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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

Riesz Representation Without a Basis: v ⊥ null φ

How does the one-dimensional complement of null φ hand you the vector that represents φ, without choosing a basis of V?


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Your summary note

    1. 1

      Where the representing vector must lie

      Show that φ=φv\varphi = \varphi_vφ=φv​ forces v∈(null⁡φ)⊥v \in (\operatorname{null}\varphi)^\perpv∈(nullφ)⊥, and derive dim⁡(null⁡φ)⊥=1\dim (\operatorname{null}\varphi)^\perp = 1dim(nullφ)⊥=1 for nonzero φ\varphiφ from the fundamental theorem of linear maps and the complement dimension formula.

    2. 2

      Constructing v=φ(w)‾∥w∥2wv = \frac{\overline{\varphi(w)}}{\|w\|^2} wv=∥w∥2φ(w)​​w

      Prove surjectivity: pick nonzero w∈(null⁡φ)⊥w \in (\operatorname{null}\varphi)^\perpw∈(nullφ)⊥, define vvv, derive φ(v)=∥v∥2\varphi(v) = \|v\|^2φ(v)=∥v∥2, then split uuu into a null⁡φ\operatorname{null}\varphinullφ piece plus a multiple of vvv to reach ⟨u,v⟩=φ(u)\langle u, v\rangle = \varphi(u)⟨u,v⟩=φ(u).

    3. 3

      One-to-one and onto, but conjugate-linear over C\mathbf{C}C

      State that v↦φvv \mapsto \varphi_vv↦φv​ is a one-to-one function from VVV onto V′V'V′, and record φλv=λ‾φv\varphi_{\lambda v} = \overline{\lambda}\varphi_vφλv​=λφv​, so the function is linear over R\mathbf{R}R but not over C\mathbf{C}C.

    Attempt 1 of 2