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Linear Algebra Done Right
Vector Spaces
01Complex Numbers as Pairs of Real Numbers02Lists and Fⁿ: Coordinate Addition and a First Proof03Vectors in R², Scalar Multiplication, and FieldsProblem set0/10Problem set 20/10
01Definition of a Vector Space: Fⁿ, F^∞ and Function Spaces02Unique Zero and Inverses, 0v = 0, and the Subspace Test03Sums of Subspaces: The Smallest Subspace Containing Them04Direct Sums: Only One Way to Write ZeroProblem set0/10Problem set 20/10
Finite-Dimensional Spaces
01Linear Combinations, Span, and Finite-Dimensional Spaces02Linear Independence and the Linear Dependence Lemma03Independent Lists Are No Longer Than Spanning ListsProblem set0/10Problem set 20/10
01Bases: Reduce a Spanning List, Extend an Independent List02Dimension: Why Every Basis Has the Same Length03The Dimension of a Sum of Two SubspacesProblem set0/10Problem set 20/10
Linear Maps
01Linear Maps and the Linear Map Lemma: Values on a Basis02Sums, Scalar Multiples and Products of Linear Maps03Null Space, Range, Injectivity and Surjectivity04The Fundamental Theorem of Linear Maps and Linear SystemsProblem set0/10Problem set 20/10
01The Matrix of a Linear Map: Each Column Is Tvₖ02Matrix Operations and Why Multiplication Is Row Times Column03Rows, Columns and Linear Combinations in Matrix Products04Column Rank Equals Row Rank: Column-Row FactorizationProblem set0/10Problem set 20/10
01Invertible Linear Maps: Injective and Surjective02Equal Dimensions: Injective or Surjective Means Invertible03Isomorphic Spaces and the Dimension of L(V, W)04The Matrix of a Vector: M(Tv) = M(T)M(v)05Change of Basis for an Operator: A = C⁻¹BCProblem set0/10Problem set 20/10
01Products of Vector Spaces: When Dimensions Add02Quotient Spaces V/U: Parallel Lines as Vectors03The Quotient Map and V/null T ≅ range TProblem set0/10Problem set 20/10
01The Dual Basis Reads Coefficients and T′ Reverses Arrows02The Annihilator U⁰ and dim U⁰ = dim V − dim U03Null T′ and Range T′ as Annihilators; M(T′) Is the TransposeProblem set0/10Problem set 20/10
Polynomials and Eigenvalues
01Conjugates, |z| and the Complex Triangle Inequality02Zeros, Factors and the Division Algorithm via a Basis03Fundamental Theorem of Algebra and Complete Factorization04Real Polynomials: Linear and Irreducible Quadratic FactorsProblem set0/10Problem set 20/10
01Invariant Subspaces and Eigenvalues: Tv = λv02Eigenvectors, T − λI and At Most dim V Eigenvalues03p(T) and Why Every Complex Operator Has an Eigenvalue04The Minimal Polynomial: Existence, Uniqueness and Computation05Eigenvalues Are the Zeros of the Minimal Polynomial06Why Odd Dimension Forces a Real EigenvalueProblem set0/10Problem set 20/10
01Upper-Triangular Matrices and Invariant Spans02Eigenvalues Sit on the Upper-Triangular Diagonal03The Minimal Polynomial Decides Upper-TriangularityProblem set0/10Problem set 20/10
01Diagonalizable Operators and Direct Sums of Eigenspaces02Four Equivalent Tests for Diagonalizability03Distinct Linear Factors Decide Diagonalizability04The Gershgorin Disk Theorem: Where Eigenvalues Live05Commuting Operators Share a Diagonalizing Basis06Commuting Operators Over C: One Upper-Triangular BasisProblem set0/10Problem set 20/10
Inner Product Spaces
01Inner Products: Why Complex Spaces Need a Conjugate02Norms, Orthogonality and the Pythagorean Theorem03Cauchy-Schwarz and the Triangle InequalityProblem set0/10Problem set 20/10
01Orthonormal Bases: Bessel's Inequality and Parseval02Gram-Schmidt, Orthonormal Bases and Schur's Theorem03Linear Functionals and the Riesz Representation TheoremProblem set0/10Problem set 20/10
01Orthogonal Complements and the Direct Sum V = U ⊕ U⊥02Orthogonal Projection onto U and Why U⊥⊥ = U03Riesz Representation Without a Basis: v ⊥ null φProblem set0/10Problem set 20/10
01The Closest Point Is the Projection: Fitting Sine on [−π, π]02The Pseudoinverse T† and Its Three Inverse-Like Properties03T†w: The Best Approximate Solution of Smallest NormProblem set0/10Problem set 20/10
Operators on Inner Product Spaces
01The Adjoint T*: Moving T into the Second Slot of ⟨Tv, w⟩02Null T* = (range T)⊥ and M(T*) as the Conjugate Transpose03Self-Adjoint Operators: Real Eigenvalues and Real ⟨Tv, v⟩04Normal Operators: ‖Tv‖ = ‖T*v‖ and Orthogonal EigenvectorsProblem set0/10Problem set 20/10

Change of Basis for an Operator: A = C⁻¹BC

How do the matrices of one operator in two different bases relate, and why is the bridge always C⁻¹BC?


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Your summary note

    1. 1

      The identity matrix and invertible square matrices

      Define III and an invertible matrix by AB=BA=IAB = BA = IAB=BA=I, and derive (A−1)−1=A(A^{-1})^{-1} = A(A−1)−1=A and (AC)−1=C−1A−1(AC)^{-1} = C^{-1}A^{-1}(AC)−1=C−1A−1 by direct multiplication.

    2. 2

      M(I)\mathcal{M}(I)M(I) between two bases and its inverse

      Apply the matrix-of-a-product rule with S=T=IS = T = IS=T=I to show the two identity matrices between the uuu- and vvv-bases are mutually inverse, and work the F2\mathbf{F}^2F2 example with basis (4,2),(5,3)(4,2), (5,3)(4,2),(5,3).

    3. 3

      Change-of-basis formula A=C−1BCA = C^{-1}BCA=C−1BC

      Define AAA, BBB and C=M(I,(u1,…,un),(v1,…,vn))C = \mathcal{M}(I, (u_1, \dots, u_n), (v_1, \dots, v_n))C=M(I,(u1​,…,un​),(v1​,…,vn​)), then apply the product rule twice, through M(T,(u1,…,un),(v1,…,vn))\mathcal{M}(T, (u_1, \dots, u_n), (v_1, \dots, v_n))M(T,(u1​,…,un​),(v1​,…,vn​)), to reach A=C−1BCA = C^{-1}BCA=C−1BC.

    4. 4

      M(T−1)=(M(T))−1\mathcal{M}(T^{-1}) = (\mathcal{M}(T))^{-1}M(T−1)=(M(T))−1 in one basis

      State the result for an invertible operator with a single basis throughout, and write its proof by applying the matrix-of-a-product rule to TT−1=T−1T=ITT^{-1} = T^{-1}T = ITT−1=T−1T=I.

    Attempt 1 of 2