from ##H## to ##\mathbb R^3##.

For all ##\lambda\in SU(2)##, the map ##R_\lambda : H\to H## defined by ##R_\lambda(x)=\lambda x\lambda^*## for all ##x\in H##, is a linear isometry. (If you want to prove this, note that ##\det x=-(x_3)^2-(x_1)^2-(x_2)^2##). Since ##H## is isometrically isomorphic to ##\mathbb R^3##, this means that we can identify ##R_\lambda## with an element of ##SO(3)##. It's easy to show that the map ##\lambda\mapsto R_\lambda## is a homomorphism. This is the map I'm denoting by ##R##.
 
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I am not too familiar with this subject, but I think you can imagine of this map roughly, i.e. topologically, by noting that elements of SU(2), being complex invertible transformations of complex 2 space, induce an isomorphism of the set of complex lines through the origin, i.e. an isomorphism of the projective line to itself. But this projective complex "line" is homeomorphic to the 2-sphere (it equals the complex numbers plus a point at infinity). This much is true for all elements of GL(2,C), but the ones in SU(2) also preserve the usual metric on the sphere.

There seems to be another analogue, but more complicated, taking SL(4,C) onto SO(6,C). This is defined by choosing a skew symmetric form on complex 4 space, which, in every basis, determines a skew 4x4 matrix. Changing bases, i.e. acting by GL(4,C), transforms these matrices into each other, i.e. defines an action on the 6 dimensional space of such matrices. Those basis changes coming from SL(4,C) and not just GL(4,C) preserve the "Pfaffian" (square root of the determinant) of the skew matrix, hence preserve the rank 6 quadric defined by that determinant in 6 space, and this seems to make its action belong to SO(6,C).

I think both these maps are double covers, i.e. 2:1 onto.
 
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