Chapter 1: Review Flashcards
Time-Dependent Schrödinger Equation

Time-Independent Schrödinger Equation

Wavefunction and Hilbert Space
-
ψ ∈ H Hilbert Space
- __linear, complex vector space
- closed under addition and multiplication
- complete
- scalar/inner product
- can be infinite but with countable set of basis states

Definition of Hermitian

Hamiltonian Operator H
- H is linear, operator of observable

Hamiltonian for Particle in 3D with no Magnetic Field

Hamiltonian for Spin-1/2 Particle
- g ≡ g-factor (≈ 2)
- µB ≡ Bohr Magneton

Pauli Matrices

Canonical Quantization

Observable
- For observable A, measurement is eigenstate an
- wavefunction collapses to eigenstate ψn associated with an

Free Particle in 1D
(Overview)
- Hilbert Space: square-integrable functions on R
- Eigenstates ψk of p continuous, but not normalizable
- Eigenenergies Hψk = Ekψk

Free Particle in 1D
(Arbitrary State, Orthonormality, Completeness)

Free Particle in 1D
(Dispersion Relations)

Harmonic Oscillator
(Overview)
- Hilbert Space: square-integrable functions in R
- Eigenstates ψn and eigenenergies En are discrete
- Eigenstates expressed as Hermite polynomials

Harmonic Oscillator
(Arbtriary State, Orthonormality, Completeness)

Harmonic Oscillator
(Spectrum and Aribtrary State)

Harmonic Oscillator
(Elegant Solution: Overview)
- Introduce lowering and raising operators
- Number operator n = a†a
- Hamiltonian expressed in number operator
- Vacuum state | 0 > exists with eigenvalue λ = 0
- Arbitrary state formed by applying raising operator to vacuum

Harmonic Oscillator
(Elegant Solution: Action of a,a†)

Harmonic Oscillator
(Elegant Solution: Commutation Relations)

Harmonic Oscillator
(Elegant Solution: Connection to WF)
Let x = q/a0

Hydrogen Atom
(Overview)
- Consider electron under Born-Oppenheimer approximation in Coulomb potential
- Eigenstates | lmn > of Hamiltonian with eigenenergies En
- Can express Hamiltponian in terms of angular momentum L2, Lz
- Eigenvalues l,m with radial component n

Hydrogen Atom
(Orbits)
- E < 0 → closed orbits
- E > 0 → hyperbolic orbits