Schur’s lemma and irreducibility
Use invariant kernels and eigenvalues to constrain intertwiners, with a real-field counterexample to the scalar conclusion.
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The question for today
What you’ll understand
- Prove the zero-or-isomorphism conclusion over any field.
- Explain why complex irreducible endomorphisms are scalar.
- Use a commutant calculation as an irreducibility test under semisimplicity.
Intertwining equations can have many unknown entries, but irreducibility makes their solutions remarkably rigid. Schur’s lemma first says that a nonzero map between irreducible representations is an isomorphism. Over the complex numbers, an endomorphism of an irreducible finite-dimensional representation is therefore scalar. These are distinct assertions with different field requirements. Keeping them separate explains both the usefulness of complex characters and the extra structure that appears when an action is studied over the real numbers.
Kernel and image do most of the proof
Let an intertwiner connect two nonzero irreducible representations over the same arbitrary field. Its kernel is invariant in the source and its image is invariant in the target. If the map is nonzero, irreducibility forces the kernel to be zero and the image to be the entire target. Hence the map is an isomorphism. This argument does not require the group to be finite or the characteristic to avoid its order; the conclusion follows directly from invariant subspaces.
For an irreducible representation, every nonzero equivariant endomorphism thus has an inverse, and that inverse is equivariant too. The endomorphism algebra is a division algebra. This does not yet identify it with the field of scalars. Over the complex numbers and in finite dimension, every endomorphism has an eigenvalue. Subtract that eigenvalue times the identity; the resulting intertwiner has nonzero kernel and therefore must vanish. This extra eigenvalue step is where algebraic closure and finite dimensionality enter.
The real rotation counterexample
Consider the real plane with a cyclic generator acting by rotation through 120 degrees. It has no invariant real line, because its rotation matrix has no real eigenvalue. The action is therefore irreducible over the real numbers. Nevertheless rotation through 90 degrees commutes with it and is not a real scalar matrix. The commutant consists of operators behaving like multiplication by complex numbers, demonstrating that the division-algebra conclusion can be stronger than scalar multiplication over the chosen base field.
After complexifying that same plane, the 120-degree rotation has the two distinct cube roots of unity as eigenvalues. The corresponding complex lines are invariant, so the complexified action is reducible. There is no contradiction: irreducibility is always relative to a field. An operator that has no real eigenvalue can acquire eigenvectors after enlarging the scalars. Whenever an irreducibility claim moves between real and complex geometry, test whether scalar extension changes the invariant subspaces before applying the complex form of Schur’s lemma.
When the converse becomes valid
A scalar commutant need not force irreducibility for an arbitrary representation of an arbitrary algebra. In our finite-group complex setting, however, Maschke supplies an invariant complement to every invariant subspace. A proper nonzero invariant subspace would then produce an equivariant projection that is neither zero nor identity and therefore cannot be scalar. Thus a scalar commutant is also an irreducibility criterion here. The logical dependency is important: the converse uses complete reducibility, not only Schur’s lemma.
More generally, if a complex semisimple representation contains inequivalent irreducibles with multiplicities, its commutant is a direct sum of full matrix algebras on the multiplicity spaces. Equivariant maps cannot mix inequivalent irreducibles, while repeated equivalent copies can mix freely. A multiplicity of two contributes four dimensions to the endomorphism algebra, rather than two. This observation anticipates the character norm, which will count precisely the sum of squared multiplicities without requiring an explicit decomposition basis.
Work it through
Add a reflection to remove the extra commutant
Use R and J above together with to represent on . Compute the joint commutant and establish irreducibility over the complex numbers.
The relations , , and hold. Since , commuting with R is equivalent to commuting with J.
Solving gives with complex a and b. But , so requiring TS = ST forces .
The joint commutant is exactly the scalar matrices. Maschke applies to the finite group over the complex numbers, so a proper invariant subspace would have an equivariant nonscalar projection. Its absence proves irreducibility.
The reflection exchanges the rotation eigenlines. Together the two generators act irreducibly even though the rotation alone splits over the complex numbers.
The living notebook
Explore the model
Interactive lab · vectors
A real line cannot survive the nontrivial rotation
Pause and Reset; set both angle degrees and magnitude , predicting the horizontal vector. Reset and set both angle degrees and magnitude , predicting a vector off that line. Repeat at degrees with magnitude . The picture illustrates the absence of a preserved real direction for this rotation. It cannot display complex eigenlines or certify the joint commutant; those require the algebra above. Reset also clears time and both controls.
- x component
- 1.393
- y component
- 0.975
- Magnitude
- 1.7
Playback traces a fixed vector and its projections. Angle and magnitude set the geometry; the moving marker does not change them. Parameter changes pause playback and recompute the model at the current elapsed time. Reset restores both parameters and returns time to zero. Playback starts paused. Adjust either parameter, then choose Play or Step.
Look forA real picture of invariant directions and a complex irreducibility claim answer different questions.
Pause & reason
Check your understanding
Your turn
Try it yourself
Let for over , where the generator acts as . Determine the form and complex dimension of its equivariant endomorphism algebra.
Take a moment to make a prediction or work it out on paper. Open a hint when you need one.
Give me a hint
Commutation preserves the positive and negative eigenspaces, but it imposes no preferred basis inside the repeated positive eigenspace.
Compare with the solution
Every commuting operator has a free two-by-two block on the first two coordinates and a free scalar on the last coordinate, with both off-block rectangles zero. The algebra is , of dimension . The two trivial copies allow arbitrary mixing, which is why counting summands without squaring multiplicities would give the wrong answer.
Keep the idea
Take it with you
- Nonzero intertwiners between irreducibles are isomorphisms over every field.
- The complex scalar conclusion needs finite dimension and an eigenvalue.
- A scalar commutant detects irreducibility here because Maschke supplies complements.
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