Operators Flashcards

1
Q

Kinetic energy operator

A

T̂ = -ħ²/2m ∂²/∂x²

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2
Q

Potential energy operator

A

V̂ = V(x)

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3
Q

Total energy operator (Hamiltonian)

A

Ĥ = -ħ²/2m ∂²/∂x² + V(x)
T̂ + V̂

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4
Q

Hamiltonian as an eigenvector

A

Ĥψᵢ(x) = Eᵢψᵢ(x)

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5
Q

Eigenvalues and states of an operator, Â

A

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.

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6
Q

Momentum operator

A

p̂ₓ = -iħ ∂/∂x

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7
Q

Position operator

A

x̂ = x

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8
Q

What is the Hermitian conjugate? Define in terms of a pair of wavefunctions Φ and Ψ.

A

For each  operator, an † operator exists such that:
∫ Φ * † Ψ dx = ∫ (ÂΦ) * Ψ dx

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9
Q

What is a Hermitian operator?

A

An operator for which † = Â

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10
Q

Two properties of Hermitian operators?

A
  1. All eigenvalues of a Hermitian operator are real, aka correspond naturally to physical observables.
  2. Eigenfunctions of a Hermitian operator with different eigenvalues are orthogonal, meaning ∫ψᵢ * ψⱼ dx = 0 if aᵢ and aⱼ not equal.
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11
Q

Destruction operator / lowering operator

A

â = √(mω/2ħ) x̂ + i/√(2mωħ) p̂ₓ

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12
Q

Creation opertor / raising operator

A

↠= √(mω/2ħ) x̂ - i/√(2mωħ) p̂ₓ

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13
Q

2D Hamiltonian

A

Ĥ = Ĥₓ + Ĥᵧ
Where Ĥₓ = -ħ²/2m ∂²/∂x² + ½ mω²x²
and Ĥᵧ = -ħ²/2m ∂²/∂y² + ½ mω²y²

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14
Q

Eigenfunctions of the Hamiltonian

A

Ĥψₙ(x) = Eₙψₙ(x)
where Eₙ = (n+½)ħω

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15
Q

What does separability of an operator tell us about its eigenfunctions?
eg  = B̂ + Ĉ

A

Products of the eigenfunctions of B̂ and Ĉ are eigenfunctions of Â

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16
Q

Angular momentum operator

A

L̂ = r̂ x p̂
L̂ᶻ = x̂p̂ᵧ - ŷp̂ₓ
= (-iħ)(x ∂/∂y - y ∂/∂x)
Using plane polar:
L̂ᶻ = -iħ ∂/∂Φ

17
Q

Hamiltonian in terms of position and momentum operators.

A

Ĥ = 1/2m p̂ₓ² + ½ mω²x̂²