Section 2 Flashcards

1
Q
A

h/2π (reduced Planck constant)

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2
Q

A wave that describes an electron should have

A

And p=mv

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3
Q

Simple, planewave

A
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4
Q

Energy of free electron in empty space

A
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5
Q

(Time dependent) Schrödinger equation

A

Simplest equation to describe free plane wave

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6
Q
A
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7
Q
A
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8
Q

Schrodinger’s equation of motion under a potential

A
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9
Q
A

-(e^2)/x

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10
Q
A
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11
Q
A

Quantum state of particle

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12
Q
A
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13
Q
A

Sqrt(2pi)

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14
Q

Normalisable, functions have

A
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15
Q
A
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16
Q
A
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17
Q
A
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18
Q

At a time t, uncertainty of position of plane wave approximated by

A
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19
Q

Heisenberg’s uncertainty, principle

A
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20
Q

Free Schrödinger equation can be used to determine

A

Wave function for all t starting with t=0 and

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21
Q

Probability density of a wave function is

A

Gaussian and centred at x-_0(t)

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22
Q

The centre of the probability density of a wave function moves with?

A

Velocity (classical velocity of particle)

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23
Q

For large times, how to deal with uncertainty of x

A

Ignore initial uncertainty and let

24
Q

After a large time t, particles coordinates x_i wil most likely be in

A

(That p_1 should be p_i)

25
Q

Linear operator for momentum

A
26
Q

Let p^ _i act on the wave function of a plane wave

A

(As this wave a definite momentum p- ψ is just multiplied by the value of p_i

27
Q

A wave function ψ is an eigenfunction function of Ο^ if ? What does that mean then?

A

With eigenvalue Ο€ R
This means that the observable described by Ο^ has a definite value in the state described by ψ

28
Q

Expectation of Ο^ in a normalised state given

A

Where Ο^ is general observable

29
Q

Rewrite Schrödinger equation using operators

A
  • use momentum linear operator (63)
30
Q

What does the Hamiltonian operator do

A

Generalises the classical expression below

31
Q

What is the Hamiltonian operator (equation)

A
32
Q

Hermitian operator

A
33
Q

Prove momentum operator is Hermitian

A

Integration by parts to get 2nd last line

34
Q

Compute time derivative of normalisation condition

A

Given that
the Hamiltonian (H^) is a Hermitian operator
And
Ψ_1 = Ψ_2 = Ψ

Therefore last line = 0
Therefore norm is constant

35
Q

Conservation of norm is what?

A

As the norm differentiates wrt time to give zero
Norm is constant
Therefore if norm = 1 at one moment of time
It is 1 for all t
Total probability is conserved under time evolution <=> time evolution is unitary

36
Q

What is the commutator

A
37
Q

For any observable operator, the time derivative of its expectation value is given by

A
38
Q

Prove result of time derivative of expectation of any observable operator

A

2.2 is definition of Hermitian
Sub in Hamiltonian for time derivative

39
Q

Commutator of Hamiltonian operator and momentum operator

A
40
Q

How to solve commutator of the Hamiltonian operator and the momentum operator

A
41
Q

Compute commutator of potential of position and momentum operator

A

Where (63) is momentum operator = -ih(d/dx_i) (line through h)

42
Q

Compute commutator of momentum from Hamiltonian and momentum operator

A
43
Q

Combined solution to commutator of Hamiltonian operator and momentum operator

A

(87) is [H^, p^_i] = 1/(2m) [p^2, p^_i] + [U(x-), p^_i]

(91) is [U(x-), p^_i] = ihd(U(x-))/dx_i

44
Q

Time derivative of momentum operator in any state

A

Using commutator of Hamiltonian (first line)
(2.3) formula for time derivative of expectation of any observable operator

45
Q

[H^, x^_i] = ?

A
46
Q

Time derivative of expectation of position operator

A
47
Q

What are Ehrenfest Theorem?

A

Quantum contrast to classical equations of motion (classical below)

48
Q

The Ehrenfest Theorem

A

Just top and bottom equations (middle used to derive bottom)

49
Q

To integrate Gaussian function

A

Sqrt(π*σ)

50
Q
A
51
Q

Process when normalising wave

A

1) integrate abs val
2) let’s abs val equal 1
3) rearrange to isolate A

52
Q

Normalising wave in R3

A

When changing variables to change dx3 to dx just cube entire integral

53
Q

What is this

A

centre of Gaussian distribution of position

54
Q

What is the wave function of a particle likely to be found at t=0 near x=x_0

A
55
Q

What is an operator?

A

Linear map from vector space to self

O: V -> V

56
Q

Prove time Unitarian

A

Using Schrödinger equation at top

57
Q

3 facts about Hermitian operators

A

1) sum of Hermitian operators is Hermitian

2) product of Hermitian operators is Hermitian

3) all R is Hermitian