Operators Flashcards
Kinetic energy operator
T̂ = -ħ²/2m ∂²/∂x²
Potential energy operator
V̂ = V(x)
Total energy operator (Hamiltonian)
Ĥ = -ħ²/2m ∂²/∂x² + V(x)
T̂ + V̂
Hamiltonian as an eigenvector
Ĥψᵢ(x) = Eᵢψᵢ(x)
Eigenvalues and states of an operator, Â
Âψₙ = aₙψₙ
System in the ψₙ state, Â will always give aₙ
System in ψₙ state will stay in ψₙ state
System in mixed state ψ, Â gives one of the {aₙ} values with expectation ⟨A⟩ = ∫ψ * Âψ dx
Once aₙ measured, system left in ψₙ state.
Momentum operator
p̂ₓ = -iħ ∂/∂x
Position operator
x̂ = x
What is the Hermitian conjugate? Define in terms of a pair of wavefunctions Φ and Ψ.
For each  operator, an † operator exists such that:
∫ Φ * † Ψ dx = ∫ (ÂΦ) * Ψ dx
What is a Hermitian operator?
An operator for which † = Â
Two properties of Hermitian operators?
- All eigenvalues of a Hermitian operator are real, aka correspond naturally to physical observables.
- Eigenfunctions of a Hermitian operator with different eigenvalues are orthogonal, meaning ∫ψᵢ * ψⱼ dx = 0 if aᵢ and aⱼ not equal.
Destruction operator / lowering operator
â = √(mω/2ħ) x̂ + i/√(2mωħ) p̂ₓ
Creation opertor / raising operator
↠= √(mω/2ħ) x̂ - i/√(2mωħ) p̂ₓ
2D Hamiltonian
Ĥ = Ĥₓ + Ĥᵧ
Where Ĥₓ = -ħ²/2m ∂²/∂x² + ½ mω²x²
and Ĥᵧ = -ħ²/2m ∂²/∂y² + ½ mω²y²
Eigenfunctions of the Hamiltonian
Ĥψₙ(x) = Eₙψₙ(x)
where Eₙ = (n+½)ħω
What does separability of an operator tell us about its eigenfunctions?
eg  = B̂ + Ĉ
Products of the eigenfunctions of B̂ and Ĉ are eigenfunctions of Â