Chapter 1: Review Flashcards

1
Q

Time-Dependent Schrödinger Equation

A
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2
Q

Time-Independent Schrödinger Equation

A
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3
Q

Wavefunction and Hilbert Space

A
  • ψH 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
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4
Q

Definition of Hermitian

A
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5
Q

Hamiltonian Operator H

A
  • H is linear, operator of observable
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6
Q

Hamiltonian for Particle in 3D with no Magnetic Field

A
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7
Q

Hamiltonian for Spin-1/2 Particle

A
  • g ≡ g-factor (≈ 2)
  • µB ≡ Bohr Magneton
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8
Q

Pauli Matrices

A
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9
Q

Canonical Quantization

A
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10
Q

Observable

A
  • For observable A, measurement is eigenstate an
    • ​wavefunction collapses to eigenstate ψn associated with an
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11
Q

Free Particle in 1D

(Overview)

A
  • Hilbert Space: square-integrable functions on R
  • Eigenstates ψk of p continuous, but not normalizable
  • Eigenenergies k = Ekψk
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12
Q

Free Particle in 1D

(Arbitrary State, Orthonormality, Completeness)

A
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13
Q

Free Particle in 1D

(Dispersion Relations)

A
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14
Q

Harmonic Oscillator

(Overview)

A
  • Hilbert Space: square-integrable functions in R
  • Eigenstates ψn and eigenenergies En are discrete
  • Eigenstates expressed as Hermite polynomials
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15
Q

Harmonic Oscillator

(Arbtriary State, Orthonormality, Completeness)

A
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16
Q

Harmonic Oscillator

(Spectrum and Aribtrary State)

A
17
Q

Harmonic Oscillator

(Elegant Solution: Overview)

A
  • Introduce lowering and raising operators
  • Number operator n = aa
  • Hamiltonian expressed in number operator
  • Vacuum state | 0 > exists with eigenvalue λ = 0
  • Arbitrary state formed by applying raising operator to vacuum
18
Q

Harmonic Oscillator

(Elegant Solution: Action of a,a)

A
19
Q

Harmonic Oscillator

(Elegant Solution: Commutation Relations)

A
20
Q

Harmonic Oscillator

(Elegant Solution: Connection to WF)

A

Let x = q/a0

21
Q

Hydrogen Atom

(Overview)

A
  • 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
22
Q

Hydrogen Atom

(Orbits)

A
  • E < 0 → closed orbits
  • E > 0 → hyperbolic orbits