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Definitions and Schurs Lemma

In this section we will use the idea of invariant subspaces of a representation (see Definition 5.1) to define irreducible representations. Then we will prove Schur s lemma, which tells us that irreducible representations are indeed good building blocks. [Pg.180]

For some representations, the largest and smallest subspaces are the only invariant ones. Consider, for example, the natural representation of the group G = 50(3) on the three-dimensional vector space C . Suppose W is an invariant subspace with at least one nonzero element. We will show that W = C-. In other words, we will show that only itself (all) and the trivial subspace 0 (nothing) are invariant subspaces of this representation. It will suffice to show that the vector (1, 0, 0) lies in W, since W would then have to contain both [Pg.180]

To show that (1, 0, 0) lies in W, consider any nonzero vector w e W. Note that w e C, and it might not be pure real or pure imaginary. Define [Pg.180]

So if V = 0 then, by the argument above, we have W =. Onthe other hand, if V 7 0, then again by Exercise 4.11 we can choose a rotation M e SO(3) such that Mv = (ryOyOy for some nonzero real number r. Thus the invariant subspace VT contains the vector Mw = a + b, cY for some real numbers a, b and c. It follows that the subspace W also contains the vector [Pg.181]

Note that because r is nonzero, so is 2a + 2ir. So in this case as well we have (1, 0, 0) e VE and hence, as argued above, W — C. This shows that the only nonzero invariant subspace of the representation is the whole space [Pg.181]




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Schurs Lemma

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