Further Quantum Flashcards

1
Q

Define a wave function that doesn’t distinguish between particles

A
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2
Q

Define Qλψ(r1,…,rn)

A
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3
Q

Prove that Qλ satisfies ψ(r1,…,rn) = λ(π)ψ(rπ(1),…,rπ(n)) ∀π∈Sn, and is a projection

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4
Q

What is a boson?

A

When λ(π)=1, spin is integral

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5
Q

Choosing a basis of N separable wave functions, describing n bosons, how many states are there? Prove it

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6
Q

What is a Fermion?

A

When λ(π) = ε(π), spin is not integral

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7
Q

What is the Pauli Exclusion Principle?

A

That no 2 Fermions can simultaneously occupy the same state. Proof as otherwise Qλψ = 0

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8
Q

Choosing a basis of N separable wave functions describing n Fermions, how many states are there? Prove it

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9
Q

What is the Schrödinger Picture?

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10
Q

What is the Heisenberg Picture?

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11
Q

What is the Interaction Picture?

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12
Q

Prove that the expectation is the same in all quantum pictures

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13
Q

By what equations is the time evolution of wave functions and observables governed in the Interaction Picture? Prove it

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14
Q

Use an equation governing time evolution in the interaction picture to set up an expansion for ψt

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15
Q

What is the Feynman-Dyson Expansion? Prove it

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16
Q

What is Fermi’s Golden Rule? Prove it

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17
Q

Set up Rayleigh-Schrödinger Perturbation Theory

A
18
Q

If φ1,…,φD form an orthonormal basis with H0φr = E0φr and ψ0 = Σcrφr, then what? Prove it

A
19
Q

What is the k’th order correction to the energy, E(k)? Prove it

A
20
Q

Prove: <ψu|H’ψv> = (Eu-Ev)/(u-v)

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21
Q

Expand (Eu-Ev)/(u-v)

A
22
Q

If ψα, α=0,1,… is an orthonormal basis such that H0ψα = Eαψ0 and Eα ≠ E0 for α≠0, then what is ψ’ and E’’? Prove it

A
23
Q

Define the Rayleigh Quotient

A
24
Q

For a subset K of the Hilbert Space of wave functions, what is the result behind Variational methods? Prove it

A

d/du(fH(ψ+uφ))|u=0 = 0 ∀φ∈K if and only if <φ|H-fH(ψ)|ψ> = 0 ∀φ∈K ie: Critical value of fH(φ) is an eigenvalue with the critical point being the eigenvector

25
Q

State and prove the Virial Theorem

A
26
Q

Using a Variational approach, if fH(ψ) > -∞, then what is the ground state energy?

A

Eground = infψ∈K{0} fH(ψ), obtained at ψground

27
Q

If ψ0 is the ground state of H0 in {ψu}, prove that Variational methods will give a better approximation for the energy than regular perturbation theory

A
28
Q

What is the k’th lowest energy eigenstate from a Variational point of view?

A

If it is attained, then: infK_k {max{fH(ψ) : ψ∈Kk} : dim(Kk)=k}

29
Q

If Vj is a basis of K, then what provides an upper bound for the k’th lowest energy (k’th lowest eigenvalue of H)? Prove it

A

If Ēk is the k’th lowest root of det(i|HVk> - Ei|Vk>) = 0, then Ēk ≥ Ek