Linear algebra Jordon block, Cheat Sheet of Linear Algebra

This document provides detailed and exam-oriented notes on Jordan Blocks and the Jordan Canonical Form, prepared for advanced linear algebra courses and competitive mathematics examinations. Subject / Course: Linear Algebra – Jordan Block & Jordan Canonical Form Level: MSc Mathematics / BSc (Honours) / CSIR-NET / GATE / NBHM / TIFR Syllabus Coverage: As per UGC-NET / CSIR-NET and IIT–NIT MSc Mathematics syllabus Author / Prepared by: MSc Mathematics (NIT)

Typology: Cheat Sheet

2025/2026

Available from 02/03/2026

raj-kumar-sharma-1
raj-kumar-sharma-1 🇮🇳

15 documents

1 / 20

Toggle sidebar

This page cannot be seen from the preview

Don't miss anything!

bg1
Polynomials Associated with a Linear
Operator
Definition 1: Annihilating Polynomial
Let T:VVbe a linear operator on a vector space Vover a field F. A
polynomial p(x)F[x] is called an annihilating polynomial of Tif
p(T) = 0.
It “annihilates” the operator when substituted into it. There can be infinitely
many annihilating polynomials for a given operator.
Definition 2: Characteristic Polynomial
For a square matrix Arepresenting T, the characteristic polynomial of T
(or A) is defined as
χT(x) = det(xI A).
Its roots are the eigenvalues of T. It is always monic and has degree dim V.
Definition 3: Minimal Polynomial
The minimal polynomial mT(x) of Tis the monic polynomial of least
degree such that
mT(T) = 0.
It divides every other annihilating polynomial and contains all eigenvalues
with the largest Jordan block multiplicity.
5 Key Differences Between Them
1. Existence: Annihilating polynomials: infinite, characteristic: unique,
minimal: unique.
2. Degree: characteristic = dim V, minimal dim V, annihilating
minimal degree.
1
pf3
pf4
pf5
pf8
pf9
pfa
pfd
pfe
pff
pf12
pf13
pf14

Partial preview of the text

Download Linear algebra Jordon block and more Cheat Sheet Linear Algebra in PDF only on Docsity!

Polynomials Associated with a Linear

Operator

Definition 1: Annihilating Polynomial Let T : V → V be a linear operator on a vector space V over a field F. A polynomial p(x) ∈ F[x] is called an annihilating polynomial of T if

p(T ) = 0.

It “annihilates” the operator when substituted into it. There can be infinitely many annihilating polynomials for a given operator.

Definition 2: Characteristic Polynomial For a square matrix A representing T , the characteristic polynomial of T (or A) is defined as χT (x) = det(xI − A).

Its roots are the eigenvalues of T. It is always monic and has degree dim V.

Definition 3: Minimal Polynomial The minimal polynomial mT (x) of T is the monic polynomial of least degree such that mT (T ) = 0.

It divides every other annihilating polynomial and contains all eigenvalues with the largest Jordan block multiplicity.

5 Key Differences Between Them

  1. Existence: Annihilating polynomials: infinite, characteristic: unique, minimal: unique.
  2. Degree: characteristic = dim V , minimal ≤ dim V , annihilating ≥ minimal degree.
  1. Monicity: characteristic and minimal are always monic; annihilating need not be.
  2. Roots: characteristic: eigenvalues with algebraic multiplicity, min- imal: eigenvalues with largest Jordan block size, annihilating: may include eigenvalues with arbitrary multiplicity.
  3. Divisibility: minimal divides every annihilating polynomial; charac- teristic is divisible by minimal.

Example for Understanding

Consider the matrix A =

  • Characteristic polynomial:

χA(x) = det(xI − A) = det

x − 2 − 1 0 x − 2

= (x − 2)^2

  • Minimal polynomial: The minimal polynomial must annihilate A and be monic. Here, mA(x) = (x − 2)^2
  • Annihilating polynomial: Any polynomial divisible by (x − 2)^2 annihi- lates A, e.g.

p(x) = (x − 2)^3 , q(x) = (x − 2)^2 (x + 1)

Observation: - The characteristic polynomial gives eigenvalues 2 with algebraic multiplicity 2. - Minimal polynomial also reflects the largest Jordan block size (2 here). - Annihilating polynomials can be many, as long as they contain the minimal polynomial as a factor.

Algebraic Multiplicity (AM) and

Geometric Multiplicity (GM) of

Eigenvalues

  • An eigenvalue may appear multiple times (AM¿1) but have only 1 independent eigenvector (GM=1).
  • For distinct eigenvalues, GM = AM = 1 automatically.
  1. Example

A =

  • Characteristic polynomial:

χA(x) = det(xI − A) = (x − 2)^2 =⇒ AM(2) = 2

  • Eigenspace: Solve (A − 2 I)v = 0:  0 1 0 0

x y

=⇒ y = 0

So eigenspace: span{(1, 0)T^ }, hence GM(2) = 1

  • Observation: AM > GM =⇒ A is not diagonalizable.
  1. Summary Table Eigenvalue AM (root multiplicity) GM (dimension of eigenspace) 2 2 1

Key takeaway: GM ≤ AM, and equality for all eigenvalues ⇐⇒ matrix diagonalizable.

Eigenspace of a Matrix or Linear

Operator

  1. Definition of Eigenspace Let A be a square matrix of order n (or T : V → V a linear operator) and let λ be an eigenvalue of A. The eigenspace corresponding to λ is the set of all eigenvectors associated with λ, together with the zero vector:

Eλ = {v ∈ Fn^ : (A − λI)v = 0}

It is a subspace of Fn, and its dimension is called the geometric multiplic- ity of λ.

  1. Properties of Eigenspace
    1. Eigenspace Eλ is always a subspace of Fn.
    2. Dimension of Eλ = geometric multiplicity of λ: 1 ≤ dim(Eλ) ≤ alge- braic multiplicity.
    3. If λ 1 , λ 2 ,... , λk are distinct eigenvalues, their eigenspaces intersect triv- ially: Eλi ∩ Eλj = { 0 } for i ̸= j.
    4. A matrix is diagonalizable ⇐⇒ the sum of dimensions of all eigenspaces = n.
    5. All eigenvectors corresponding to λ form a basis of Eλ.
  2. Hidden Concepts / Important Points
    • Eigenspace contains the zero vector even though zero is not considered an eigenvector.
    • Geometric multiplicity = number of linearly independent eigenvectors for a given eigenvalue.
    • AM = GM for all eigenvalues =⇒ matrix diagonalizable. If AM > GM for any eigenvalue, matrix is defective.
    • The dimension of an eigenspace determines how “much freedom” we have in choosing eigenvectors for that eigenvalue.
    • Eigenspaces of distinct eigenvalues are linearly independent subspaces.
  3. Example

A =

Each Jki (λ) is a Jordan block of size ki:

Jk(λ) =

λ 1 0 · · · 0 0 λ 1 · · · 0 0 0 λ

0 0 · · · 0 λ

k×k —

  1. Rules and Conditions
    1. Every eigenvalue λ appears on the diagonal of JCF.
    2. The number of Jordan blocks corresponding to λ = geometric multi- plicity (GM) of λ.
    3. The sum of sizes of Jordan blocks for λ = algebraic multiplicity (AM) of λ.
    4. If AM = GM for all eigenvalues, then JCF = diagonal matrix.
    5. Size of largest Jordan block for λ = degree of λ in the minimal poly- nomial.

  1. Stepwise Method to Find JCF
    1. Find the characteristic polynomial χA(λ) = det(A − λI).
    2. Find all eigenvalues and their algebraic multiplicities (AM).
    3. For each eigenvalue λ, find the nullity of (A − λI) =⇒ geometric multiplicity (GM).
    4. Construct Jordan blocks: - Number of blocks = GM. - Total size of blocks = AM.
    5. Determine sizes of blocks by studying dim ker((A − λI)k) for k = 1 , 2 ,... until it stabilizes.
    6. Assemble blocks in block-diagonal form = JCF.
  1. Important Points and Hidden Concepts
    • JCF is unique up to reordering of Jordan blocks.
    • The minimal polynomial of A tells the largest Jordan block size for each eigenvalue.
    • Diagonalizability ⇐⇒ every Jordan block is 1 × 1.
    • JCF gives complete structural information about a linear operator: spectrum, AM, GM, minimal polynomial.
    • Even if A is not diagonalizable, JCF provides the “nearest diagonal form”.

  1. Example

A =

Step 1: Characteristic polynomial:

det(A − λI) = (5 − λ)^3

Eigenvalue: λ = 5, Algebraic multiplicity = 3. Step 2: Geometric multiplicity: Solve (A − 5 I)v = 0:

(A − 5 I) =

Rank = 2, so nullity = 1. Thus GM = 1. Step 3: Jordan block structure: AM = 3, GM = 1 =⇒ only 1 block of size 3. So JCF is:

J =

  1. Summary
  1. Algebraic multiplicities (AM) must satisfy

AM(1) + AM(2) = 4,

with AM(1) ≥ GM(1) = 1 and AM(2) ≥ GM(2) = 2. The only possibilities are

(AM(1), AM(2)) = (1, 3) or (2, 2).

(Values like (3, 1) are impossible because AM(2) ≥ 2.)

  1. Now determine Jordan block structures consistent with the AM and GM data. Recall: - The number of Jordan blocks for eigenvalue λ equals GM(λ). - The sum of sizes of those blocks equals AM(λ).
  2. Case 1: (AM(1), AM(2)) = (1, 3). Since GM(1) = 1 and AM(1) = 1, the blocks for eigenvalue 1 consist of one 1 × 1 block J 1 (1) = [1]. For eigenvalue 2: GM(2) = 2 so there are two Jordan blocks whose sizes sum to 3. The only possibility (up to ordering) is block sizes 2 and 1. Thus the Jordan form is

J ∼ diag

J 1 (1), J 2 (2), J 1 (2)

i.e. (upper-triangular) matrix

J =

 (rows/columns permuted so blocks appear in this order).

  1. Case 2: (AM(1), AM(2)) = (2, 2). Here GM(1) = 1 but AM(1) = 2, so there must be a single Jordan block of size 2 for eigenvalue 1 (one block because GM=1, total size=2). For eigenvalue 2, AM(2) = 2 and GM(2) = 2, so there are two 1 × 1 blocks for 2. Thus the Jordan form is

J ∼ diag

J 2 (1), J 1 (2), J 1 (2)

i.e.

J =

 (after suitable permutation of basis).

Final Answer (all possible upper-triangular Jordan forms).

Exactly two similarity-types (up to reordering of Jordan blocks) are possible:

diag

J 1 (1), J 2 (2), J 1 (2)

or diag

J 2 (1), J 1 (2), J 1 (2)

(Here Jk(λ) denotes the k × k Jordan block with λ on the diagonal and 1’s on the superdiagonal.)

Remark. Which of these two actually occurs depends on the algebraic multiplicities; the data given (only GM for λ = 1 and range-dimension for T − 2 I) permit both possibilities.

Question & Solution

Problem. Let M be a 7 × 7 real matrix with characteristic polynomial

cM (x) = (x − 1)α(x − 2)β^ (x − 3)^2 , α > β.

Suppose

rank(M − I 7 ) = rank(M − 2 I 7 ) = rank(M − 3 I 7 ) = 5.

If mM (x) is the minimal polynomial of M , find the value of mM (5).

Solution.

We proceed stepwise.

  1. From the ranks given, for each λ ∈ { 1 , 2 , 3 } we have

dim ker(M − λI) = 7 − rank(M − λI) = 7 − 5 = 2.

Hence the geometric multiplicities are

GM(1) = GM(2) = GM(3) = 2.

Question & Answer (with

explanation)

Problem. Let T : C^7 → C^7 be a C-linear operator whose eigenvalues are 2, 3 , 5. Define

W := { v ∈ C^7 : (T − 5 I)kv = 0 for some k > 0 }

(so W is the generalized eigenspace for the eigenvalue 5). Suppose

(T − 2 I)^2 (T − 3 I)^2 (T − 5 I)^2 = 0.

Which of the following statements are necessarily true?

  1. T has at least four linearly independent eigenvectors.
  2. dim W ≥ 2.
  3. ker((T − 2 I)^2025 ) = ker((T − 2 I)^2026 ).
  4. (T − 2 I)(T − 3 I) is a nilpotent operator.

Solution and reasoning. Write the algebraic multiplicities of the eigenvalues 2, 3 , 5 as a 2 , a 3 , a 5. They are positive integers with

a 2 + a 3 + a 5 = 7.

The relation (T − 2 I)^2 (T − 3 I)^2 (T − 5 I)^2 = 0 implies that the size of every Jordan block for each eigenvalue is at most 2. In other words, for each eigenvalue λ ∈ { 2 , 3 , 5 } every Jordan block has size 1 or 2.

Key observation (blocks vs geometric multiplicity). If an eigenvalue λ has algebraic multiplicity aλ and each Jordan block has size ≤ 2, then the minimum possible number of Jordan blocks for λ is la λ 2

m ,

because we can pack at most two eigenvalues into a single 2×2 Jordan block. The geometric multiplicity (number of linearly independent eigenvectors) for λ equals the number of Jordan blocks for λ.

(1) T has at least four linearly independent eigenvectors. — True. The total number of linearly independent eigenvectors (sum of geometric multiplicities) is at least (^) X

λ∈{ 2 , 3 , 5 }

la λ 2

m .

We must minimize this sum subject to a 2 + a 3 + a 5 = 7 and ai ≥ 1. Evaluate possibilities: (a 2 , a 3 , a 5 )

P

⌈ai/ 2 ⌉ example (3, 2 , 2) 2 + 1 + 1 = 4 gives 4 (4, 2 , 1) 2 + 1 + 1 = 4 gives 4 (5, 1 , 1) 3 + 1 + 1 = 5 gives 5

One checks there is no distribution summing to 7 with all ai ≥ 1 that yields a sum < 4. Hence the total geometric multiplicity is ≥ 4. Thus statement (1) is necessarily true.

(2) dim W ≥ 2. — Not necessarily true. The dimension dim W equals the algebraic multiplicity a 5 of the eigenvalue

  1. From a 2 + a 3 + a 5 = 7 with each ai ≥ 1, it is possible to have a 5 = 1 (for instance try (a 2 , a 3 , a 5 ) = (4, 2 , 1)). That choice is compatible with the block-size constraint (one can take two 2×2 blocks for eigenvalue 2, one 2× 2 block for 3, and one 1 × 1 block for 5, etc.). Hence dim W might be 1, so (2) is not necessarily true. (Counterexample: choose algebraic multiplicities (4, 2 , 1).)

(3) ker((T − 2 I)^2025 ) = ker((T − 2 I)^2026 ). — True. For any eigenvalue λ, the chain of subspaces ker((T − λI)k) stabilizes once k reaches the size of the largest Jordan block for λ. Here every Jordan block for eigenvalue 2 has size ≤ 2, so the kernel stabilizes at exponent 2. Therefore for all integers m ≥ 2 we have

ker((T − 2 I)m) = ker((T − 2 I)^2 ).

In particular, ker((T − 2 I)^2025 ) = ker((T − 2 I)^2026 ). Thus (3) is necessarily true.

(4) (T − 2 I)(T − 3 I) is nilpotent. — Not necessarily true. The operator (T − 2 I)(T − 3 I) is a polynomial in T. An operator is nilpotent iff 0 is its only eigenvalue. If v is an eigenvector of T with eigenvalue λ ∈ { 2 , 3 , 5 }, then (T − 2 I)(T − 3 I)v = (λ − 2)(λ − 3) v.

  1. Step 1: Compute eigenvalues - Solve det(λI −A) = 0 - Eigenvalues and their algebraic multiplicities must match.
  2. Step 2: Compute geometric multiplicities - For each eigenvalue λ, compute dim ker(A − λI) - Number of Jordan blocks for λ = geometric multiplicity.
  3. Step 3: Determine nilpotency / Jordan block sizes - For each eigenvalue λ, compute the sequence:

dim ker((A − λI)k), k = 1, 2 ,...

  • The ”jumps” in dimensions determine the sizes of Jordan blocks. - For nilpotent matrices (all eigenvalues = 0), the largest Jordan block size = nilpotency index (smallest p such that Ap^ = 0).
  1. Step 4: Check minimal polynomial - Minimal polynomial gives the size of the largest Jordan block for each eigenvalue.
  2. Step 5: Compare rank (optional check) - Rank can help quickly identify Jordan structure for nilpotent matrices.

— Solution: Step-by-step check of options Target matrix T : - Eigenvalues = 0 (AM = 3) - Nilpotency index = 2 (T 2 = 0) - Rank = 1

  • Option 1: M 1 =

 (^) M 12 = 0, rank = 1 → Same JCF

  • Option 2: M 2 =

 (^) M 22 = 0, rank = 1 → Same JCF

  • Option 3: M 3 =

 (^) M 32 = 0, rank = 1 → Same JCF

  • Option 4: M 4 =

 (^) M 42 ̸= 0, nilpotency index = 3 → Does

NOT match JCF

Conclusion:

Matrices with the same Jordan canonical form as T are: M 1 , M 2 , M 3.

Exam Tip:

  • For nilpotent matrices, always check Ap^ = 0 to determine the largest Jordan block.
  • Eigenvalues alone are not enough to determine JCF.
  • Rank and minimal polynomial help quickly verify JCF for nilpotent matrices.

Question & Detailed Solution

Question. Let T : R^4 → R^4 be a linear transformation with

χT (x) = (x − 2)^4 , mT (x) = (x − 2)^2.

Which one of the following matrices can represent the Jordan canonical form of T?

(A)

(two 2 × 2 Jordan blocks)

(B)

(one 2 × 2 block and two 1 × 1 blocks)

This is exactly two 2 × 2 Jordan blocks J 2 (2) ⊕ J 2 (2). - Largest block size = 2 ⇒ minimal polynomial has factor (x − 2)^2. - Algebraic multiplicity = 4 (two blocks of size 2). Hence (A) is valid.

(B) (^) 

  

This is one 2 × 2 block plus two 1 × 1 blocks: J 2 (2) ⊕ 2 ⊕ 2. - Largest block size = 2 ⇒ minimal polynomial (x − 2)^2. - Algebraic multiplicity = 4. Hence (B) is valid.

(C) (^) 

  

This is a single 4 × 4 Jordan block J 4 (2). - Largest block size = 4 ⇒ minimal polynomial would be (x − 2)^4 , which contradicts mT = (x − 2)^2. Hence (C) is not valid.

(D)

2 I 4 =

This is four 1 × 1 Jordan blocks. - Largest block size = 1 ⇒ minimal polyno- mial would be (x − 2), contradicting mT = (x − 2)^2. Hence (D) is not valid.

Final answer: (A) and (B) only.

Exam tips / hidden checks:

  • χT fixes algebraic multiplicities; mT fixes the maximal Jordan-block size.
  • Compare degrees: deg mT = size of largest Jordan block for each eigen- value.
  • If the minimal polynomial degree equals the degree of the characteristic polynomial for that eigenvalue, a single largest block of that size is forced.
  • Always rule out (i) a single large block that would make deg mT too big, and (ii) a purely diagonal form that would make deg mT too small.