23.3  Simple and Semisimple Algebras

Section 2 found that Mn(F) has no two-sided ideals except the two unavoidable ones: as an algebra it cannot be collapsed. This section is about a second kind of object that is indecomposable — not the algebra, but a space the algebra acts on — and about what happens when a space does break apart. The main theorem says that “every invariant subspace can be split off” and “the space is a sum of unbreakable pieces” are one condition wearing two faces, and that condition is what the rest of the chapter runs on. At the end we check the new vocabulary against the old: an operator is semisimple in Chapter 10’s sense exactly when the algebra it generates acts semisimply.

Throughout, F is any field. Nothing in this section asks it to be algebraically closed or to have a particular characteristic; the hypotheses start biting in the next section. Algebras are associative, unital and finite-dimensional over F, as agreed in Section 1.

23.3.1. Two meanings of the word simple

Section 2 proved that Mn(F) has exactly two two-sided ideals (Theorem 23.2.2), while F[x] — the infinite-dimensional standing exception of Section 1 — has infinitely many. That difference deserves a name.

A simple algebra is one that cannot be collapsed: forming the quotient by an ideal either changes nothing or destroys everything.

Definition 23.3.1 (Simple Algebra)

An F-algebra A is simple if A≠{0} and the only two-sided ideals (Definition 15.10.3) of A are {0} and A itself.

In words: two conditions, and the first is not decoration. The zero algebra has only one ideal, so without the clause A≠{0} it would count as simple and every theorem below would need an exception for it.

Examples.

  • The field itself. A=F is simple: a non-zero ideal contains some c≠0, hence contains c−1c=1, hence everything.
  • Matrix algebras. Mn(F) is simple for every n≥1 (Theorem 23.2.2). This is the example the whole chapter is aimed at.
  • A degenerate case. n=1 recovers M1(F)=F, so the two examples above are one.

Non-example by minimal change. Replace Mn(F) by the algebra A of upper triangular 2×2 matrices over F. It is a subalgebra of M2(F) of dimension 3, with basis E11,E12,E22, and the set N={(0b00):b∈F} is a two-sided ideal of A: it is a subspace, and (ac0d)(0b00)=(0ab00),(0b00)(ac0d)=(0bd00). Since {0}≠N≠A, the algebra A is not simple. The clause that fails is the second one; A≠{0} is fine.

  • Another non-example, the infinite-dimensional one. F[x] has the ideal ⟨x⟩ (Proposition 6.2.1), the polynomials with zero constant term (Example (First Ideals) (b)), which is neither {0} nor F[x].

Why this definition. Section 2 identified ideals with kernels: the kernel of an algebra homomorphism out of A is a two-sided ideal, and conversely every two-sided ideal is the kernel of the map onto the quotient algebra (Definition 23.2.2, Theorem 23.2.5). Simplicity therefore says that A admits no interesting image under a homomorphism, which is the following one-line consequence.

Proposition 23.3.1 (Maps Out of a Simple Algebra)

Let A be a simple F-algebra, let B≠{0} be an F-algebra, and let φ:A→B be an algebra homomorphism (Definition 23.1.2). Then φ is injective.

Proof. Since B≠{0} we have 1B≠0: otherwise y=1By=0 for every y∈B. The kernel of φ is a two-sided ideal of A, and it does not contain 1A, because φ(1A)=1B≠0. So kerφ≠A, and simplicity forces kerφ={0}. A linear map with zero kernel is injective (Theorem 2.2.3).

Section 2 had already seen the case A=Mn(F), which is simple by Theorem 23.2.2: that is Corollary 23.2.3. So a simple algebra has only one image under a homomorphism worth the name: itself. Section 6 will turn this around and recognize the semisimple algebras, over an algebraically closed field, as products of matrix algebras; its Exercise C1 picks out the simple ones among them as the single matrix algebras.

23.3.2. Algebras acting on spaces

An algebra is already a set of operators, by Section 1’s embedding theorem (Theorem 23.1.3). But the same abstract algebra acts on many different spaces — Mn(F) acts on Fn, on itself, on Mn(F) by conjugation — and the differences between those actions are the subject. We need a word for one of them.

Definition 23.3.2 (Representation of an Algebra, and Invariant Subspaces)

Let A be an F-algebra. A representation of A on a finite-dimensional vector space V over F is an algebra homomorphism ρ:A→L(V), so that ρ is linear, ρ(ab)=ρ(a)ρ(b), and ρ(1A)=idV. We then call V an A-space and abbreviate ρ(a)(v) to av. A subspace U⊆V is A-invariant if au∈U for every a∈A and every u∈U.

In words: the multiplication of A is carried to composition of operators, and — the clause that is easy to overlook — the identity of A must act as the identity of V. Two standing examples:

  • The tautological representation. If A⊆L(V) is a subalgebra containing idV (Definition 23.1.1), the inclusion is a representation. This is the case we usually mean when we say “an algebra of operators on V”.
  • The regular representation. A acts on itself by left multiplication: ρ(a)(b)=ab. Associativity gives ρ(ab)=ρ(a)ρ(b), bilinearity gives linearity, and ρ(1A)=idA. Here the A-invariant subspaces are precisely the left ideals of Section 2.

Non-example by minimal change. Take A=F, V=F2, and ρ(c)=0 for every c. This is linear and multiplicative, but ρ(1)=0≠idV, so it is not a representation. The clause that fails is unitality, and it is not a technicality: it is what makes v=1v lie in Av, a step used twice below.

Now the indecomposable actions.

An irreducible A-space is one with nothing inside it for A to see.

Definition 23.3.3 (Irreducible, or Simple, A-space)

An A-space V is irreducible — equivalently, simple — if V≠{0} and the only A-invariant subspaces of V are {0} and V.

Both words are standard and we use them interchangeably. Again two clauses, and again the first is needed: {0} has only one subspace and must be excluded by hand, exactly as the zero algebra was.

Examples.

  • Lines. Any A-space of dimension 1 is irreducible, whatever A is, since its only subspaces are {0} and itself. These are the smallest possible pieces, and Section 4 will show that over an algebraically closed field a commutative algebra has no others.
  • The column space of a matrix algebra. Fn is an irreducible Mn(F)-space. Indeed, let U≠{0} be invariant and pick u∈U with u≠0. Given any w∈Fn, extend u to a basis of Fn (Theorem 1.6.5) and let X be the matrix of the linear map sending u to w and the other basis vectors to 0 (Theorem 2.1.6). Then w=Xu∈U. So U=Fn.

Non-example by minimal change. Shrink M2(F) to the upper triangular algebra A above, still acting on F2. The line Fe1 is A-invariant, because an upper triangular X has Xe1=x11e1. So F2 is not an irreducible A-space; the clause that fails is the second.

Warning. Two different words are both spelled “simple”. An algebra is simple when it has no proper non-zero two-sided ideal; an A-space is simple when it has no proper non-zero invariant subspace. The first does not imply the second. For n≥2 the algebra Mn(F) is simple, yet Mn(F) as a space over itself is not: the matrices whose columns other than the first are zero form a left ideal that is neither {0} nor all of Mn(F), that is, a proper non-zero invariant subspace of the regular representation.

Quick check. Let A⊆M2(F) be the algebra of diagonal matrices and let V=F2. Which subspaces of V are A-invariant? Is V irreducible?

Solution. The invariant subspaces are {0}, Fe1, Fe2 and F2. Each of these four is invariant because diag(d1,d2) fixes each coordinate line. No other line Fv with v=(x,y) is: E11v=(x,0) must be a multiple c(x,y) of v, and if both x≠0 and y≠0 then cy=0 forces c=0 and hence x=0, a contradiction. So V is not irreducible: Fe1 is a proper non-zero invariant subspace.

23.3.3. Splitting a space into pieces

Here is the phenomenon the section is built on. Take V=F2 and the single operator N=J2(0), that is, Ne1=0 and Ne2=e1. The line Fe1 is invariant. Is there an invariant complement? A complement of a line in F2 is a line Fv with v=(x,y) and y≠0, and Nv=(y,0) is a non-zero element of Fe1, which meets Fv only in 0. So Nv∉Fv: there is no invariant complement, and F2 does not break into invariant lines.

Compare D=diag(1,2), where F2=Fe1⊕Fe2 splits perfectly. The difference between these two pictures is the definition we want.

An algebra acts semisimply when every invariant subspace can be split off.

Definition 23.3.4 (Semisimple Action, Semisimple Algebra)

Let A be an F-algebra and V an A-space. We say A acts semisimply on V if every A-invariant subspace U⊆V has an A-invariant complement: a subspace W⊆V with V=U⊕WandW is A-invariant. The algebra A is semisimple if it acts semisimply on itself in the regular representation — that is, if every left ideal of A has a complementary left ideal.

In words: the first notion is a property of an action, the second a property of the algebra alone, obtained by feeding the algebra its own most faithful space. The examples come after the theorem that makes the definition usable.

Warning. Acting semisimply depends on the space, not only on the algebra. The upper triangular algebra A does not act semisimply on F2, as we check below. Yet it does act semisimply on the one-dimensional space F through X↦x11, for the silly reason that a one-dimensional space has no invariant subspace to split off. Always say which space. The unqualified phrase “A is semisimple” is reserved for the regular representation, and a proposition below shows that this is the right choice: a semisimple algebra acts semisimply on every space.

The first thing to know is that the property passes to invariant subspaces. Without this, no induction on dimension gets started.

Lemma 23.3.2 (Splitting Is Inherited by Invariant Subspaces)

Let A act semisimply on a finite-dimensional A-space V, and let W⊆V be A-invariant. Then W, with the action a↦ρ(a)|W, is an A-space, and A acts semisimply on W.

Idea. An invariant subspace U of W is also one of V, so it has an invariant complement U′ in V. That complement is too big; cut it down to U′∩W and check that nothing was lost.

Proof. Since W is A-invariant, ρ(a)|W∈L(W) for every a∈A, and a↦ρ(a)|W is linear, multiplicative and sends 1A to idW; so it is a representation.

Let U⊆W be A-invariant. Then U is an A-invariant subspace of V, so there is an A-invariant U′ with V=U⊕U′. Put W′=U′∩W, which is A-invariant because U′ and W are.

U+W′=W: the inclusion ⊆ holds since U⊆W and W′⊆W. Conversely, let w∈W and write w=u+u′ with u∈U, u′∈U′. Then u′=w−u∈W, because both w and u lie in W; hence u′∈U′∩W=W′ and w∈U+W′.

The sum is direct: U∩W′⊆U∩U′={0}.

Therefore W=U⊕W′ with W′ an A-invariant complement, which is what semisimplicity of the action on W asks for.

Now the theorem. It is the section’s real content, and every later section uses it.

Theorem 23.3.3 (Complete Reducibility)

Let A be an F-algebra and let V be a finite-dimensional A-space. The following are equivalent:

  • (a) A acts semisimply on V;
  • (b) V is a sum of irreducible A-invariant subspaces;
  • (c) V is a direct sum of finitely many irreducible A-invariant subspaces.

Here a sum over the empty family is {0}, so all three hold when V={0}. No hypothesis is placed on F.

Idea. For (a) ⇒ (c), induct on dim⁡V. The smallest non-zero invariant subspace is automatically irreducible: it has no room for a proper one. Split it off using (a), and apply the inductive hypothesis to the complement — which is legitimate precisely because of Lemma 23.3.2. For (b) ⇒ (a), given an invariant U, build a complement greedily out of the given irreducible pieces: add pieces to U as long as the sum stays direct, and then show that a piece left outside would have to meet the sum in {0}, so it could have been added too.

Proof.

  • (a) ⇒ (c). Induction on dim⁡V. If dim⁡V=0 then V is the empty direct sum and there is nothing to prove. Let dim⁡V≥1 and suppose the implication holds for every A-space of smaller dimension.

Among the non-zero A-invariant subspaces of V — there is at least one, namely V — choose W of smallest dimension. Then W is irreducible: it is non-zero, and if U⊆W is A-invariant with U≠{0}, then U is a non-zero A-invariant subspace of V, so dim⁡U≥dim⁡W by the choice of W, and U=W by Theorem 1.6.8.

By (a) there is an A-invariant W′ with V=W⊕W′. By Lemma 23.3.2, W′ is an A-space on which A acts semisimply, and dim⁡W′=dim⁡V−dim⁡W<dim⁡V because dim⁡W≥1. The inductive hypothesis writes W′=W1⊕⋯⊕Wr with each Wi an irreducible A-invariant subspace of W′. Invariance and irreducibility refer only to the action of A, not to the ambient space, so each Wi is an irreducible A-invariant subspace of V as well. Hence V=W⊕W1⊕⋯⊕Wr, a direct sum of finitely many irreducibles.

  • (c) ⇒ (b). A direct sum is in particular a sum.

  • (d) ⇒ (a). Write V=∑i∈IWi with each Wi an irreducible A-invariant subspace, and let U⊆V be A-invariant. Call a finite subset J⊆I good if the sum U+∑j∈JWj is direct. The empty set is good. Every good J satisfies |J|≤dim⁡U+∑j∈Jdim⁡Wj=dim⁡(U⊕⨁j∈JWj)≤dim⁡V, where the first inequality uses dim⁡Wj≥1 and the middle equality is Theorem 1.7.5. So the sizes of good sets are bounded, and we may choose a good J with |J| as large as possible. Put W=∑j∈JWj, an A-invariant subspace, since a sum of A-invariant subspaces is A-invariant. Write S=U⊕W.

Claim: Wi⊆S for every i∈I. Fix i. The subspace Wi∩S is A-invariant and contained in the irreducible Wi, so it is {0} or Wi. Suppose it were {0}. Then i∉J, since j∈J gives Wj⊆S and Wj≠{0}. We show J∪{i} is good, contradicting maximality. Let u+∑j∈Jwj+wi=0,u∈U, wj∈Wj, wi∈Wi. Then wi=−(u+∑jwj)∈Wi∩S={0}, so wi=0; and then u+∑jwj=0 forces u=0 and every wj=0, because J is good (Theorem 1.7.5 (b)). So the sum over J∪{i} is direct, which is the contradiction. Hence Wi∩S=Wi, that is, Wi⊆S.

The claim gives V=∑iWi⊆S, so V=S=U⊕W with W invariant. This proves (a).

Two features of the proof are worth keeping. The complement produced in (b) ⇒ (a) is a sum of some of the given pieces, so nothing new has to be constructed. And the pieces in (c) are far from unique: F2 under the scalar matrices is a direct sum of any two distinct lines.

Example (Upper Triangular Matrices Are Not Semisimple)

Let A⊆M2(F) be the algebra of upper triangular matrices, of dimension 3. Show that A does not act semisimply on F2, and list the irreducible A-subspaces of F2.

Solution. The A-invariant subspaces of F2 are {0}, Fe1 and F2, and no others. Certainly all three are invariant, the middle one because Xe1=x11e1 for upper triangular X. Conversely, let Fv be an invariant line with v=(x,y). Since E12∈A and E12v=(y,0), invariance gives (y,0)=c(x,y) for some c∈F. If y≠0 then cy=0 gives c=0, hence y=0 after all; so y=0 and Fv=Fe1.

Now Fe1 is an invariant subspace with no invariant complement, since a complement of a line in F2 is a line, and Fe1 is the only invariant one. So A does not act semisimply on F2. The only irreducible A-subspace is Fe1; in particular F2 is not a sum of irreducibles, in agreement with Theorem 23.3.3.

For contrast, here is an action that does split, and it is the one Section 6 will build on.

Example (Matrix Algebras Are Semisimple)

Show that A=Mn(F) is a semisimple algebra for every n≥1.

Solution. Section 2 did the work. For j=1,…,n let Cj⊆A be the column ideal: the matrices all of whose columns except the j-th are zero. By Proposition 23.2.4 (d), each Cj is a left ideal and A=C1⊕⋯⊕Cn. Moreover Cj=LW for the one-dimensional space of row vectors W=span(ej⊤), so Cj is a minimal non-zero left ideal by part (c) of the same proposition.

The A-invariant subspaces of the regular representation are the left ideals of A, so “minimal non-zero left ideal” says exactly “irreducible A-subspace”. Hence the regular representation of A is a direct sum of irreducibles, and Theorem 23.3.3 makes A semisimple.

The definition of a semisimple algebra only looked at one space. It controls all of them.

Proposition 23.3.4 (A Semisimple Algebra Has No Other Kind of Representation)

Let A be a semisimple F-algebra and let V be any finite-dimensional A-space. Then A acts semisimply on V.

Idea. Every vector v lies in Av, because 1A acts as the identity; so V is the sum of the subspaces Av. Chop A itself into irreducible left ideals L and show each Lv is either zero or irreducible. Then V is a sum of irreducibles and Theorem 23.3.3 finishes.

Proof. If V={0} there is nothing to prove, so let dim⁡V≥1. Since A is semisimple, Theorem 23.3.3 applied to the regular representation gives A=L1⊕⋯⊕Lk with each Lm an irreducible left ideal.

Claim: for a left ideal L that is irreducible and a vector v∈V, the subspace Lv={av:a∈L} is either {0} or an irreducible A-invariant subspace of V. It is a subspace, being the image of the linear map a↦av restricted to L, and it is A-invariant because b(av)=(ba)v with ba∈L. Suppose Lv≠{0} and let U⊆Lv be A-invariant with U≠{0}. Put L0={a∈L:av∈U}. This is a subspace of L, and it is a left ideal: for b∈A and a∈L0 we have ba∈L and (ba)v=b(av)∈U since U is invariant. As L is irreducible, L0={0} or L0=L. If L0={0}, then every u∈U has the form u=av with a∈L, whence a∈L0={0} and u=0, contradicting U≠{0}. So L0=L, which says Lv⊆U and therefore U=Lv. This proves the claim.

Now let v∈V. Since 1Av=v, we have v∈Av=L1v+⋯+Lkv. Hence V=∑v∈VAv=∑v∈V ∑m=1kLmv, and discarding the summands that are {0} exhibits V as a sum of irreducible A-invariant subspaces. By Theorem 23.3.3, A acts semisimply on V.

23.3.4. How far from semisimple: the radical

The upper triangular algebra failed to act semisimply on F2, and the ideal N was visibly to blame: it is non-zero, yet it squares to zero, so no irreducible space can feel it. That suggests measuring the failure by collecting everything invisible.

We write radA for what follows. Chapter 14 §01 writes rad(β) for the radical of a bilinear form; here the argument is an algebra and the two never meet.

Definition 23.3.5 (Radical of an Algebra)

Let A be an F-algebra. Its radical is radA:=⋂V{a∈A:aV={0}}, where V runs over all irreducible A-spaces and aV={av:v∈V}.

In words: the elements that every irreducible representation sends to 0. The quantifier ranges over a manageable supply: if V is irreducible and v∈V is non-zero, then Av is a non-zero invariant subspace, so V=Av is the image of the linear map a↦av, and dim⁡V≤dim⁡A.

The radical is a two-sided ideal. It is a subspace, being an intersection of kernels of linear maps; and if a∈radA, x,y∈A and V is irreducible, then (xay)v=x(a(yv))=x0=0 for every v∈V. Taking y=1A and x=1A in turn shows xa and ay lie in radA.

The first fact we want is the one the triangular example suggested.

Lemma 23.3.5 (A Nilpotent Ideal Is Invisible)

Let A be an F-algebra and let I⊆A be a two-sided ideal which is nilpotent: for some m≥1, every product a1a2⋯am of m elements of I is 0. Then I⊆radA.

Proof. Let V be an irreducible A-space and write IV=span{av:a∈I, v∈V}, and more generally IkV=span{a1⋯akv:ai∈I, v∈V}.

The subspace IV is A-invariant, since b(av)=(ba)v with ba∈I. By irreducibility, IV={0} or IV=V.

Suppose IV=V. Applying I to both sides, I2V=I(IV)=IV=V, and repeating gives IkV=V for every k≥1. But ImV={0} by nilpotency, so V={0}, contradicting irreducibility.

Hence IV={0}, that is, every a∈I acts as 0 on V. Since V was an arbitrary irreducible A-space, I⊆radA.

And the radical really does obstruct semisimplicity.

Proposition 23.3.6 (A Semisimple Algebra Has Zero Radical)

Let A be a semisimple F-algebra. Then radA={0}.

Proof. By Theorem 23.3.3 applied to the regular representation, A=L1⊕⋯⊕Lk with each Lm an irreducible A-space. Let a∈radA. Then a acts as 0 on each Lm, so aLm={0} for every m, and therefore aA={0}. In particular a=a1A=0.

Remark. The converse is also true for finite-dimensional algebras: radA={0} forces A to be semisimple. We do not prove it, and nothing in this book uses it; whenever semisimplicity is needed later it is established directly, by Maschke’s theorem in Section 7 or by exhibiting a decomposition.

We can now finish the running example.

Quick check. Let A be the algebra of upper triangular 2×2 matrices and N its ideal of strictly upper triangular matrices. Using the two results above, identify radA and decide whether A is a semisimple algebra. Hint: the maps X↦x11 and X↦x22 go from A to F.

Solution. radA=N, and A is not semisimple.

(⊇) We saw that N is a two-sided ideal, and N2={0} because E12E12=0. By Lemma 23.3.5, N⊆radA.

(⊆) For upper triangular X,Y the product has (XY)11=x11y11 and (XY)22=x22y22. So ρ1(X)=x11 and ρ2(X)=x22 are algebra homomorphisms A→F, each sending I2 to 1; they make F an A-space in two ways, irreducible because dim⁡F=1. An element of radA must be killed by both, so it has x11=x22=0 and lies in N.

Since radA=N≠{0}, Proposition 23.3.6 shows A is not a semisimple algebra.

23.3.5. Back to a single operator

Chapter 10 §08 already used the word semisimple, for an operator: T is semisimple when mT is a product of distinct monic irreducible polynomials (Definition 10.8.1). That definition was about a polynomial. This section’s is about invariant subspaces. They agree, and proving so is the best check that the new definition is the right one.

Fix a finite-dimensional V≠{0} over F and T∈L(V), and let F[T]:={p(T):p∈F[x]}⊆L(V), which is a commutative subalgebra of L(V) containing idV (Proposition 23.1.2). A subspace U is F[T]-invariant if and only if it is T-invariant: one direction is the case p=x, and the other holds because TU⊆U gives TkU⊆U for every k, hence p(T)U⊆U for every p.

Theorem 23.3.7 (The Two Meanings of Semisimple Agree)

Let V≠{0} be a finite-dimensional vector space over F and let T∈L(V). The following are equivalent:

  • (a) T is semisimple in the sense of Definition 10.8.1, that is, mT is a product of distinct monic irreducible polynomials;
  • (b) F[T] acts semisimply on V: every T-invariant subspace has a T-invariant complement;
  • (c) V is a sum of irreducible F[T]-invariant subspaces.

No hypothesis is placed on F.

Idea.

  • (b) and (c) are Theorem 23.3.3 for the algebra F[T], so the work is the polynomial statement (a). Forwards: the primary decomposition splits V into pieces on which the minimal polynomial is a single irreducible p, and inside such a piece every non-zero vector generates a cyclic subspace of dimension deg⁡p — which leaves no room for a proper invariant subspace. Backwards: an irreducible piece is cyclic, and a factorization of its minimal polynomial would manufacture a smaller invariant subspace inside it; so each piece contributes one irreducible polynomial, and their product, which is squarefree, kills T.

Proof. By the remark preceding the theorem, “T-invariant” and “F[T]-invariant” are the same condition, so (b) ⇔ (c) is Theorem 23.3.3 applied to A=F[T].

  • (a) ⇒ (c). Write mT=p1⋯pk with p1,…,pk distinct monic irreducibles, so that every exponent in the factorization is 1. By Theorem 9.8.1, V=V1⊕⋯⊕Vk with Vi=kerpi(T) a non-zero T-invariant subspace on which mT|Vi=pi.

Fix i and let v∈Vi with v≠0. Then pi(T)v=0, so the T-annihilator mT,v divides pi (Definition 10.5.2); it is monic of degree at least 1 because v≠0, and pi is irreducible, so mT,v=pi. By Theorem 10.5.2 (a), the cyclic subspace Z(v;T) has dimension deg⁡pi, and it is T-invariant (Proposition 10.5.1).

Z(v;T) is irreducible. Let U⊆Z(v;T) be T-invariant with U≠{0} and pick u∈U with u≠0. Since u∈Vi, the same argument gives mT,u=pi and dim⁡Z(u;T)=deg⁡pi. As Z(u;T)⊆U⊆Z(v;T) and the two ends have equal dimension, Theorem 1.6.8 gives U=Z(v;T).

Every non-zero v∈Vi lies in Z(v;T)⊆Vi, so Vi is a sum of irreducible T-invariant subspaces, and hence so is V=V1+⋯+Vk.

  • (c) ⇒ (a). Write V=∑i∈IWi with each Wi irreducible.

Each mT|Wi is irreducible. Pick w∈Wi with w≠0. Then Z(w;T) is a non-zero T-invariant subspace of Wi, so Z(w;T)=Wi, and Theorem 10.5.2 (a), (c) give q:=mT|Wi=mT,w with deg⁡q=dim⁡Wi≥1. Suppose q were not irreducible. Since deg⁡q≥1, Definition 6.3.1 then gives q=fg with both f and g non-constant, and we may take them monic after dividing each by its leading coefficient. So 1≤deg⁡f<deg⁡q and 1≤deg⁡g<deg⁡q. Put u=g(T)w. Then u≠0: otherwise g(T)w=0 would give mT,w∣g (Definition 10.5.2), impossible since g≠0 has degree less than deg⁡mT,w. Also f(T)u=(fg)(T)w=q(T)w=0, so mT,u∣f and, by Theorem 10.5.2 (a), dim⁡Z(u;T)≤deg⁡f<dim⁡Wi. But Z(u;T) is a non-zero T-invariant subspace of Wi, hence equal to Wi by irreducibility — a contradiction. So no such factorization exists and q is irreducible.

Finitely many pieces suffice. Start with one Wi1; as long as the sum of the chosen pieces is not V, some Wi is not contained in it, and adding that one strictly increases the dimension. The process stops, giving V=Wi1+⋯+Wir.

Conclusion. Let q1,…,qs be the distinct polynomials among mT|Wi1,…,mT|Wir and put q=q1⋯qs, a product of distinct monic irreducibles. For each j, the polynomial mT|Wij divides q, so q(T) vanishes on Wij; as these subspaces span V, q(T)=0 and therefore mT∣q (Theorem 9.5.1). If some irreducible p had p2∣mT, then p2∣q, which contradicts the uniqueness of the factorization of q into irreducibles (Theorem 6.3.5), every exponent there being 1. So no irreducible square divides mT, which is (a).

Two things follow at once. First, the operator case is nothing but the case A=F[T] of Theorem 23.3.3, so Chapter 10’s vocabulary was this chapter’s all along. Second, over an algebraically closed field every irreducible polynomial is linear — a monic polynomial of degree at least 2 has a root λ, hence the non-constant factor x−λ (Theorem 6.1.3) — so “semisimple” there means “a product of distinct linear factors”, which is diagonalizability (Theorem 9.8.2): over such a field, F[T] acts semisimply on V exactly when T is diagonalizable. The shear J2(0) fails on both counts, as it must. Chapter 10 §08 made a finer statement in the same direction, Proposition 10.8.2: in characteristic zero, semisimple means diagonalizable after the field has been enlarged enough to split mT. That proposition needs its characteristic hypothesis; Theorem 23.3.7 does not, because it never leaves F.

23.3.6. Exercises

A. Check your understanding

Exercise (A1)
  • (a) State what it means for an algebra to be simple and what it means for an A-space to be irreducible, and give one object that is the first but whose regular representation is not the second.
  • (b) True or false: if A acts semisimply on V, then every A-invariant subspace of V is irreducible. Justify your answer.
  • (c) Where exactly does the proof of Proposition 23.3.4 use the requirement ρ(1A)=idV built into Definition 23.3.2? And why is the step a=a1A in the proof of Proposition 23.3.6 not an instance of that requirement?
  • (d) Name radA for the algebra A of upper triangular 2×2 matrices, and say which two results identify it.

Solution.

  • (a) A is simple if A≠{0} and its only two-sided ideals are {0} and A (Definition 23.3.1); an A-space V is irreducible if V≠{0} and its only A-invariant subspaces are {0} and V (Definition 23.3.3). For n≥2 the algebra Mn(F) is simple, but its regular representation is not irreducible, since the first column ideal C1 of Example (Matrix Algebras Are Semisimple) is a proper non-zero left ideal.

  • (b) False. Take A=F acting on V=F2 by scalars. Every subspace is invariant and every subspace has a complement, so A acts semisimply; but V itself is an invariant subspace of dimension 2, and it is not irreducible.

  • (c) In the final paragraph, at the words “Since 1Av=v”: that is the requirement ρ(1A)=idV and nothing else, and without it v need not lie in Av, so V need not be the sum of the subspaces Av. The step a=a1A in Proposition 23.3.6 is a different statement: it is axiom (A3) of Definition 14.12.1, which makes 1A a two-sided identity of A itself, and it holds with no representation in sight.

  • (d) radA=N, the strictly upper triangular matrices: the inclusion ⊇ is Lemma 23.3.5 applied to the nilpotent ideal N, and ⊆ comes from the two one-dimensional representations X↦x11 and X↦x22.

B. Practice

Exercise (B1: Which actions split?)

Determine which of the following subalgebras of M2(F), acting on V=F2, act semisimply. Justify your answer in each case, and when the action is semisimple exhibit V as a direct sum of irreducibles.

  • (a) the scalar matrices {cI2:c∈F};
  • (b) the diagonal matrices;
  • (c) F[N]={aI2+bN:a,b∈F}, where N=J2(0);
  • (d) M2(F) itself.

Solution.

  • (a) Semisimple. Every subspace is invariant, and every subspace of a finite-dimensional space has a complement (Theorem 1.7.6). V=Fe1⊕Fe2, and each line is irreducible because it has dimension 1.

  • (b) Semisimple. By the Quick check above, the invariant subspaces are {0}, Fe1, Fe2, F2; the two lines are complements of each other and the two extreme cases are complements of each other. Again V=Fe1⊕Fe2 with both summands irreducible.

  • (c) Not semisimple. The invariant subspaces are the N-invariant ones, and the only invariant line is Fe1: if v=(x,y) with y≠0 then Nv=(y,0) is a non-zero element of Fe1, which is not a multiple of v. So Fe1 has no invariant complement. (Alternatively: mN=x2 is not squarefree, so Theorem 23.3.7 applies.)

  • (d) Semisimple, trivially: V is itself irreducible, as shown after Definition 23.3.3, so V is a one-term direct sum of irreducibles.

Exercise (B2: A two-dimensional algebra)

Let N=J2(0)∈M2(F) and A={aI2+bN:a,b∈F}.

  • (a) Prove that A is a commutative subalgebra of M2(F) of dimension 2.
  • (b) Prove that FN is a two-sided ideal of A and compute radA.
  • (c) Is A a semisimple algebra? Justify your answer.

Solution.

  • (a) A=span(I2,N) is a subspace, and I2,N are independent since N is not a scalar. It contains I2, and (aI2+bN)(a′I2+b′N)=aa′I2+(ab′+a′b)N, using N2=0; the right-hand side lies in A and is symmetric in the two factors, so A is a commutative subalgebra of dimension 2.

  • (b) The displayed product shows (aI2+bN)(cN)=acN∈FN, and A is commutative, so FN is a two-sided ideal; (FN)2={0} since N2=0. By Lemma 23.3.5, FN⊆radA. Conversely φ(aI2+bN)=a is an algebra homomorphism A→F by the same display, and φ(I2)=1, so F is an irreducible A-space; an element of radA must have a=0. Hence radA=FN.

  • (c) No: radA≠{0}, so Proposition 23.3.6 rules it out.

Exercise (B3: Semisimple operators)

For each of the following, decide whether F[T] acts semisimply on V, using Theorem 23.3.7.

  • (a) F=R, V=R2, T the rotation matrix (0−110);
  • (b) F=Q, V=Q3, T=diag(1,1,2);
  • (c) F=Q, V=Q3, T=J3(0);
  • (d) F=R, V=R4, T=C((x2+1)2).

Solution.

  • (a) Yes. mT=x2+1, irreducible over R and occurring once, so T is semisimple. Note that T is not diagonalizable over R; semisimplicity is the weaker condition.

  • (b) Yes. mT=(x−1)(x−2), two distinct irreducibles.

  • (c) No. mT=x3 repeats the irreducible x.

  • (d) No. mT=(x2+1)2 by Theorem 10.5.3, and x2+1 is repeated.

C. Going deeper

Exercise (C1: The diagonal algebra)

Let A⊆Mn(F) be the algebra of all diagonal matrices, acting on V=Fn.

  • (a) Prove that every A-invariant subspace of V is the span of a subset of {e1,…,en}. Hint: consider Eiiv.
  • (b) Deduce that A acts semisimply on V and identify the irreducible A-subspaces.

Solution.

  • (a) Let U be A-invariant and put S={i:ui≠0 for some u∈U}. For u∈U and each i, the matrix Eii is diagonal, so Eiiu=uiei∈U; if i∈S, choosing u with ui≠0 gives ei∈U. Hence span{ei:i∈S}⊆U. Conversely every u∈U is ∑i∈Suiei, since ui=0 for i∉S by the definition of S. So U=span{ei:i∈S}.

  • (b) By (a) the invariant subspaces are indexed by subsets S⊆{1,…,n}, and the complement of span{ei:i∈S} inside V given by the complementary subset is again invariant. So A acts semisimply, and V=Fe1⊕⋯⊕Fen. The irreducible A-subspaces are exactly the coordinate lines Fei: they are irreducible because they have dimension 1, and by (a) no other subspace is both invariant and free of a proper non-zero invariant subspace.

Exercise (C2: The radical is never everything)

Let A≠{0} be a finite-dimensional F-algebra.

  • (a) Prove that A has at least one irreducible A-space. Hint: among the non-zero left ideals, take one of smallest dimension.
  • (b) Prove that every irreducible A-space has dimension at most dim⁡A.
  • (c) Deduce that 1A∉radA, so radA≠A.

Solution.

  • (a) A itself is a non-zero left ideal, so among the non-zero left ideals there is one, L, of smallest dimension. A non-zero left ideal contained in L is a non-zero left ideal of A, hence has dimension at least dim⁡L, hence equals L by Theorem 1.6.8. Since the A-invariant subspaces of the regular representation are the left ideals, L is an irreducible A-space.

  • (b) Let V be irreducible and v∈V non-zero. The set Av is an A-invariant subspace containing v=1Av, so Av=V. It is the image of the linear map A→V, a↦av, so dim⁡V≤dim⁡A by Theorem 2.3.1.

  • (c) Let L be as in (a). Since L≠{0}, pick a∈L with a≠0; then 1Aa=a≠0, so 1A does not act as 0 on L and therefore 1A∉radA. Hence radA≠A. (Note the contrast with Proposition 23.3.6: the radical is always a proper ideal, but it is {0} only in the semisimple case.)

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