Quantum Theory Flashcards

1
Q

Quantum Theory

What are the De Broglie relations and when do they apply (D)

A

E=hw (Energy, constant, angular frequency)
p=hk (Momentum vector, constant, wave vector)

They apply for a free particle (no forces / V=0)

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2
Q

Quantum Theory

What is the Schrodinger equation? (D)

A

ih * βˆ‚π›Ή/βˆ‚t = - h^2 / 2m * βˆ‡^2𝛹 + V𝛹

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3
Q

Quantum Theory

What is the stationary state Schrodinger equation? (D)

A
  • h^2 / 2m * βˆ‡^2πœ“+Vπœ“=Eπœ“
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4
Q

Quantum Theory

How do you arrive at the stationary state equation from the Schrodinger equation? (Q)

A

You look for separable solutions. Let 𝛹(x,t)=πœ“(x)T(t) and divide by it to get:

( ih dT/dt ) / T
= ( - h^2 / 2m * βˆ‡^2πœ“ + Vπœ“ ) / πœ“
= constant
= E

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5
Q

Quantum Theory

What is the one-dimensional Schrodinger equation? (D)

A

ih * βˆ‚π›Ή/βˆ‚t = - h^2 / 2m * βˆ‚^2𝛹/dx^2 + V𝛹

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6
Q

Quantum Theory

What is the one-dimensional stationary state Schrodinger equation? (D)

A
  • h^2 / 2m * d^2πœ“/dx^2 + Vπœ“ = Eπœ“
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7
Q

Quantum Theory

What are the stationary state solutions and associated energies of the one-dimensional particle in a box? (Q)

A

πœ“n(x)=Bsin(npix/a)

Energy: En=n^2 pi^2 h^2 / 2ma^2

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8
Q

Quantum Theory

What are the wave functions of the one-dimensional particle in a box? (Q)

A

𝛹n(x,t)=Bsin(npix/a) * e^( -i n^2 pi^2 h t / 2 m a^2 )

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9
Q

Quantum Theory

What is the ground state energy? (D)

A

When the possible energies of a quantum system are discrete and bounded below, the ground state energy is the smallest energy state

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10
Q

Quantum Theory

What are the stationary state solutions and associated energies of the three-dimensional particle in a box? (Q)

A

πœ“n1,n2,n3(x,y,z)= Bsin(n1pix/a)sin(n2piy/b)sin(n3piz/c)

With energies En1,n2,n3
= pi^2 h^2 / 2m ( n1^2/a^2 + n2^2/b^2 + n3^2/c^2 )

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11
Q

Quantum Theory

What does it mean to say an energy level E has d-fold degeneracy? (D)

A

It means the space of solutions to the stationary state schrodinger equation with energy level E has a dimension d>1. When d=1 we call E a non-degenerate energy state

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12
Q

Quantum Theory

What is the correspondence principle? (D)

A

The tendency for quantum results to tend to the classical result as the quantum number tends to ∞ (as the energy of the system increases)

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13
Q

Quantum Theory

What is the probability density function for the particles position? (D)

A

The square of the magnitude of the wave function

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14
Q

Quantum Theory

What does it mean for a wave function to be normalised? (D)

A

For the integral over all space of the magnitude square of the wave function to be equal to 1

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15
Q

Quantum Theory

What does it mean for a wave function to be normalisable? (D)

A

For the integral over all space of the magnitude square of the wave function to be strictly between 0 and ∞

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16
Q

Quantum Theory

What is the continuity equation? (D)

A

βˆ‚Ο/βˆ‚t + βˆ‡Β·j = 0

17
Q

Quantum Theory

What is the probability current j? (D)

A

j(X,t) = ih / 2m ( 𝛹*conj(βˆ‡π›Ή)-conj(𝛹)βˆ‡π›Ή )

18
Q

Quantum Theory

What’s the rough proof of the continuity equation? (T)

A

Note ¦𝛹(x,t)Β¦^2 = conj(𝛹)𝛹.
Differentiate with product rule
Expand with Schrodinger
Then collect terms and note βˆ‡^2 = βˆ‡Β·βˆ‡

19
Q

Quantum Theory

What is the condition for int[R^3] ¦𝛹¦^2 dxdydz to be independent of t? (T)

A

j must tend to 0 faster than 1/¦x¦^2 as ¦x¦ ->∞

20
Q

Quantum Theory
Prove the theorem that if j tends to 0 faster than 1/Β¦xΒ¦^2 as Β¦xΒ¦ -> ∞. Then the integral of R^3 of ¦𝛹¦^2 is independent of time. (T)

A

Idea of proof if to look at the derivative of the integral of a general space D with border S. Use continuity. Divergence. Then transform to spherical. Let S be sphere and show it tends to 0 as r->∞.
Proof in Chapter 3 notes

21
Q

Quantum Theory

3 conditions on solutions to the Schrodinger equation? (Q)

A

The wave function should be a continuous, single valued function. This means the probability density is single-valued with no discontinuities

The wave function should be normalisable

βˆ‡π›Ή should be continuous everywhere, except when there is an infinite discontinuity in V. This follows as discontinuity in βˆ‡π›Ή => infinite discontinuity in βˆ‡^2𝛹 => infinite discontinuity in V from Schrodinger

22
Q

Quantum Theory

When solving an IVP for a particle in a box, how to you calculate the coefficients cn? (Q)

A

[0]int[a] f(x)πœ“m(x) dx = [n=1]sum[∞] ( cn * [0]int[a] πœ“n(x)πœ“m(x) dx ) = cm

Since [0]int[a] πœ“mπœ“n dx = 0 as they are orthogonal
The 2nd equality comes from the fourier series for f(x)

23
Q

Quantum Theory

What is the probability of measuring the energy of the particle to be En? (Q)

A

¦cn¦^2

24
Q

Quantum Theory

Show [n=1]sum[∞] ¦cn¦^2 = 1 (T)

A

1
= [0]int[a] ¦𝛹¦^2 dx
= [m,n=1]sum[∞] of conj(cm)cn * e^-i(En-Em)t/h * [0]int[a] conj(πœ“m)πœ“n dx
= [n=1]sum[∞] ¦cn¦^2

2nd equality from series expansion of 𝛹. 3rd equality since πœ“ is real