
Essential Student Algebra: Volume Four, Linear Algebra
T. S. Blyth & E. F. Robertson · First-year university · Study material generated by AI from this edition. Not affiliated with the publisher.

T. S. Blyth & E. F. Robertson · First-year university · Study material generated by AI from this edition. Not affiliated with the publisher.
Chapter 4 · pp. 54–67
A linear map may have eigenvalues that do not lie in the ground field, so the Jordan form is not always available. This chapter builds a canonical matrix that works over any field and reduces to the Jordan form when all eigenvalues are in . The main tools are quotient spaces, cyclic subspaces, and the Cyclic Decomposition Theorem.
The minimum polynomial of a linear map is a product of powers of irreducible polynomials. Those irreducible factors need not be linear, so the eigenvalues may lie outside the ground field (p. 54). Over , the factor is irreducible but has no real root. A map with this factor has no Jordan form over (p. 54). We therefore need a canonical matrix that does not depend on roots being present.
Let be a subspace of . The quotient space is the set of cosets . Addition is and scalar multiplication is (p. 54). Two vectors give the same coset exactly when their difference lies in . With these operations is a vector space over . Example: take and the -plane. Each coset is a plane parallel to , and the -coordinate identifies it (p. 54).
Suppose is finite-dimensional, is a basis of , and is a basis of . Then is a basis of (p. 55). The map is linear, so independent cosets give independent representatives. For spanning, take any and write . Then lies in , so it is a combination of the (p. 55).
Counting basis vectors gives
For example, if and , then (p. 55).
If , then is isomorphic to . Both have dimension , and finite-dimensional spaces over of equal dimension are isomorphic (p. 55).
Let be -invariant. The induced map is defined by (pp. 56–57). It is well defined: if , then , so by invariance. It is linear because is. Without invariance, different representatives of one coset could give different answers (pp. 56–57).
The minimum polynomial of divides that of . By induction , so for every polynomial . Taking gives , hence (p. 56).
For a non-zero , the -cyclic subspace is the set of all vectors with . It is an -invariant subspace (p. 57). Example: let and . Then and , so (p. 57).
The -annihilator of a vector is the monic polynomial of least degree with . It comes from the least for which is a combination of . In the example above, gives (p. 57).
If , then is a basis of , so (p. 58). These vectors are independent by minimality of . Every higher power is a combination of them, by induction using (p. 58).
Relative to the basis , the induced map on has the companion matrix of . It has ones on the subdiagonal, last column , and zeros elsewhere (pp. 58–59). Each basis vector except the last goes to the next one, which gives the subdiagonal. The last vector goes to , which gives the last column. For the matrix is (pp. 58–59).
The minimum polynomial of equals . It divides , and its degree is at least , since otherwise would be a combination of earlier vectors. Because is a restriction of , its minimum polynomial divides that of . So the annihilator of any vector divides . The same argument works in a quotient , using (pp. 58–59).
A cyclic vector is a vector whose cyclic basis spans . A subspace with such a basis is a cyclic subspace. On it, has the companion matrix of the annihilator of . Cyclic subspaces are the building blocks of the rational form (p. 59).
Suppose has minimum polynomial with irreducible. Then , where has annihilator and each (pp. 59–61). So the matrix of is block diagonal, with each block the companion matrix of . Example: for , and , splits into two 2-dimensional cyclic pieces (pp. 59–61).
The proof is by induction on (pp. 60–61):
Since , we get
For and , this means (p. 61).
The integers are determined by (p. 62). Let . The image of under has dimension if , and otherwise. Summing,
The left side depends only on , so the number of is fixed for every . That fixes the whole sequence (p. 62).
The polynomials are the elementary divisors of . The first, , is the minimum polynomial. Repeats are allowed, and a repeated divisor means its companion matrix appears more than once (p. 63).
To build it (p. 63):
Each gives a block , itself block diagonal in companion matrices of the divisors . The result is unique up to the order of the . Each has size , where is the multiplicity of in the characteristic polynomial (p. 63).
Example: if has minimum polynomial , the characteristic polynomial is . Then with and all forces and . The form is (p. 64).
Mistake 1: the characteristic and minimum polynomials determine the form. They do not. Let on have minimum polynomial and characteristic polynomial . The part has dimension 4 with . Both and are possible, giving two different rational forms (p. 64).
Mistake 2: the rational form equals the Jordan form when both exist. Take characteristic and minimum polynomial . The rational form is the single companion matrix of , with last column . This looks nothing like a Jordan block with on the diagonal (p. 65).
Suppose has minimum polynomial with , and is a cyclic vector. The vectors , for and , form a basis of (pp. 65–66). They are independent because a dependence would give a polynomial of degree less than that kills , contradicting minimality of . Relative to this basis, the matrix of is block diagonal with copies of on the diagonal. The blocks sit just above them, where is the matrix with a single in its bottom-left corner. This arises because, for the first vector in a row, gives a combination of that row's vectors plus a vector from the previous row (pp. 65–66).
The classical canonical matrix is obtained from the rational one by replacing each group of companion matrices of with the classical -matrix. Each such block uses the companion matrix of rather than of . For this gives blocks linked by connecting -entries (pp. 66–67).
When , we have , so and . The classical -matrix is the Jordan block with on the diagonal and on the superdiagonal. This is the case where is nilpotent of index . So the classical form reduces to the Jordan form whenever all eigenvalues lie in the ground field (p. 67).