physics2u
Depth
Unit · year 1

PU-104 · Mathematical Methods I — Linear Algebra & Operators

Threads symmetry · waves · matter · chance30 lectures17 derivations

This unit builds the linear-algebraic machinery on which all of quantum mechanics, normal-mode analysis, and modern classical mechanics rest: vector spaces, inner products, linear operators, and above all the spectral theory of self-adjoint operators. Starting from abstract axioms and ending with the spectral theorem and its physical incarnations, it teaches the student to see eigenvalue problems, orthogonal decompositions, and unitary symmetries as one coherent structure.

PREREQUISITES

PU-101, PU-103

Lectures

L01
—
L02
L03
L04
L05
L06
L07
L08
L09
L10
L11
L12
L13
L14
L15
L16
L17
L18
L19
L20
L21
L22
L23
L24
L25
L26
L27
L28
L29
L30

Derivations homed in this unit

D-074

Invariance of Dimension of a Vector Space

Any two bases of a finite-dimensional vector space have the same cardinality, so dimension is well-defined.

D-075

Gram–Schmidt Orthonormalization

Any linearly independent set in an inner-product space can be converted into an orthonormal set spanning the same subspace.

D-076

Cauchy–Schwarz and the Triangle Inequality

The inner product bounds |⟨u,v⟩| ≤ ‖u‖‖v‖, from which the norm's triangle inequality follows.

D-077

Existence and Uniqueness of the Adjoint

Every linear operator on a finite-dimensional inner-product space has a unique adjoint defined by ⟨Au,v⟩=⟨u,A†v⟩.

D-078

Riesz Representation in Finite Dimensions

Every linear functional on a finite-dimensional inner-product space is inner product with a unique fixed vector.

D-018 verified

Properties of Hermitian Operators

Hermitian operators have real eigenvalues and mutually orthogonal eigenvectors for distinct eigenvalues.

D-079

Determinant as the Unique Alternating Multilinear Form

The determinant is the unique normalized alternating multilinear function of columns, giving det(AB)=det(A)det(B).

D-080

Eigenvalues as Roots of the Characteristic Polynomial

The eigenvalues of an operator are exactly the roots of det(A−λI), which is basis-independent.

D-081

Diagonalizability and the Eigenbasis Criterion

An operator is diagonalizable iff its eigenvectors span the space, equivalently algebraic equals geometric multiplicity.

D-082

Spectral Theorem for Self-Adjoint Operators

Every self-adjoint operator admits an orthonormal eigenbasis and is diagonalized by a unitary transformation.

D-083

Unitary Operators as Inner-Product Isometries

An operator preserves the inner product iff it is unitary (U†U=I), and its eigenvalues lie on the unit circle.

D-084

Simultaneous Diagonalization of Commuting Operators

Two commuting self-adjoint operators share a common orthonormal eigenbasis.

D-085

Normal Modes from the Generalized Eigenvalue Problem

Coupled small oscillations reduce to the generalized problem Kx=ω²Mx with M-orthogonal normal modes.

D-086

Variational Characterization of Eigenvalues

The extrema of the Rayleigh quotient are the eigenvalues, giving the min-max principle for self-adjoint operators.

D-087

Singular Value Decomposition

Any linear map factors as A=UΣV† with orthonormal bases and non-negative singular values.

D-088

Matrix Exponential and One-Parameter Flows

exp(tA) is the unique solution operator of ẋ=Ax, with self-adjoint generators producing unitary flows.

D-089

Orthogonal Projections and Spectral Resolution

Self-adjoint idempotents are orthogonal projectors, and the spectral theorem resolves the identity into them.