Mathematics · Book 3 · Bachelor Year 1

University Mathematics — Year 1

University Mathematics — Year 1 · Bachelor Year 1

20Linear Maps

The maps worth studying between vector spaces are those compatible with the structure: linear maps. Their two fundamental subspaces — kernel and image — measure injectivity and surjectivity, and in finite dimension the rank–nullity theorem binds their sizes into one conservation law. Projections and symmetries, then linear forms and hyperplanes, close the chapter.

20.1 Definitions and first properties

Definition 20.1

Let E,FE, F be KK-vector spaces. A map u ⁣:E→Fu \colon E \to F is linear when

∀x,y∈E, ∀λ∈K,u(x+λy)=u(x)+λu(y).\forall x, y \in E,\ \forall \lambda \in K, \qquad u(x + \lambda y) = u(x) + \lambda u(y).

Then u(0)=0u(0) = 0 and u(∑λixi)=∑λiu(xi)u(\sum \lambda_i x_i) = \sum \lambda_i u(x_i). The set L(E,F)\mathcal{L}(E, F) of linear maps is itself a vector space; composition of linear maps is linear, and bilinear in the pair. An endomorphism is a linear E→EE \to E; an isomorphism is a bijective linear map (its inverse is then automatically linear); u−1u^{-1} of an isomorphism, compositions of isomorphisms, are isomorphisms.

Proof that the inverse is linear. Let uu be linear bijective, y,y′∈Fy, y' \in F and λ∈K\lambda \in K. Put x=u−1(y)x = u^{-1}(y) and x′=u−1(y′)x' = u^{-1}(y'). Then

u(x+λx′)=u(x)+λu(x′)=y+λy′,u\bigl(x + \lambda x'\bigr) = u(x) + \lambda u(x') = y + \lambda y' ,

and applying u−1u^{-1} to both ends: u−1(y+λy′)=x+λx′=u−1(y)+λ u−1(y′)u^{-1}(y + \lambda y') = x + \lambda x' = u^{-1}(y) + \lambda\,u^{-1}(y'). Nothing about u−1u^{-1} was computed: linearity transports through the defining property of uu alone — a pattern worth remembering, as structure often rides along bijections for free. ∎

Proposition 20.2 (A linear map is known on a basis)

Let (e1,…,en)(e_1, \dots, e_n) be a basis of EE and (v1,…,vn)(v_1, \dots, v_n) arbitrary vectors of FF. There is exactly one linear map u ⁣:E→Fu \colon E \to F with u(ei)=viu(e_i) = v_i for all ii. Moreover:

u injective  ⟺  (vi) free;u surjective  ⟺  (vi) generates F.u \text{ injective} \iff (v_i) \text{ free}; \qquad u \text{ surjective} \iff (v_i) \text{ generates } F .

Proof. Existence/uniqueness: every xx has unique coordinates x=∑λieix = \sum \lambda_i e_i (Proposition 18.15); linearity forces u(x)=∑λiviu(x) = \sum \lambda_i v_i, and this formula does define a linear map.

Injectivity: by Proposition 20.5 below, uu is injective iff its kernel is trivial. Now u(∑λiei)=0u\bigl(\sum\lambda_i e_i\bigr) = 0 means exactly ∑λivi=0\sum\lambda_i v_i = 0. If (vi)(v_i) is free, this forces every λi=0\lambda_i = 0, i.e. the kernel reduces to 00: injective. If (vi)(v_i) is linked, a nontrivial relation ∑λivi=0\sum\lambda_i v_i = 0 produces the nonzero vector ∑λiei\sum\lambda_i e_i in the kernel ((ei)(e_i) is free): not injective. The two conditions match term for term.

Surjectivity: the image of uu is the set of all ∑λivi\sum\lambda_i v_i, i.e. exactly Vect⁡(v1,…,vn)\operatorname{Vect}(v_1, \dots, v_n), which equals FF iff the family generates. ∎

Definition 20.3 (Kernel and image)

For u∈L(E,F)u \in \mathcal{L}(E, F):

ker⁡u={x∈E:u(x)=0}⊆E,im⁡u=u(E)⊆F,\ker u = \{x \in E : u(x) = 0\} \subseteq E, \qquad \operatorname{im} u = u(E) \subseteq F ,

both subspaces (direct verification with the criterion).

Method 20.4 (Kernel and image, in practice)

Kernel: write u(x)=0u(x) = 0 as a system on the coordinates (or coefficients) of xx, solve, and parametrize — the kernel comes out with a basis attached (Method 19.10). Image: it is the span of the images of any generating family of EE — usually a basis, so im⁡u=Vect⁡(u(e1),…,u(en))\operatorname{im} u = \operatorname{Vect}\bigl(u(e_1), \dots, u(e_n)\bigr); then eliminate redundant images to extract a basis. Shortcut: compute whichever of the two is easier and get the other’s dimension for free by rank–nullity (Theorem 20.7); when a plausible candidate subspace for the image is known, comparing dimensions upgrades the easy inclusion to equality (Theorem 19.14). Both shortcuts are used in Example 20.11 below.

Proposition 20.5

uu is injective   ⟺  \iff ker⁡u={0}\ker u = \{0\}; uu is surjective   ⟺  \iff im⁡u=F\operatorname{im} u = F.

Proof. As for groups (Proposition 7.11): u(x)=u(y)  ⟺  u(x−y)=0  ⟺  x−y∈ker⁡uu(x) = u(y) \iff u(x - y) = 0 \iff x - y \in \ker u. The second point is the definition. ∎

20.2 The rank–nullity theorem

Definition 20.6

The rank of u∈L(E,F)u \in \mathcal{L}(E, F) (with EE finite-dimensional) is rk⁡u=dim⁡im⁡u\operatorname{rk} u = \dim \operatorname{im} u — also the rank of the family (u(e1),…,u(en))\bigl(u(e_1), \dots, u(e_n)\bigr) for any basis (ei)(e_i) of EE.

Theorem 20.7 (Rank–nullity)

Let EE be finite-dimensional and u∈L(E,F)u \in \mathcal{L}(E, F). Then

dim⁡E=dim⁡ker⁡u+rk⁡u.\dim E = \dim \ker u + \operatorname{rk} u .

More precisely, if SS is any supplementary subspace of ker⁡u\ker u in EE, then uu restricts to an isomorphism from SS onto im⁡u\operatorname{im} u.

Proof. Let SS satisfy E=ker⁡u⊕SE = \ker u \oplus S (Theorem 19.14), and let v ⁣:S→im⁡uv \colon S \to \operatorname{im} u be the restriction of uu.

vv is injective: ker⁡v=S∩ker⁡u={0}\ker v = S \cap \ker u = \{0\}.

vv is surjective: any u(x)u(x) with x=k+sx = k + s (k∈ker⁡uk \in \ker u, s∈Ss \in S) equals u(s)=v(s)u(s) = v(s).

So vv is an isomorphism; an isomorphism sends a basis to a basis (Proposition 20.2), so dim⁡S=dim⁡im⁡u\dim S = \dim\operatorname{im} u, and dim⁡E=dim⁡ker⁡u+dim⁡S\dim E = \dim\ker u + \dim S concludes. ∎

Example 20.8 (Building a map to specification)

Construct u∈L(R3)u \in \mathcal{L}(\R^3) with ker⁡u=Vect⁡(1,1,1)\ker u = \operatorname{Vect}(1,1,1) and im⁡u={z=0}\operatorname{im} u = \{z = 0\}. Sanity first: rank–nullity demands 1+2=31 + 2 = 3 — consistent, so a solution may exist. Choose a basis adapted to the kernel, say ((1,1,1), e1, e2)\bigl((1,1,1),\ e_1,\ e_2\bigr) (Example 19.7), and prescribe images (Proposition 20.2):

u(1,1,1)=0,u(e1)=e1,u(e2)=e2.u(1,1,1) = 0, \qquad u(e_1) = e_1, \qquad u(e_2) = e_2 .

Then ker⁡u⊇Vect⁡(1,1,1)\ker u \supseteq \operatorname{Vect}(1,1,1) and im⁡u=Vect⁡(e1,e2)={z=0}\operatorname{im} u = \operatorname{Vect}(e_1, e_2) = \{z = 0\}; rank–nullity forces dim⁡ker⁡u=1\dim\ker u = 1, so the kernel is exactly the prescribed line. Explicitly, decomposing (x,y,z)=z(1,1,1)+(x−z)e1+(y−z)e2(x, y, z) = z(1,1,1) + (x - z)e_1 + (y - z)e_2:

u(x,y,z)=(x−z, y−z, 0).u(x, y, z) = (x - z,\ y - z,\ 0).

The recipe generalizes: a linear map with prescribed kernel NN and image II exists exactly when dim⁡N+dim⁡I=dim⁡E\dim N + \dim I = \dim E — necessity is rank–nullity, sufficiency is this construction.

Corollary 20.9

If dim⁡E=dim⁡F\dim E = \dim F (finite), then for u∈L(E,F)u \in \mathcal{L}(E, F):

u injective  ⟺  u surjective  ⟺  u bijective.u \text{ injective} \iff u \text{ surjective} \iff u \text{ bijective}.

In particular this holds for endomorphisms in finite dimension. (It fails in infinite dimension: on K[X]K[X], the derivative is surjective but not injective, and P↦XPP \mapsto XP is injective but not surjective.)

Proof. Injective   ⟺  dim⁡ker⁡u=0  ⟺  rk⁡u=dim⁡E=dim⁡F  ⟺  im⁡u=F\iff \dim\ker u = 0 \iff \operatorname{rk} u = \dim E = \dim F \iff \operatorname{im} u = F (a subspace of full dimension is everything, Theorem 19.14)   ⟺  \iff surjective. ∎

Example 20.10 (Interpolation, structurally)

Fix distinct x0,…,xnx_0, \dots, x_n and let u ⁣:Rn[X]→Rn+1u \colon \R_n[X] \to \R^{n+1}, P↦(P(x0),…,P(xn))P \mapsto (P(x_0), \dots, P(x_n)): linear. Its kernel is {P:deg⁡P≤n, n+1 roots}={0}\{P : \deg P \leq n,\ n+1 \text{ roots}\} = \{0\} (Corollary 8.8). Equal dimensions n+1n + 1: uu is an isomorphism — existence and uniqueness of the Lagrange interpolant (Theorem 8.23) in one line.

The same one-line pattern handles data mixing values and derivatives: v ⁣:R3[X]→R4v \colon \R_3[X] \to \R^4, P↦(P(0),P′(0),P(1),P′(1))P \mapsto \bigl(P(0), P'(0), P(1), P'(1)\bigr) is linear, and its kernel consists of degree-≤3\leq 3 polynomials with double roots at 00 and 11, i.e. divisible by X2(X−1)2X^2(X-1)^2 of degree 44: only P=0P = 0. Equal dimensions again: every quadruple of data (P(0),P′(0),P(1),P′(1))(P(0), P'(0), P(1), P'(1)) is realized by exactly one cubic — Hermite interpolation, granted by a kernel computation before any formula is written (the weekend problem of Chapter 22 meets its determinant).

Example 20.11 (Rank–nullity at work: the difference operator)

Let Δ ⁣:Rn[X]→Rn[X]\Delta \colon \R_n[X] \to \R_n[X], P↦P(X+1)−P(X)P \mapsto P(X+1) - P(X): linear. Kernel: if ΔP=0\Delta P = 0, then P(0)=P(1)=P(2)=…P(0) = P(1) = P(2) = \dots, so P−P(0)P - P(0) has infinitely many roots and vanishes (Corollary 8.8): ker⁡Δ\ker\Delta is the line of constants. Rank–nullity: rk⁡Δ=(n+1)−1=n\operatorname{rk}\Delta = (n + 1) - 1 = n. Since deg⁡ΔP<deg⁡P\deg \Delta P < \deg P for nonconstant PP (the top terms cancel), im⁡Δ⊆Rn−1[X]\operatorname{im}\Delta \subseteq \R_{n-1}[X], which has dimension exactly nn: the inclusion is an equality. Conclusion, with no computation of preimages: every polynomial QQ of degree ≤n−1\leq n - 1 is a difference Q=P(X+1)−P(X)Q = P(X+1) - P(X) — the discrete antiderivative exists. (Compare the weekend problem of Chapter 18, where Δ\Delta was inverted explicitly in the binomial basis.)

Example 20.12 (Rank bookkeeping along a composition)

On R2[X]\R_2[X], compose the derivative D(P)=P′D(P) = P' (rank 22: image R1[X]\R_1[X], kernel the constants) with itself. Then D∘D=D2D \circ D = D^2 maps P↦P′′P \mapsto P'', with image R0[X]\R_0[X]: rank 11. Compare with the general bounds: the crude one gives rk⁡D2≤min⁡(2,2)=2\operatorname{rk} D^2 \leq \min(2, 2) = 2; the exact formula of Exercise 20.12 accounts for the loss precisely,

rk⁡D2=rk⁡D−dim⁡(ker⁡D∩im⁡D)=2−1=1,\operatorname{rk} D^2 = \operatorname{rk} D - \dim\bigl(\ker D \cap \operatorname{im} D\bigr) = 2 - 1 = 1 ,

since the constants (kernel of the outer DD) sit inside R1[X]\R_1[X] (image of the inner DD) with dimension 11. Rank is lost exactly where the outer kernel ambushes the inner image — the sentence to remember when composition ranks misbehave.

Example 20.13 (Kernel and image of the Euler operator)

On Rn[X]\R_n[X], let u(P)=X P′u(P) = X\,P' (linear: differentiation and multiplication by XX are). Kernel: XP′=0XP' = 0 forces P′=0P' = 0 (a product of polynomials vanishes only if one factor does), so ker⁡u\ker u is the line of constants. Image: on the monomial basis,

u(Xk)=k Xk(k=0,1,…,n),u(X^k) = k\,X^{k} \qquad (k = 0, 1, \dots, n),

so im⁡u=Vect⁡(X,2X2,…,nXn)=Vect⁡(X,X2,…,Xn)\operatorname{im} u = \operatorname{Vect}(X, 2X^2, \dots, nX^n) = \operatorname{Vect}(X, X^2, \dots, X^n): the polynomials with zero constant term. Check against rank–nullity: rk⁡u=(n+1)−1=n\operatorname{rk} u = (n + 1) - 1 = n, which is indeed the dimension found. Two remarks worth keeping. First, here im⁡u⊕ker⁡u=Rn[X]\operatorname{im} u \oplus \ker u = \R_n[X] — but that is a happy accident of this operator, not a theorem: for the shift-like v(P)=P′v(P) = P' on R1[X]\R_1[X], ker⁡v=im⁡v=R0[X]\ker v = \operatorname{im} v = \R_0[X] and the sum is not direct. Second, the relation u(Xk)=kXku(X^k) = kX^k says each monomial is merely rescaled by uu — a basis adapted to the map, the germ of the eigenvalue idea developed in the Year 2 volume.

20.3 Projections and symmetries

Definition 20.14

Let E=F⊕GE = F \oplus G. The projection onto FF along GG maps x=f+gx = f + g (unique decomposition) to p(x)=fp(x) = f; the associated symmetry is s(x)=f−gs(x) = f - g. Both are linear, and s=2p−ids = 2p - \mathrm{id}.

Theorem 20.15 (Algebraic characterization)

  1. An endomorphism pp is a projection (onto some FF along some GG) if and only if p∘p=pp \circ p = p; then F=im⁡p=ker⁡(p−id)F = \operatorname{im} p = \ker(p - \mathrm{id}) and G=ker⁡pG = \ker p.
  2. An endomorphism ss is a symmetry if and only if s∘s=ids \circ s = \mathrm{id}; then E=ker⁡(s−id)⊕ker⁡(s+id)E = \ker(s - \mathrm{id}) \oplus \ker(s + \mathrm{id}).

Proof. (1) A projection satisfies p(f+g)=fp(f + g) = f and p(f)=fp(f) = f: p2=pp^2 = p. Conversely, let p2=pp^2 = p; set F=im⁡pF = \operatorname{im} p, G=ker⁡pG = \ker p. Every xx writes x=p(x)+(x−p(x))x = p(x) + (x - p(x)) with p(x)∈Fp(x) \in F and p(x−p(x))=p(x)−p2(x)=0p\bigl(x - p(x)\bigr) = p(x) - p^2(x) = 0: E=F+GE = F + G. If y∈F∩Gy \in F \cap G: y=p(z)y = p(z) and p(y)=0p(y) = 0, so y=p(z)=p2(z)=p(y)=0y = p(z) = p^2(z) = p(y) = 0: direct sum, and pp is the projection onto FF along GG. Finally on FF: y=p(z)y = p(z) gives p(y)=yp(y) = y, so F⊆ker⁡(p−id)F \subseteq \ker(p - \mathrm{id}), and conversely p(y)=yp(y) = y puts yy in the image.

(2) The correspondence s=2p−ids = 2p - \mathrm{id}, p=s+id2p = \frac{s + \mathrm{id}}2 is a bijection between endomorphisms, and under it

s2=4p2−4p+id=id  ⟺  4p2=4p  ⟺  p2=p:s^2 = 4p^2 - 4p + \mathrm{id} = \mathrm{id} \iff 4p^2 = 4p \iff p^2 = p :

symmetries correspond exactly to projections. Translating the subspaces: s(x)=x  ⟺  p(x)=xs(x) = x \iff p(x) = x, so ker⁡(s−id)=im⁡p=F\ker(s - \mathrm{id}) = \operatorname{im} p = F; and s(x)=−x  ⟺  2p(x)=0  ⟺  x∈ker⁡p=Gs(x) = -x \iff 2p(x) = 0 \iff x \in \ker p = G, so ker⁡(s+id)=G\ker(s + \mathrm{id}) = G. The direct sum E=F⊕GE = F \oplus G of point (1) becomes the announced decomposition into the fixed vectors and the reversed vectors of ss. ∎

Example 20.16 (A projection and its symmetry, explicitly)

In R2\R^2, project onto F=Vect⁡(1,1)F = \operatorname{Vect}(1,1) along G=Vect⁡(0,1)G = \operatorname{Vect}(0,1). Decompose (x,y)=a(1,1)+b(0,1)(x, y) = a(1,1) + b(0,1): the first coordinate gives a=xa = x, the second b=y−xb = y - x. Hence

p(x,y)=(x,x),s(x,y)=2p(x,y)−(x,y)=(x, 2x−y).p(x, y) = (x, x), \qquad s(x, y) = 2p(x,y) - (x,y) = (x,\ 2x - y).

Check the algebra: p(p(x,y))=p(x,x)=(x,x)p(p(x,y)) = p(x,x) = (x,x), and s(s(x,y))=s(x,2x−y)=(x,2x−(2x−y))=(x,y)s(s(x,y)) = s(x, 2x - y) = (x, 2x - (2x - y)) = (x, y). Geometrically, ss is the “oblique reflection” across the line y=xy = x in the vertical direction: it fixes FF pointwise and reverses GG. Had we projected onto the same FF along G′=Vect⁡(1,−1)G' = \operatorname{Vect}(1,-1) instead, the formula would change to p′(x,y)=(x+y2,x+y2)p'(x,y) = \bigl(\frac{x+y}2, \frac{x+y}2\bigr): a projection is determined by its image and its kernel, never by the image alone.

The projection onto F = Vect(1,1) along G = Vect(0,1) and its symmetry, on the point M = (2,\ 0.5): sliding vertically, M hits F at p(M) = (2,2) and lands at s(M) = 2p(M) - M = (2,\ 3.5), as far above F (measured along G) as M was below.
The projection onto F=Vect⁡(1,1)F = \operatorname{Vect}(1,1) along G=Vect⁡(0,1)G = \operatorname{Vect}(0,1) and its symmetry, on the point M=(2, 0.5)M = (2,\ 0.5): sliding vertically, MM hits FF at p(M)=(2,2)p(M) = (2,2) and lands at s(M)=2p(M)−M=(2, 3.5)s(M) = 2p(M) - M = (2,\ 3.5), as far above FF (measured along GG) as MM was below.

20.4 Linear forms and hyperplanes

Definition 20.17

A linear form on EE is a linear map φ ⁣:E→K\varphi \colon E \to K. A hyperplane of EE (dim⁡E=n\dim E = n) is a subspace of dimension n−1n - 1.

Example 20.18 (An evaluation form and its hyperplane)

On R2[X]\R_2[X], the evaluation φ(P)=P(2)\varphi(P) = P(2) is a linear form, nonzero (φ(1)=1\varphi(1) = 1). Its kernel is the hyperplane of polynomials vanishing at 22, i.e. (factor theorem, Theorem 8.7) the multiples of X−2X - 2 within R2[X]\R_2[X]:

ker⁡φ=Vect⁡(X−2, X(X−2)),dim⁡=2.\ker\varphi = \operatorname{Vect}\bigl(X - 2,\ X(X - 2)\bigr), \qquad \dim = 2 .

In coordinates on (1,X,X2)(1, X, X^2), φ(a+bX+cX2)=a+2b+4c\varphi(a + bX + cX^2) = a + 2b + 4c: every linear form on a finite-dimensional space is, once a basis is fixed, a fixed linear expression in the coordinates — forms are “row vectors”, as Chapter 21 will make literal, and the coefficient row here, (1,2,4)(1, 2, 4), is a Vandermonde row: evaluation forms are how the interpolation theory of Chapter 22’s weekend problem enters linear algebra.

Theorem 20.19

The hyperplanes of EE are exactly the kernels of nonzero linear forms. Two nonzero forms have the same kernel if and only if they are proportional.

Proof. If φ≠0\varphi \neq 0: rk⁡φ=1\operatorname{rk}\varphi = 1 (image a nonzero subspace of KK), so dim⁡ker⁡φ=n−1\dim\ker\varphi = n - 1: a hyperplane. Conversely, let HH be a hyperplane, (e1,…,en−1)(e_1, \dots, e_{n-1}) a basis of HH completed by ene_n: the form “last coordinate” has kernel HH.

Proportional forms share their kernel. Conversely, suppose ker⁡φ=ker⁡ψ=H\ker\varphi = \ker\psi = H and pick a∉Ha \notin H: every xx writes x=h+λax = h + \lambda a (as E=H⊕KaE = H \oplus Ka), and

φ(x)=λφ(a),ψ(x)=λψ(a):\varphi(x) = \lambda \varphi(a), \qquad \psi(x) = \lambda\psi(a):

so φ=φ(a)ψ(a) ψ\varphi = \frac{\varphi(a)}{\psi(a)}\,\psi. ∎

Example 20.20

In KnK^n, a hyperplane is a solution set {a1x1+⋯+anxn=0}\{a_1 x_1 + \dots + a_n x_n = 0\} with not all aia_i zero — the familiar equation of a plane through the origin in R3\R^3. In function spaces, evaluation forms P↦P(1)P \mapsto P(1) or f↦∫01ff \mapsto \int_0^1 f define hyperplanes of Rn[X]\R_n[X], of C([0, 1])C(\intcc{0}{1}) (cf. Exercise 19.6).

Example 20.21 (One hyperplane, worked three ways)

Take φ(x,y,z)=x−2y+3z\varphi(x, y, z) = x - 2y + 3z on R3\R^3 and H=ker⁡φH = \ker\varphi. Basis: solve x=2y−3zx = 2y - 3z:

(2y−3z, y, z)=y (2,1,0)+z (−3,0,1),(2y - 3z,\ y,\ z) = y\,(2, 1, 0) + z\,(-3, 0, 1),

two free vectors: dim⁡H=2\dim H = 2, a hyperplane, as Theorem 20.19 predicts from φ≠0\varphi \neq 0. Supplementary line: any vector outside HH spans one, e.g. a=(1,0,0)a = (1, 0, 0) (φ(a)=1≠0\varphi(a) = 1 \neq 0); the decomposition of an arbitrary vv is explicit:

v=(v−φ(v) a)⏟∈ H+φ(v) a⏟∈ Vect⁡(a),v = \underbrace{\bigl(v - \varphi(v)\,a\bigr)}_{\in\,H} + \underbrace{\varphi(v)\,a}_{\in\,\operatorname{Vect}(a)},

since φ(v−φ(v)a)=φ(v)−φ(v)φ(a)=0\varphi\bigl(v - \varphi(v)a\bigr) = \varphi(v) - \varphi(v)\varphi(a) = 0. Proportionality: if ψ(x,y,z)=−2x+4y−6z\psi(x,y,z) = -2x + 4y - 6z, then ψ=−2φ\psi = -2\varphi and both have kernel HH; conversely, any form vanishing on HH is a multiple of φ\varphi (Exercise 20.8) — the equation of a hyperplane is unique up to scale, a fact used constantly for planes in geometry.

Remark 20.22 (Common pitfalls)

Kernel and image live in different spaces: ker⁡u⊆E\ker u \subseteq E, im⁡u⊆F\operatorname{im} u \subseteq F; the sum ker⁡u+im⁡u\ker u + \operatorname{im} u only makes sense for endomorphisms, and even then it need not be direct (u(x,y)=(y,0)u(x, y) = (y, 0) has ker⁡u=im⁡u\ker u = \operatorname{im} u; Exercise 20.7 characterizes when directness holds). u2=0u^2 = 0 does not mean u=0u = 0: the same u(x,y)=(y,0)u(x,y) = (y, 0) squares to zero without vanishing — what u2=0u^2 = 0 really says is im⁡u⊆ker⁡u\operatorname{im} u \subseteq \ker u (Exercise 20.5). Injective   ⟺  \iff surjective needs equal finite dimensions: on K[X]K[X], the derivative is surjective and not injective, P↦XPP \mapsto XP injective and not surjective (Corollary 20.9); and between spaces of different dimensions, one implication is simply impossible (rk⁡u≤min⁡(dim⁡E,dim⁡F)\operatorname{rk} u \leq \min(\dim E, \dim F)). Prescribing images works on a basis, not on any family: demanding u(1,0)=au(1, 0) = a, u(0,1)=bu(0, 1) = b, u(1,1)=cu(1, 1) = c overdetermines uu unless c=a+bc = a + b; a linear map is free on a basis, enslaved everywhere else. Rank is not preserved by composition: it can only drop, rk⁡(vu)≤min⁡(rk⁡u,rk⁡v)\operatorname{rk}(vu) \leq \min(\operatorname{rk} u, \operatorname{rk} v) (Exercise 20.4), with exact loss measured in Exercise 20.12.

Remark 20.23 (Where these maps go)

Linear maps are about to become matrices: once bases are fixed, Chapter 21 encodes every u∈L(E,F)u \in \mathcal{L}(E, F) by a rectangular array, and composition becomes the matrix product — rank–nullity then drives the theory of linear systems in Chapter 22. Projections return in Chapter 23 in their most useful special case, the orthogonal projection, where the kernel is chosen perpendicular to the image. The weekend problem below pushes the projector algebra as far as first-year tools reach, up to Fitting’s lemma; the Year 2 volume goes further with the trace and with eigenvalue theory, for which projectors onto stable subspaces are the basic building blocks.

Remark 20.24 (Perspectives inside Book 3: rank–nullity three more times)

The conservation law dim⁡E=dim⁡ker⁡u+rk⁡u\dim E = \dim\ker u + \operatorname{rk} u will be re-read three times before the volume ends. In Chapter 22 it becomes the shape of solution sets: a compatible system with pp unknowns and rank rr has a solution set of dimension p−rp - r — kernel dimension in disguise. In Chapter 23 it splits orthogonally, dim⁡F+dim⁡F⊥=dim⁡E\dim F + \dim F^\perp = \dim E, and powers every distance computation. In the weekend problem of Chapter 25, it is the accountant of least squares: nn observations, 22 fitted parameters, n−2n - 2 residual dimensions, and the Pythagorean identity ∥b∥2=∥p∥2+∥b−p∥2\norm b^2 = \norm p^2 + \norm{b - p}^2 is rank–nullity’s Euclidean shadow. One theorem, four costumes.

20.5 Exercises

Exercise 20.1 ★

Which maps are linear?

  1. R2→R2\R^2 \to \R^2, (x,y)↦(x+y,x−2y)(x, y) \mapsto (x + y, x - 2y);
  2. R2→R\R^2 \to \R, (x,y)↦xy(x, y) \mapsto xy;
  3. R[X]→R[X]\R[X] \to \R[X], P↦P′+XPP \mapsto P' + XP;
  4. F(R,R)→R\mathcal{F}(\R,\R) \to \R, f↦f(3)f \mapsto f(3).
Solution

Solution of Exercise 20.1.

(1) Linear: coordinates are linear expressions. (2) Not linear: u(2(1,1))=4≠2=2u(1,1)u(2(1,1)) = 4 \neq 2 = 2u(1,1). (3) Linear: differentiation and multiplication by XX are, and sums of linear maps are. (4) Linear: evaluation respects pointwise operations.

Exercise 20.2 ★

Let u ⁣:R3→R3u \colon \R^3 \to \R^3, (x,y,z)↦(x+y−z,  2x+y+z,  3x+2y)(x,y,z) \mapsto (x + y - z,\; 2x + y + z,\; 3x + 2y). Determine ker⁡u\ker u (basis, dimension), rk⁡u\operatorname{rk} u, and a basis of im⁡u\operatorname{im} u. Is uu injective? surjective?

Solution

Solution of Exercise 20.2.

Kernel: solve x+y−z=0x + y - z = 0, 2x+y+z=02x + y + z = 0, 3x+2y=03x + 2y = 0. From the third, y=−3x2y = -\frac{3x}{2}; the first gives z=x+y=−x2z = x + y = -\frac x2; check in the second: 2x−3x2−x2=02x - \frac{3x}{2} - \frac x2 = 0: satisfied. So ker⁡u=Vect⁡((2,−3,−1))\ker u = \operatorname{Vect}\bigl((2, -3, -1)\bigr) (taking x=2x = 2), dimension 11.

Rank–nullity: rk⁡u=3−1=2\operatorname{rk} u = 3 - 1 = 2. Image: spanned by the images of the canonical basis, u(e1)=(1,2,3)u(e_1) = (1,2,3), u(e2)=(1,1,2)u(e_2) = (1,1,2), u(e3)=(−1,1,0)u(e_3) = (-1,1,0); the first two are free, and the rank is 22: basis ((1,2,3),(1,1,2))\bigl((1,2,3), (1,1,2)\bigr).

Not injective (ker⁡≠{0}\ker \neq \{0\}), not surjective (rank 2<32 < 3): consistent with Corollary 20.9.

Exercise 20.3 ★

Let u ⁣:Rn[X]→Rn[X]u \colon \R_n[X] \to \R_n[X], P↦P−P′P \mapsto P - P'. Prove that uu is an isomorphism: once via ker⁡u\ker u, once by exhibiting the inverse (consider P+P′+P′′+…P + P' + P'' + \dots).

Solution

Solution of Exercise 20.3.

Kernel: P=P′P = P' forces deg⁡P=deg⁡P′\deg P = \deg P' unless P=0P = 0; but deg⁡P′<deg⁡P\deg P' < \deg P for P≠0P \neq 0: so ker⁡u={0}\ker u = \{0\}, and uu, an injective endomorphism of the finite-dimensional Rn[X]\R_n[X], is an isomorphism (Corollary 20.9).

Inverse: let v(P)=P+P′+P′′+⋯+P(n)v(P) = P + P' + P'' + \dots + P^{(n)} (a finite sum on Rn[X]\R_n[X]). Then

v(u(P))=∑k=0n(P−P′)(k)=∑k=0nP(k)−∑k=0nP(k+1)=P−P(n+1)=P,v\bigl(u(P)\bigr) = \sum_{k=0}^{n} (P - P')^{(k)} = \sum_{k=0}^{n} P^{(k)} - \sum_{k=0}^{n} P^{(k+1)} = P - P^{(n+1)} = P ,

telescoping, since P(n+1)=0P^{(n+1)} = 0. So v=u−1v = u^{-1}.

Exercise 20.4 ★

Let u∈L(E,F)u \in \mathcal{L}(E, F) and v∈L(F,G)v \in \mathcal{L}(F, G), spaces finite-dimensional. Prove:

rk⁡(v∘u)≤min⁡(rk⁡u, rk⁡v).\operatorname{rk}(v \circ u) \leq \min\bigl(\operatorname{rk} u,\ \operatorname{rk} v\bigr).
Solution

Solution of Exercise 20.4.

im⁡(v∘u)=v(im⁡u)⊆im⁡v\operatorname{im}(v \circ u) = v(\operatorname{im} u) \subseteq \operatorname{im} v: rank ≤rk⁡v\leq \operatorname{rk} v. And vv restricted to im⁡u\operatorname{im} u has image im⁡(vu)\operatorname{im}(vu) with rank–nullity inside im⁡u\operatorname{im} u: rk⁡(vu)≤dim⁡im⁡u=rk⁡u\operatorname{rk}(vu) \leq \dim\operatorname{im} u = \operatorname{rk} u.

Exercise 20.5 ★★

Let uu be an endomorphism of EE (finite-dimensional) with u2=0u^2 = 0. Prove that im⁡u⊆ker⁡u\operatorname{im} u \subseteq \ker u, hence rk⁡u≤dim⁡E2\operatorname{rk} u \leq \frac{\dim E}{2}. For E=R2E = \R^2, give an example with equality.

Solution

Solution of Exercise 20.5.

u2=0u^2 = 0 means u(u(x))=0u(u(x)) = 0 for all xx: every u(x)u(x) lies in ker⁡u\ker u, i.e. im⁡u⊆ker⁡u\operatorname{im} u \subseteq \ker u. Then rank–nullity:

dim⁡E=dim⁡ker⁡u+rk⁡u≥2rk⁡u.\dim E = \dim\ker u + \operatorname{rk} u \geq 2\operatorname{rk} u .

Equality example in R2\R^2: u(x,y)=(y,0)u(x, y) = (y, 0): u2=0u^2 = 0, rk⁡u=1=dim⁡E2\operatorname{rk} u = 1 = \frac{\dim E}{2}.

Exercise 20.6 ★★

Let p,qp, q be projections of EE with p∘q=q∘pp \circ q = q \circ p. Prove that p∘qp \circ q is a projection, with

im⁡(pq)=im⁡p∩im⁡q,ker⁡(pq)=ker⁡p+ker⁡q.\operatorname{im}(pq) = \operatorname{im} p \cap \operatorname{im} q , \qquad \ker (pq) = \ker p + \ker q .
Solution

Solution of Exercise 20.6.

(pq)2=pqpq=ppqq=pq(pq)^2 = pqpq = ppqq = pq (commutation): a projection (Theorem 20.15).

Image: im⁡(pq)⊆im⁡p\operatorname{im}(pq) \subseteq \operatorname{im} p, and =im⁡(qp)⊆im⁡q= \operatorname{im}(qp) \subseteq \operatorname{im} q: contained in the intersection. Conversely, if x∈im⁡p∩im⁡qx \in \operatorname{im} p \cap \operatorname{im} q, then p(x)=xp(x) = x and q(x)=xq(x) = x (fixed points characterize the image of a projection), so pq(x)=xpq(x) = x: x∈im⁡(pq)x \in \operatorname{im}(pq).

Kernel: ker⁡p⊆ker⁡(qp)=ker⁡(pq)\ker p \subseteq \ker(qp) = \ker(pq) and likewise ker⁡q⊆ker⁡(pq)\ker q \subseteq \ker(pq): the sum is contained. Conversely, let pq(x)=0pq(x) = 0, and write

x=q(x)⏟∈ ker⁡p+(x−q(x))⏟∈ ker⁡q:x = \underbrace{q(x)}_{\in\, \ker p} + \underbrace{(x - q(x))}_{\in\, \ker q} :

the first term satisfies p(q(x))=0p(q(x)) = 0, so it lies in ker⁡p\ker p; the second is in ker⁡q\ker q since q(x−q(x))=q(x)−q2(x)=0q(x - q(x)) = q(x) - q^2(x) = 0. Hence x∈ker⁡p+ker⁡qx \in \ker p + \ker q.

Exercise 20.7 ★★

Let u∈L(E)u \in \mathcal{L}(E), EE finite-dimensional. Prove the equivalence of:

  1. E=ker⁡u⊕im⁡uE = \ker u \oplus \operatorname{im} u;
  2. ker⁡u=ker⁡u2\ker u = \ker u^2;
  3. im⁡u=im⁡u2\operatorname{im} u = \operatorname{im} u^2.
Solution

Solution of Exercise 20.7.

Note first the general inclusions ker⁡u⊆ker⁡u2\ker u \subseteq \ker u^2 and im⁡u2⊆im⁡u\operatorname{im} u^2 \subseteq \operatorname{im} u, and by rank–nullity, (2)   ⟺  \iff (3) (equal kernels   ⟺  \iff equal ranks   ⟺  \iff equal images, given the inclusions).

(1 ⇒\Rightarrow 2): let u2(x)=0u^2(x) = 0; then u(x)∈ker⁡u∩im⁡u={0}u(x) \in \ker u \cap \operatorname{im} u = \{0\}, so x∈ker⁡ux \in \ker u.

(2 ⇒\Rightarrow 1): by Grassmann and rank–nullity, dim⁡(ker⁡u+im⁡u)=dim⁡ker⁡u+rk⁡u−dim⁡(ker⁡u∩im⁡u)=dim⁡E−dim⁡(ker⁡u∩im⁡u)\dim(\ker u + \operatorname{im} u) = \dim\ker u + \operatorname{rk} u - \dim(\ker u \cap \operatorname{im} u) = \dim E - \dim(\ker u \cap \operatorname{im} u): the sum is EE iff the intersection is {0}\{0\}. Let y∈ker⁡u∩im⁡uy \in \ker u \cap \operatorname{im} u: y=u(x)y = u(x) and u(y)=0u(y) = 0, so u2(x)=0u^2(x) = 0, so (by (2)) u(x)=0u(x) = 0: y=0y = 0. Hence E=ker⁡u⊕im⁡uE = \ker u \oplus \operatorname{im} u.

Exercise 20.8 ★★

Let φ,ψ\varphi, \psi be linear forms on EE with ker⁡φ⊆ker⁡ψ\ker\varphi \subseteq \ker\psi. Prove ψ=λφ\psi = \lambda\varphi for some λ∈K\lambda \in K (including the degenerate cases).

Solution

Solution of Exercise 20.8.

If φ=0\varphi = 0: then ker⁡φ=E⊆ker⁡ψ\ker\varphi = E \subseteq \ker\psi forces ψ=0=0⋅φ\psi = 0 = 0\cdot\varphi. If φ≠0\varphi \neq 0: ker⁡φ\ker\varphi is a hyperplane; pick a∉ker⁡φa \notin \ker\varphi. Set λ=ψ(a)φ(a)\lambda = \frac{\psi(a)}{\varphi(a)}. The form ψ−λφ\psi - \lambda\varphi vanishes on ker⁡φ\ker\varphi (both do, by the inclusion) and at aa: it vanishes on ker⁡φ⊕Ka=E\ker\varphi \oplus Ka = E. So ψ=λφ\psi = \lambda\varphi.

Exercise 20.9 ★★★

Let u∈L(E)u \in \mathcal{L}(E) with dim⁡E=n\dim E = n, and suppose un=0u^n = 0 but un−1≠0u^{n-1} \neq 0 (a maximally nilpotent endomorphism). Pick xx with un−1(x)≠0u^{n-1}(x) \neq 0; prove that (x,u(x),…,un−1(x))\bigl(x, u(x), \dots, u^{n-1}(x)\bigr) is a basis of EE. (Apply powers of uu to a null combination, starting with un−1u^{n-1}.)

Solution

Solution of Exercise 20.9.

Suppose λ0x+λ1u(x)+⋯+λn−1un−1(x)=0\lambda_0 x + \lambda_1 u(x) + \dots + \lambda_{n-1} u^{n-1}(x) = 0. Apply un−1u^{n-1}: all terms with a factor u≥nu^{\geq n} die, leaving λ0un−1(x)=0\lambda_0 u^{n-1}(x) = 0, so λ0=0\lambda_0 = 0. Apply un−2u^{n-2} to the remaining relation: λ1un−1(x)=0\lambda_1 u^{n-1}(x) = 0, so λ1=0\lambda_1 = 0; and so on. The family is free; being of size n=dim⁡En = \dim E, it is a basis (Proposition 19.8). (In this basis, uu acts as a shift — the model of maximal nilpotence.)

Exercise 20.10 ★★★

Let f∈L(Rn)f \in \mathcal{L}(\R^n) with f∘f=−idf \circ f = -\mathrm{id}.

  1. Prove that ff is an isomorphism and that no x≠0x \neq 0 satisfies f(x)=λxf(x) = \lambda x with λ∈R\lambda \in \R.
  2. Prove that nn is even. Hint: pick x1≠0x_1 \neq 0; show Vect⁡(x1,f(x1))\operatorname{Vect}(x_1, f(x_1)) is a plane stable under ff; choose x2x_2 outside it and iterate, proving that (x1,f(x1),x2,f(x2),… )\bigl(x_1, f(x_1), x_2, f(x_2), \dots\bigr) stays free.
Solution

Solution of Exercise 20.10.

  1. f∘f=−idf \circ f = -\mathrm{id} is bijective, so ff is (Proposition 1.26 adapted: ff has the two-sided inverse −f-f). If f(x)=λxf(x) = \lambda x with x≠0x \neq 0: applying ff, −x=λ2x-x = \lambda^2 x, so λ2=−1\lambda^2 = -1: impossible in R\R.
  2. Build the family greedily. Take x1≠0x_1 \neq 0: (x1,f(x1))(x_1, f(x_1)) is free by (1). If Vect⁡\operatorname{Vect} of the current family (x1,f(x1),…,xk,f(xk))\bigl(x_1, f(x_1), \dots, x_k, f(x_k)\bigr), call it VkV_k — a subspace stable under ff (each generator maps to another generator or its negative: f(f(xi))=−xif(f(x_i)) = -x_i) — is not all of EE, choose xk+1∉Vkx_{k+1} \notin V_k. Claim: the enlarged family is free. Suppose αxk+1+βf(xk+1)+v=0\alpha x_{k+1} + \beta f(x_{k+1}) + v = 0 with v∈Vkv \in V_k and (α,β)≠(0,0)(\alpha, \beta) \neq (0,0). Apply ff: αf(xk+1)−βxk+1+f(v)=0\alpha f(x_{k+1}) - \beta x_{k+1} + f(v) = 0 with f(v)∈Vkf(v) \in V_k. Eliminate f(xk+1)f(x_{k+1}) between the two relations (multiply the first by α\alpha, the second by −β-\beta, and add):

    (α2+β2) xk+1∈Vk,(\alpha^2 + \beta^2)\, x_{k+1} \in V_k ,

    and α2+β2≠0\alpha^2 + \beta^2 \neq 0 forces xk+1∈Vkx_{k+1} \in V_k: contradiction. So the construction continues, adding vectors two at a time, until Vk=EV_k = E: the final family is a basis of even size, and nn is even.

Exercise 20.11 ★★

Let u,v∈L(E,F)u, v \in \mathcal{L}(E, F), spaces finite-dimensional. Prove the two-sided bound

∣rk⁡u−rk⁡v∣  ≤  rk⁡(u+v)  ≤  rk⁡u+rk⁡v.\abs{\operatorname{rk} u - \operatorname{rk} v} \;\leq\; \operatorname{rk}(u + v) \;\leq\; \operatorname{rk} u + \operatorname{rk} v .

(For the upper bound, compare im⁡(u+v)\operatorname{im}(u+v) with im⁡u+im⁡v\operatorname{im} u + \operatorname{im} v; for the lower one, apply the upper bound cleverly.)

Solution

Solution of Exercise 20.11.

Upper bound: for every xx, (u+v)(x)=u(x)+v(x)∈im⁡u+im⁡v(u + v)(x) = u(x) + v(x) \in \operatorname{im} u + \operatorname{im} v, so

rk⁡(u+v)≤dim⁡(im⁡u+im⁡v)≤rk⁡u+rk⁡v\operatorname{rk}(u + v) \leq \dim(\operatorname{im} u + \operatorname{im} v) \leq \operatorname{rk} u + \operatorname{rk} v

(Grassmann, Theorem 19.18). Lower bound: apply the upper bound to the pair (u+v,−v)(u + v, -v), whose sum is uu:

rk⁡u≤rk⁡(u+v)+rk⁡(−v)=rk⁡(u+v)+rk⁡v,\operatorname{rk} u \leq \operatorname{rk}(u + v) + \operatorname{rk}(-v) = \operatorname{rk}(u + v) + \operatorname{rk} v,

so rk⁡u−rk⁡v≤rk⁡(u+v)\operatorname{rk} u - \operatorname{rk} v \leq \operatorname{rk}(u+v); exchanging uu and vv gives the absolute value.

Exercise 20.12 ★★★

(Frobenius’ inequality) Let u∈L(E,F)u \in \mathcal{L}(E, F), w∈L(F,G)w \in \mathcal{L}(F, G) and v∈L(G,H)v \in \mathcal{L}(G, H), all spaces finite-dimensional. Prove the exact formula

rk⁡(v∘w)=rk⁡w−dim⁡(ker⁡v∩im⁡w),\operatorname{rk}(v \circ w) = \operatorname{rk} w - \dim\bigl(\ker v \cap \operatorname{im} w\bigr),

and deduce Frobenius’ inequality

rk⁡(v∘w)+rk⁡(w∘u)  ≤  rk⁡w+rk⁡(v∘w∘u).\operatorname{rk}(v \circ w) + \operatorname{rk}(w \circ u) \;\leq\; \operatorname{rk} w + \operatorname{rk}(v \circ w \circ u) .

Check that the case w=idFw = \mathrm{id}_F is Sylvester’s inequality, proved in matrix form in Exercise 21.10.

Solution

Solution of Exercise 20.12.

Exact formula. Let v′v' be the restriction of vv to the subspace im⁡w\operatorname{im} w. Its image is v(w(F))=im⁡(v∘w)v(w(F)) = \operatorname{im}(v \circ w), and its kernel is ker⁡v∩im⁡w\ker v \cap \operatorname{im} w. Rank–nullity for v′v' on the space im⁡w\operatorname{im} w:

rk⁡w=dim⁡im⁡w=rk⁡(v∘w)+dim⁡(ker⁡v∩im⁡w).\operatorname{rk} w = \dim\operatorname{im} w = \operatorname{rk}(v \circ w) + \dim(\ker v \cap \operatorname{im} w) .

Frobenius. Apply the exact formula twice, to ww and to w∘uw \circ u:

rk⁡w−rk⁡(vw)=dim⁡(ker⁡v∩im⁡w),rk⁡(wu)−rk⁡(vwu)=dim⁡(ker⁡v∩im⁡(wu)).\operatorname{rk} w - \operatorname{rk}(vw) = \dim\bigl(\ker v \cap \operatorname{im} w\bigr), \qquad \operatorname{rk}(wu) - \operatorname{rk}(vwu) = \dim\bigl(\ker v \cap \operatorname{im}(wu)\bigr) .

Since im⁡(w∘u)⊆im⁡w\operatorname{im}(w \circ u) \subseteq \operatorname{im} w, the second intersection is contained in the first, and its dimension is no larger:

rk⁡(wu)−rk⁡(vwu)  ≤  rk⁡w−rk⁡(vw),\operatorname{rk}(wu) - \operatorname{rk}(vwu) \;\leq\; \operatorname{rk} w - \operatorname{rk}(vw) ,

which rearranges into Frobenius’ inequality. With w=idFw = \mathrm{id}_F (rank dim⁡F\dim F, and im⁡ idF=F\operatorname{im}\, \mathrm{id}_F = F): rk⁡v+rk⁡u≤dim⁡F+rk⁡(vu)\operatorname{rk} v + \operatorname{rk} u \leq \dim F + \operatorname{rk}(vu), Sylvester’s inequality — proved again, in matrix form, in Exercise 21.10.

20.6 Problem: projector calculus and Fitting’s lemma

Problem 20.1

Projections are the endomorphisms that direct sums produce, and conversely: every identity E=F1⊕⋯⊕FkE = F_1 \oplus \dots \oplus F_k is secretly a family of projectors summing to the identity. This problem develops that dictionary — the algebra of one projector, of two, of kk — then applies the same stabilization ideas to an arbitrary endomorphism and proves Fitting’s lemma: every endomorphism of a finite-dimensional space splits into a nilpotent part and an invertible part. Throughout, EE is a KK-vector space of dimension nn, and projector means p∈L(E)p \in \mathcal{L}(E) with p2=pp^2 = p (Theorem 20.15).

Part I — The algebra around one projector. Let pp be a projector, p≠0p \neq 0, p≠idp \neq \mathrm{id}.

  1. Show that id−p\mathrm{id} - p is a projector and identify im⁡(id−p)\operatorname{im}(\mathrm{id} - p) and ker⁡(id−p)\ker(\mathrm{id} - p).
  2. Compute (λ id+μ p)2(\lambda\,\mathrm{id} + \mu\,p)^2 and determine all pairs (λ,μ)∈K2(\lambda, \mu) \in K^2 for which λ id+μ p\lambda\,\mathrm{id} + \mu\,p is a projector.
  3. Show that the plane Vect⁡(id,p)\operatorname{Vect}(\mathrm{id}, p) of L(E)\mathcal{L}(E) is stable under composition, and that for every polynomial Q∈K[X]Q \in K[X],

    Q(p)=Q(0) id+(Q(1)−Q(0)) p.Q(p) = Q(0)\,\mathrm{id} + \bigl(Q(1) - Q(0)\bigr)\,p .
  4. Determine for which (λ,μ)(\lambda, \mu) the map λ id+μ p\lambda\,\mathrm{id} + \mu\,p is invertible, and give its inverse in the form α id+β p\alpha\,\mathrm{id} + \beta\,p. Interpret the answer through the action of λ id+μ p\lambda\,\mathrm{id} + \mu\,p on im⁡p\operatorname{im} p and on ker⁡p\ker p.
  5. Let p′p' be another projector with the same image im⁡p′=im⁡p\operatorname{im} p' = \operatorname{im} p. Show that p p′=p′p\,p' = p' and p′ p=pp'\,p = p. What do these identities say about composing projections onto the same subspace along different kernels?

Part II — Two projectors. Let p,qp, q be projectors of EE; assume the characteristic is not 22 (true for K=R,CK = \R, \C).

  1. Suppose p+qp + q is a projector. Expanding (p+q)2(p + q)^2, show pq+qp=0pq + qp = 0; composing with pp on the left, then on the right, deduce pq=qppq = qp, and conclude pq=qp=0pq = qp = 0.
  2. Conversely, suppose pq=qp=0pq = qp = 0. Show that p+qp + q is a projector, with

    im⁡(p+q)=im⁡p⊕im⁡q,ker⁡(p+q)=ker⁡p∩ker⁡q.\operatorname{im}(p + q) = \operatorname{im} p \oplus \operatorname{im} q, \qquad \ker(p + q) = \ker p \cap \ker q .
  3. Show that p−qp - q is a projector if and only if pq=qp=qpq = qp = q. (Apply questions 6–7 to id−p\mathrm{id} - p and qq.)
  4. Show the geometric meaning of pq=qp=qpq = qp = q: it holds if and only if im⁡q⊆im⁡p\operatorname{im} q \subseteq \operatorname{im} p and ker⁡p⊆ker⁡q\ker p \subseteq \ker q. (One then writes q≤pq \leq p: “qq projects onto less, along more”.)
  5. Now let p,qp, q commute. Recall from Exercise 20.6 that pqpq is the projector onto im⁡p∩im⁡q\operatorname{im} p \cap \operatorname{im} q along ker⁡p+ker⁡q\ker p + \ker q. Show that r=p+q−pqr = p + q - pq is a projector with

    im⁡r=im⁡p+im⁡q,ker⁡r=ker⁡p∩ker⁡q.\operatorname{im} r = \operatorname{im} p + \operatorname{im} q, \qquad \ker r = \ker p \cap \ker q .

    (Consider id−r=(id−p)(id−q)\mathrm{id} - r = (\mathrm{id} - p)(\mathrm{id} - q).)

Part III — Decompositions of the identity.

  1. Let E=F1⊕⋯⊕FkE = F_1 \oplus \dots \oplus F_k and, for x=x1+⋯+xkx = x_1 + \dots + x_k (unique decomposition, xi∈Fix_i \in F_i), set pi(x)=xip_i(x) = x_i. Show that each pip_i is a projector, that pipj=0p_i p_j = 0 for i≠ji \neq j, and that p1+⋯+pk=idp_1 + \dots + p_k = \mathrm{id}; identify im⁡pi\operatorname{im} p_i and ker⁡pi\ker p_i.
  2. Conversely, let p1,…,pk∈L(E)p_1, \dots, p_k \in \mathcal{L}(E) satisfy p1+⋯+pk=idp_1 + \dots + p_k = \mathrm{id} and pipj=0p_i p_j = 0 for all i≠ji \neq j. Show that each pip_i is a projector and that E=im⁡p1⊕⋯⊕im⁡pkE = \operatorname{im} p_1 \oplus \dots \oplus \operatorname{im} p_k.
  3. Two projectors with p+q=idp + q = \mathrm{id}: show that pq=qp=0pq = qp = 0 holds automatically.
  4. Three projectors with p+q+r=idp + q + r = \mathrm{id}: show that p+qp + q is a projector, and deduce from question 6 that all pairwise products vanish — hence E=im⁡p⊕im⁡q⊕im⁡rE = \operatorname{im} p \oplus \operatorname{im} q \oplus \operatorname{im} r, with no hypothesis on the products.
  5. For kk projectors with p1+⋯+pk=idp_1 + \dots + p_k = \mathrm{id}: show first that for any subspaces, dim⁡(F1+⋯+Fk)≤dim⁡F1+⋯+dim⁡Fk\dim (F_1 + \dots + F_k) \leq \dim F_1 + \dots + \dim F_k, with equality if and only if the sum is direct; then show E=im⁡p1+⋯+im⁡pkE = \operatorname{im} p_1 + \dots + \operatorname{im} p_k, and prove that if moreover ∑irk⁡pi≤n\sum_i \operatorname{rk} p_i \leq n, the sum is direct and pipj=0p_i p_j = 0 for i≠ji \neq j.

Part IV — Iterated kernels: Fitting’s lemma. Let u∈L(E)u \in \mathcal{L}(E), dim⁡E=n\dim E = n.

  1. Show the two chains, valid for every k≥0k \geq 0:

    ker⁡uk⊆ker⁡uk+1,im⁡uk+1⊆im⁡uk.\ker u^k \subseteq \ker u^{k+1}, \qquad \operatorname{im} u^{k+1} \subseteq \operatorname{im} u^k .
  2. Show that if ker⁡ur=ker⁡ur+1\ker u^{r} = \ker u^{r+1} for some rr, then ker⁡uk=ker⁡ur\ker u^{k} = \ker u^{r} for all k≥rk \geq r; state and prove the analogous stabilization for images.
  3. Deduce that there is a smallest integer rr with ker⁡ur=ker⁡ur+1\ker u^{r} = \ker u^{r+1}, that r≤nr \leq n, and that images stabilize at the same rr.
  4. (Fitting’s lemma) Prove that

    E  =  ker⁡ur ⊕ im⁡ur.E \;=\; \ker u^{r} \,\oplus\, \operatorname{im} u^{r} .
  5. Show that both subspaces are stable under uu, that the restriction of uu to ker⁡ur\ker u^{r} is nilpotent, and that the restriction of uu to im⁡ur\operatorname{im} u^{r} is an isomorphism of im⁡ur\operatorname{im} u^{r}: every endomorphism is, on a canonical direct sum, “nilpotent plus invertible”.
  6. Let π\pi be the projector onto ker⁡ur\ker u^{r} along im⁡ur\operatorname{im} u^{r}. Show that π∘u=u∘π\pi \circ u = u \circ \pi.

Part V — A worked case, and synthesis.

  1. Let u(x,y,z)=(y,0,z)u(x, y, z) = (y, 0, z) on R3\R^3. Compute u2u^2 and u3u^3, determine the stabilization index rr, the subspaces ker⁡ur\ker u^{r} and im⁡ur\operatorname{im} u^{r}, the Fitting projector π\pi, and verify on the formulas that πu=uπ\pi u = u\pi and that uu is nilpotent on one factor, bijective on the other.
  2. Show the equivalences: uu nilpotent   ⟺  \iff ker⁡ur=E\ker u^{r} = E   ⟺  \iff π=id\pi = \mathrm{id}; and deduce that a nilpotent endomorphism of an nn-dimensional space always satisfies un=0u^{n} = 0 (the nilpotency index never exceeds the dimension).
  3. (Uniqueness) Suppose E=A⊕BE = A \oplus B with A,BA, B stable under uu, the restriction u∣Au|_A nilpotent and u∣Bu|_B bijective. Prove A=ker⁡urA = \ker u^{r} and B=im⁡urB = \operatorname{im} u^{r}: the Fitting decomposition is unique.
  4. Synthesis, in four sentences: what dictionary Part III establishes between direct sums and families of projectors; why question 14 needed no product hypotheses while question 15 needed a rank hypothesis (and which Year 2 tool, the trace, removes it); in what sense Fitting’s lemma is the stabilized version of Exercise 20.7; and what the two factors of Fitting become in the eigenvalue theory of the Year 2 volume. Name the theorem proved in Part IV.
Solution

Solution of Problem 20.1.

1. (id−p)2=id−2p+p2=id−p(\mathrm{id} - p)^2 = \mathrm{id} - 2p + p^2 = \mathrm{id} - p: a projector. If y=x−p(x)y = x - p(x), then p(y)=p(x)−p2(x)=0p(y) = p(x) - p^2(x) = 0, and conversely x∈ker⁡px \in \ker p gives x=(id−p)(x)x = (\mathrm{id} - p)(x): im⁡(id−p)=ker⁡p\operatorname{im}(\mathrm{id} - p) = \ker p. And (id−p)(x)=0  ⟺  p(x)=x  ⟺  x∈im⁡p(\mathrm{id} - p)(x) = 0 \iff p(x) = x \iff x \in \operatorname{im} p (fixed points, Theorem 20.15): ker⁡(id−p)=im⁡p\ker(\mathrm{id} - p) = \operatorname{im} p.

2. (λ id+μp)2=λ2 id+(2λμ+μ2) p(\lambda\,\mathrm{id} + \mu p)^2 = \lambda^2\,\mathrm{id} + (2\lambda\mu + \mu^2)\,p. The pair (id,p)(\mathrm{id}, p) is free in L(E)\mathcal{L}(E): p=c idp = c\, \mathrm{id} would give c2=cc^2 = c, so p=0p = 0 or id\mathrm{id}, excluded. Identifying coefficients, the map is a projector iff λ2=λ\lambda^2 = \lambda and 2λμ+μ2=μ2\lambda\mu + \mu^2 = \mu. For λ=0\lambda = 0: μ∈{0,1}\mu \in \{0, 1\}. For λ=1\lambda = 1: μ2+μ=0\mu^2 + \mu = 0, μ∈{0,−1}\mu \in \{0, -1\}. Exactly four projectors in the plane: 00, pp, id\mathrm{id}, id−p\mathrm{id} - p.

3. (λ id+μp)(λ′ id+μ′p)=λλ′ id+(λμ′+μλ′+μμ′) p(\lambda\,\mathrm{id} + \mu p)(\lambda'\,\mathrm{id} + \mu' p) = \lambda\lambda'\,\mathrm{id} + (\lambda\mu' + \mu\lambda' + \mu\mu')\,p: the plane is stable under composition. Since pk=pp^k = p for every k≥1k \geq 1, for Q=∑kakXkQ = \sum_k a_k X^k:

Q(p)=a0 id+(∑k≥1ak)p=Q(0) id+(Q(1)−Q(0)) p.Q(p) = a_0\,\mathrm{id} + \Bigl(\sum_{k \geq 1} a_k\Bigr) p = Q(0)\,\mathrm{id} + \bigl(Q(1) - Q(0)\bigr)\,p .

4. On im⁡p\operatorname{im} p (where pp acts as the identity), λ id+μp\lambda\,\mathrm{id} + \mu p multiplies by λ+μ\lambda + \mu; on ker⁡p\ker p, by λ\lambda. As E=im⁡p⊕ker⁡pE = \operatorname{im} p \oplus \ker p, the map is bijective iff λ≠0\lambda \neq 0 and λ+μ≠0\lambda + \mu \neq 0. Solving λα=1\lambda\alpha = 1, λβ+μα+μβ=0\lambda\beta + \mu\alpha + \mu\beta = 0 in the composition rule of question 3:

(λ id+μp)−1=1λ id−μλ(λ+μ) p,(\lambda\,\mathrm{id} + \mu p)^{-1} = \frac1\lambda\,\mathrm{id} - \frac{\mu}{\lambda(\lambda + \mu)}\,p ,

whose action is by 1/λ1/\lambda on ker⁡p\ker p and 1/(λ+μ)1/(\lambda + \mu) on im⁡p\operatorname{im} p, as it must be.

5. Write F=im⁡p=im⁡p′F = \operatorname{im} p = \operatorname{im} p'. For every xx, p′(x)∈Fp'(x) \in F and pp fixes FF pointwise: p(p′(x))=p′(x)p(p'(x)) = p'(x), i.e. p p′=p′p\,p' = p'; symmetrically p′ p=pp'\,p = p. When two projections share their image, the one applied first decides: its output already lies in FF, where the outer projection acts as the identity and changes nothing.

6. (p+q)2=p2+pq+qp+q2=(p+q)+pq+qp(p + q)^2 = p^2 + pq + qp + q^2 = (p + q) + pq + qp, so p+qp + q projector forces pq+qp=0pq + qp = 0. Compose on the left with pp: pq+pqp=0pq + pqp = 0; on the right with pp: pqp+qp=0pqp + qp = 0. Subtracting, pq=qppq = qp; then pq+qp=2pq=0pq + qp = 2pq = 0 and the characteristic is not 22: pq=qp=0pq = qp = 0.

7. With pq=qp=0pq = qp = 0, the same expansion gives (p+q)2=p+q(p + q)^2 = p + q. Image: im⁡(p+q)⊆im⁡p+im⁡q\operatorname{im}(p + q) \subseteq \operatorname{im} p + \operatorname{im} q always. Conversely, for x∈im⁡px \in \operatorname{im} p: q(x)=q(p(x))=0q(x) = q(p(x)) = 0, so (p+q)(x)=p(x)=x(p + q)(x) = p(x) = x and x∈im⁡(p+q)x \in \operatorname{im}(p+q); same for im⁡q\operatorname{im} q. Directness: x∈im⁡p∩im⁡qx \in \operatorname{im} p \cap \operatorname{im} q gives x=p(x)=p(q(x))=0x = p(x) = p(q(x)) = 0. Kernel: if p(x)+q(x)=0p(x) + q(x) = 0, applying pp gives p(x)+p(q(x))=p(x)=0p(x) + p(q(x)) = p(x) = 0, and applying qq gives q(x)=0q(x) = 0: ker⁡(p+q)=ker⁡p∩ker⁡q\ker(p + q) = \ker p \cap \ker q (the reverse inclusion is clear).

8. p−qp - q is a projector iff id−(p−q)=(id−p)+q\mathrm{id} - (p - q) = (\mathrm{id} - p) + q is one (question 1 twice). By questions 6–7 applied to the projectors id−p\mathrm{id} - p and qq, this holds iff (id−p)q=q(id−p)=0(\mathrm{id} - p)q = q(\mathrm{id} - p) = 0, i.e. iff pq=qpq = q and qp=qqp = q.

9. pq=qpq = q means pp fixes every q(x)q(x), i.e. im⁡q⊆ker⁡(p−id)=im⁡p\operatorname{im} q \subseteq \ker(p - \mathrm{id}) = \operatorname{im} p. And qp=qqp = q means q((id−p)(x))=0q\bigl((\mathrm{id} - p)(x)\bigr) = 0 for all xx, i.e. qq vanishes on im⁡(id−p)=ker⁡p\operatorname{im}(\mathrm{id} - p) = \ker p: ker⁡p⊆ker⁡q\ker p \subseteq \ker q. Both steps are equivalences: the order q≤pq \leq p says qq projects onto a smaller image, along a larger kernel.

10. Expanding, (id−p)(id−q)=id−p−q+pq=id−r(\mathrm{id} - p)(\mathrm{id} - q) = \mathrm{id} - p - q + pq = \mathrm{id} - r. The projectors id−p\mathrm{id} - p and id−q\mathrm{id} - q commute, so by Exercise 20.6 their product id−r\mathrm{id} - r is the projector onto im⁡(id−p)∩im⁡(id−q)=ker⁡p∩ker⁡q\operatorname{im}(\mathrm{id} - p) \cap \operatorname{im}(\mathrm{id} - q) = \ker p \cap \ker q along ker⁡(id−p)+ker⁡(id−q)=im⁡p+im⁡q\ker(\mathrm{id} - p) + \ker(\mathrm{id} - q) = \operatorname{im} p + \operatorname{im} q. By question 1, r=id−(id−r)r = \mathrm{id} - (\mathrm{id} - r) is then the projector with im⁡r=im⁡p+im⁡q\operatorname{im} r = \operatorname{im} p + \operatorname{im} q and ker⁡r=ker⁡p∩ker⁡q\ker r = \ker p \cap \ker q.

11. pip_i is well defined (uniqueness of the decomposition) and linear (the decomposition of x+λyx + \lambda y is the sum of the decompositions, again by uniqueness). For xi∈Fix_i \in F_i the decomposition is xix_i itself, so pi(xi)=xip_i(x_i) = x_i: pi2=pip_i^2 = p_i, and pj(xi)=0p_j(x_i) = 0 for j≠ij \neq i: pipj=0p_i p_j = 0 (pj(x)∈Fjp_j(x) \in F_j). Summing the components, ∑ipi=id\sum_i p_i = \mathrm{id}. Finally im⁡pi=Fi\operatorname{im} p_i = F_i and ker⁡pi=⨁j≠iFj\ker p_i = \bigoplus_{j \neq i} F_j.

12. pi=pi∘id=pi∑jpj=pi2+∑j≠ipipj=pi2p_i = p_i \circ \mathrm{id} = p_i\sum_j p_j = p_i^2 + \sum_{j \neq i} p_i p_j = p_i^2: each pip_i is a projector. Every x=id(x)=∑ipi(x)x = \mathrm{id}(x) = \sum_i p_i(x) lies in ∑iim⁡pi\sum_i \operatorname{im} p_i: the images sum to EE. Directness: suppose y1+⋯+yk=0y_1 + \dots + y_k = 0 with yi∈im⁡piy_i \in \operatorname{im} p_i, so pi(yi)=yip_i(y_i) = y_i. Apply pjp_j: pj(yi)=pjpi(yi)=0p_j (y_i) = p_j p_i (y_i) = 0 for i≠ji \neq j, so 0=pj(∑yi)=yj0 = p_j\bigl(\sum y_i\bigr) = y_j, for every jj. Hence E=⨁iim⁡piE = \bigoplus_i \operatorname{im} p_i.

13. q=id−pq = \mathrm{id} - p, and question 1 gives pq=p−p2=0=qppq = p - p^2 = 0 = qp directly: for two projectors, summing to the identity already forces orthogonality of the pair.

14. p+q=id−rp + q = \mathrm{id} - r with rr a projector, and (id−r)(\mathrm{id} - r) is a projector (question 1): so p+qp + q is a projector, and question 6 gives pq=qp=0pq = qp = 0. By symmetry (q+r=id−pq + r = \mathrm{id} - p and p+r=id−qp + r = \mathrm{id} - q), all pairwise products vanish, and question 12 concludes: E=im⁡p⊕im⁡q⊕im⁡rE = \operatorname{im} p \oplus \operatorname{im} q \oplus \operatorname{im} r, automatically.

15. Lemma. By induction with Grassmann (Theorem 19.18):

dim⁡(F1+⋯+Fk)≤dim⁡(F1+⋯+Fk−1)+dim⁡Fk≤⋯≤∑idim⁡Fi.\dim(F_1 + \dots + F_k) \leq \dim(F_1 + \dots + F_{k-1}) + \dim F_k \leq \dots \leq \sum_i \dim F_i .

If the total is an equality, each step is: (F1+⋯+Fj−1)∩Fj={0}(F_1 + \dots + F_{j-1}) \cap F_j = \{0\} for every jj, and a relation y1+⋯+yk=0y_1 + \dots + y_k = 0 (yi∈Fiy_i \in F_i) collapses from the right: yk∈(F1+⋯+Fk−1)∩Fk={0}y_k \in (F_1 + \dots + F_{k-1}) \cap F_k = \{0\}, then yk−1=0y_{k-1} = 0, etc.: the sum is direct. Conversely a direct sum has additive dimensions (concatenate bases). Application: x=∑ipi(x)x = \sum_i p_i(x) shows E=∑iim⁡piE = \sum_i \operatorname{im} p_i, so n≤∑irk⁡pin \leq \sum_i \operatorname{rk} p_i; the hypothesis gives equality, hence directness. Products: fix jj and y∈im⁡pjy \in \operatorname{im} p_j. Then y=∑ipi(y)y = \sum_i p_i(y) with pi(y)∈im⁡pip_i(y) \in \operatorname{im} p_i, while y=yy = y is also a decomposition (component jj alone); uniqueness forces pi(y)=0p_i(y) = 0 for i≠ji \neq j. Applied to y=pj(x)y = p_j(x): pipj=0p_i p_j = 0.

16. If uk(x)=0u^k(x) = 0 then uk+1(x)=u(0)=0u^{k+1}(x) = u(0) = 0. And im⁡uk+1=uk(u(E))⊆uk(E)=im⁡uk\operatorname{im} u^{k+1} = u^k\bigl(u(E)\bigr) \subseteq u^k(E) = \operatorname{im} u^k.

17. Assume ker⁡ur=ker⁡ur+1\ker u^{r} = \ker u^{r+1} and let x∈ker⁡ur+2x \in \ker u^{r+2}: then u(x)∈ker⁡ur+1=ker⁡uru(x) \in \ker u^{r+1} = \ker u^{r}, so ur+1(x)=0u^{r+1}(x) = 0: x∈ker⁡ur+1x \in \ker u^{r+1}. With question 16, ker⁡ur+1=ker⁡ur+2\ker u^{r+1} = \ker u^{r+2}, and by induction all later kernels coincide with ker⁡ur\ker u^{r}. For images: rank–nullity gives dim⁡im⁡uk=n−dim⁡ker⁡uk\dim\operatorname{im} u^k = n - \dim\ker u^k, so the image dimensions freeze exactly when the kernel dimensions do, and with the inclusions of question 16, equal dimensions mean equal subspaces (Theorem 19.14).

18. The sequence (dim⁡ker⁡uk)k\bigl(\dim\ker u^k\bigr)_k is nondecreasing with values in [ ⁣[0, n] ⁣]\intint{0}{n}; it cannot increase strictly n+1n + 1 times, so some dim⁡ker⁡ur=dim⁡ker⁡ur+1\dim\ker u^{r} = \dim\ker u^{r+1} with r≤nr \leq n, hence ker⁡ur=ker⁡ur+1\ker u^{r} = \ker u^{r+1} (inclusion plus equal dimension). Take rr smallest; question 17 freezes everything from rr on, images included.

19. Intersection: let x∈ker⁡ur∩im⁡urx \in \ker u^{r} \cap \operatorname{im} u^{r}, say x=ur(y)x = u^{r}(y) with ur(x)=0u^{r}(x) = 0. Then u2r(y)=0u^{2r}(y) = 0, and ker⁡u2r=ker⁡ur\ker u^{2r} = \ker u^{r} (question 17), so x=ur(y)=0x = u^{r}(y) = 0. Dimensions: rank–nullity for uru^{r} gives dim⁡ker⁡ur+dim⁡im⁡ur=n\dim\ker u^{r} + \dim\operatorname{im} u^{r} = n; with trivial intersection, Grassmann makes the sum a subspace of dimension nn: E=ker⁡ur⊕im⁡urE = \ker u^{r} \oplus \operatorname{im} u^{r}.

20. Stability: ur(u(x))=u(ur(x))=0u^{r}(u(x)) = u(u^{r}(x)) = 0 for x∈ker⁡urx \in \ker u^{r}; and u(ur(y))=ur(u(y))∈im⁡uru(u^{r}(y)) = u^{r}(u(y)) \in \operatorname{im} u^{r}. On N=ker⁡urN = \ker u^{r}: (u∣N)r=0(u|_N)^{r} = 0 by definition of NN: nilpotent. On I=im⁡urI = \operatorname{im} u^{r}: ker⁡(u∣I)=ker⁡u∩I⊆ker⁡ur∩I={0}\ker(u|_I) = \ker u \cap I \subseteq \ker u^{r} \cap I = \{0\}, so u∣Iu|_I is an injective endomorphism of the finite-dimensional II, hence bijective (Corollary 20.9).

21. Let x=a+bx = a + b with a∈Na \in N, b∈Ib \in I. Then u(x)=u(a)+u(b)u(x) = u(a) + u(b) with u(a)∈Nu(a) \in N and u(b)∈Iu(b) \in I (question 20): this is the decomposition of u(x)u(x), so π(u(x))=u(a)=u(π(x))\pi(u(x)) = u(a) = u(\pi(x)): πu=uπ\pi u = u\pi.

22. u2(x,y,z)=u(y,0,z)=(0,0,z)u^2(x,y,z) = u(y, 0, z) = (0, 0, z) and u3(x,y,z)=u(0,0,z)=(0,0,z)=u2(x,y,z)u^3(x,y,z) = u(0,0,z) = (0,0,z) = u^2(x,y,z). Kernels: ker⁡u={y=z=0}=Vect⁡(e1)\ker u = \{y = z = 0\} = \operatorname{Vect}(e_1), ker⁡u2={z=0}=Vect⁡(e1,e2)\ker u^2 = \{z = 0\} = \operatorname{Vect}(e_1, e_2), ker⁡u3=ker⁡u2\ker u^3 = \ker u^2: stabilization at r=2r = 2. Images: im⁡u=Vect⁡(e1,e3)\operatorname{im} u = \operatorname{Vect}(e_1, e_3), im⁡u2=Vect⁡(e3)\operatorname{im} u^2 = \operatorname{Vect}(e_3). Fitting: R3=Vect⁡(e1,e2)⊕Vect⁡(e3)\R^3 = \operatorname{Vect}(e_1, e_2) \oplus \operatorname{Vect}(e_3), and π(x,y,z)=(x,y,0)\pi(x, y, z) = (x, y, 0). Check: πu(x,y,z)=π(y,0,z)=(y,0,0)\pi u(x,y,z) = \pi(y, 0, z) = (y, 0, 0) and uπ(x,y,z)=u(x,y,0)=(y,0,0)u\pi(x,y,z) = u(x, y, 0) = (y, 0, 0): equal. On the first factor u(x,y,0)=(y,0,0)u(x, y, 0) = (y, 0, 0), whose square is 00: nilpotent; on the second u(0,0,z)=(0,0,z)u(0,0,z) = (0,0,z): the identity, bijective.

23. If um=0u^m = 0 then ker⁡um=E\ker u^m = E; since kernels are frozen from rr on, ker⁡ur=ker⁡umax⁡(m,r)=E\ker u^{r} = \ker u^{\max(m, r)} = E. Conversely ker⁡ur=E\ker u^{r} = E means ur=0u^{r} = 0. And ker⁡ur=E  ⟺  \ker u^{r} = E \iff the Fitting projector is onto EE along {0}\{0\}, i.e. π=id\pi = \mathrm{id}. Finally r≤nr \leq n (question 18) gives: every nilpotent endomorphism satisfies un=0u^{n} = 0 — the nilpotency index never exceeds the dimension.

24. Let mm be a nilpotency index of u∣Au|_A: A⊆ker⁡um⊆ker⁡umax⁡(m,r)=ker⁡urA \subseteq \ker u^{m} \subseteq \ker u^{\max(m,r)} = \ker u^{r}. Since u∣Bu|_B is bijective, B=u(B)=uk(B)⊆im⁡ukB = u(B) = u^{k}(B) \subseteq \operatorname{im} u^{k} for every kk, in particular B⊆im⁡urB \subseteq \operatorname{im} u^{r}. Then

n=dim⁡A+dim⁡B≤dim⁡ker⁡ur+dim⁡im⁡ur=n:n = \dim A + \dim B \leq \dim\ker u^{r} + \dim\operatorname{im} u^{r} = n :

both inclusions are equalities of dimensions, hence of subspaces: A=ker⁡urA = \ker u^{r}, B=im⁡urB = \operatorname{im} u^{r}.

25. (i) Part III is a dictionary: splittings E=F1⊕⋯⊕FkE = F_1 \oplus \dots \oplus F_k correspond exactly to families of projectors with ∑pi=id\sum p_i = \mathrm{id} and pipj=0p_i p_j = 0, the FiF_i being the images. (ii) For k=3k = 3 the complements id−pi\mathrm{id} - p_i are themselves projectors, which closed the argument with no extra hypothesis; for general kk one needs ∑irk⁡pi≤n\sum_i \operatorname{rk} p_i \leq n, an inequality the Year 2 trace gives for free (tr⁡p=rk⁡p\operatorname{tr} p = \operatorname{rk} p for a projector, and traces add up to tr⁡id=n\operatorname{tr} \mathrm{id} = n). (iii) Exercise 20.7 is Fitting’s lemma in the already-stabilized case r≤1r \leq 1; in general one lets the kernel and image chains freeze, which takes at most nn steps. (iv) In the Year 2 volume, applied to u−λ idu - \lambda\, \mathrm{id}, the nilpotent factor becomes the generalized eigenspace at λ\lambda and the projectors of Part III become the spectral projectors of the reduction theory. The theorem of Part IV is Fitting’s lemma.

Terms defined in this chapter

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