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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

Eigenvectors, T − λI and At Most dim V Eigenvalues

Why does T − λI failing to be injective pin down an eigenvalue, and why can't T have more than dim V of them?


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Your summary note

    1. 1

      Equivalent conditions for λ\lambdaλ to be an eigenvalue

      State the four equivalent conditions on finite-dimensional VVV, prove them from Tv=λv  ⟺  (T−λI)v=0Tv = \lambda v \iff (T - \lambda I)v = 0Tv=λv⟺(T−λI)v=0, and define eigenvectors as the nonzero vectors of null⁡(T−λI)\operatorname{null}(T - \lambda I)null(T−λI).

    2. 2

      The 90∘90^\circ90∘ rotation T(w,z)=(−z,w)T(w, z) = (-z, w)T(w,z)=(−z,w)

      Record that over R\mathbf{R}R it has no eigenvalues, then solve −z=λw-z = \lambda w−z=λw, w=λzw = \lambda zw=λz over C\mathbf{C}C to get λ=±i\lambda = \pm iλ=±i with their eigenvectors.

    3. 3

      Eigenvectors for distinct eigenvalues are linearly independent

      Write the minimal-counterexample proof: take the smallest dependent list, apply T−λmIT - \lambda_m IT−λm​I to the dependence relation, and reach a shorter dependent list.

    4. 4

      At most dim⁡V\dim VdimV distinct eigenvalues

      Deduce the bound from the independence result and the fact that an independent list is no longer than a spanning list.

    Attempt 1 of 2