Quantum Theory I: Class Exam 2 for Phys 321, Exams of Physics

A class exam for the phys 321 course, focusing on quantum theory i. The exam consists of three questions, covering topics such as spin-1/2 particles in magnetic fields, spin observables, and particles in infinite square well potentials. Physical constants, useful formulae, and spin state equations are provided.

Typology: Exams

Pre 2010

Uploaded on 08/18/2009

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Phys 321
Fall 2006
Quantum Theory I : Class Exam 2
30 October 2006
Name: Total: /50
Instructions
There are 3 questions on 7 pages.
Show your reasoning and calculations and always motivate your answers.
Physical constants and useful formulae
Charge of an electron e=1.60 ×1019 C
Planck’s constant h= 6.63 ×1034 Js ~= 1.05 ×1034 Js
Mass of electron me= 9.11 ×1031 kg = 511 ×103eV/c2
Spherical coordinates ˆn= sin θcos φˆx+ sin θsin φˆy+ cos θˆz
Spin 1/2 state |+ˆni= cos θ
2|+ˆzi+e sin θ
2|−ˆzi
Spin 1/2 state |−ˆni= sin θ
2|+ˆzi e cos θ
2|−ˆzi
Rotation Generators ˆσn=|+ˆni h+ˆn| |− ˆni h−ˆn|
Rep. in ˆzibasis ˆ
R(ϕn) =
cos ϕ
2isin ϕ
2cos θisin ϕ
2e sin θ
isin ϕ
2e sin θ cosϕ
2+isin ϕ
2cos θ
Zsin (ax) sin (bx) dx=sin ((ab)x)
2(ab)sin ((a+b)x)
2(a+b)if a6=b
Zsin (ax) cos (ax) dx=1
2asin2(ax)
Zsin2(ax) dx=x
2sin (2ax)
4a
Zxsin2(ax) dx=x2
4xsin (2ax)
4acos (2ax)
8a2
Zx2sin2(ax) dx=x3
6x2
4asin (2ax)x
4a2cos (2ax) + 1
8a3sin (2ax)
pf3
pf4
pf5

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Phys 321

Fall 2006

Quantum Theory I : Class Exam 2

30 October 2006

Name: Total: /

Instructions

  • There are 3 questions on 7 pages.
  • Show your reasoning and calculations and always motivate your answers.

Physical constants and useful formulae

Charge of an electron e = − 1. 60 × 10

− 19 C

Planck’s constant h = 6. 63 × 10

− 34

Js ℏ = 1. 05 × 10

− 34

Js

Mass of electron m e

= 9. 11 × 10

− 31

kg = 511 × 10

3

eV/c

2

Spherical coordinates ˆn = sin θ cos φxˆ + sin θ sin φyˆ + cos θ zˆ

Spin 1/2 state |+nˆ〉 = cos

θ

2

|+zˆ〉 + e

iφ sin

θ

2

|−zˆ〉

Spin 1/2 state |−nˆ〉 = sin

θ

2

|+zˆ〉 − e

cos

θ

2

|−zˆ〉

Rotation Generators ˆσn = |+ˆn〉 〈+nˆ| − |−nˆ〉 〈−nˆ|

Rep. in |±zˆ〉 basis

R(ϕn) =

cos

ϕ

2

− i sin

ϕ

2

cos θ −i sin

ϕ

2

e

−iφ sin θ

−i sin

ϕ

2

e

iφ sin θ cos

ϕ

2

  • i sin

ϕ

2

cos θ

sin (ax) sin (bx) dx =

sin ((a − b)x)

2(a − b)

sin ((a + b)x)

2(a + b)

if a 6 = b

sin (ax) cos (ax) dx =

2 a

sin

2 (ax)

sin

2 (ax) dx =

x

sin (2ax)

4 a

x sin

2

(ax) dx =

x

2

x sin (2ax)

4 a

cos (2ax)

8 a

2

x

2

sin

2

(ax) dx =

x

3

x

2

4 a

sin (2ax) −

x

4 a

2

cos (2ax) +

8 a

3

sin (2ax)

This page is intentionally blank.

b) After the particle leaves the magnetic field, the z-component of spin is measured. De-

termine the probability with which the outcome Sz = −ℏ/2 occurs.

/

Question 2

The observables corresponding to components of spin for a spin-1/2 particle are

Sx =

σˆx

Sy =

ˆσy

Sz =

σˆz

where, in terms of representations in the {|+zˆ〉 , |−zˆ〉} basis,

σ x

σ y

0 −i

i 0

σ z

a) Verify that

[

Sy ,

Sx

]

= −iℏ

Sz.

Question 2 continued...

Question 3

A particle of mass m is in an infinite square well potential

V (x) =

0 0 6 x 6 L

∞ otherwise

for which the energy eigenstates are

ψn(x) =

L

sin

nπx

L

0 6 x 6 L

0 otherwise

corresponding to energy eigenvalues

En =

π

2 ℏ

2 n

2

2 mL

2

for n = 1, 2 ,....

a) Consider an ensemble of particles that are prepared so that, at some instant, they are

each in the state

|ψ〉 =

e

iπ/ 4 |ψ 1

e

−iπ/ 4 |ψ 4

The energy of each particle is measured. List the possible outcomes and determine the

probabilities with which they occur.

/