Linear Combination - Quantum Mechanics - Exam, Exams of Quantum Mechanics

This is the Past Exam of Quantum Mechanics which includes Wavefunction for Particle, Valid Wavefunction, Stern Gehrlach Device, Square Barrier, Spin System etc. Key important points are: Linear Combination, One-Dimensional Simple Harmonic Oscillator, Energy Basis, Schrodinger Picture, Expectation Values, Angular Momentum Operators, Function of Time, Simultaneaus Eigenvalues

Typology: Exams

2012/2013

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Midterm Exam
30.Oct.2001
Quantum Mechanics
Intructions:
Please read all questions carefully before attempting to answer them. Write your
name and number on top of every answersheet. No books, calculators or
materials other than blank paper and pencils/pens are allowed on the desks. If
you need a formula or integral from the book to solve an exercise, which you
cannot remember please ask and it will be given to you (for a possible small
point penalty). You have until 19:00 to answer all questions in Swedish or
English. The exam counts for 30% of your total grade (1 point=0.5%).
1.) (15 points) Consider a one-dimensional simple harmonic oscillator. Do the
following algebraically in the energy basis (i.e. without using wavefunctions).
Hint:
ω
ω
m
iP
a
2
/
)
(
+
=
a.) Construct a linear combination of
0
and
1
such that
X
is as large as
possible.
b.) Suppose at t=0 the oscillator is in the state contructed in a.). What is the
state vector for t>0 in the Schrödinger picture?
c.) Evaluate the expectation values
X
and
2
X
as a function of time t>0.
2.) (18 points) Consider the angular momentum operators with the commutation
relations
[
]
,
,
k
ijk
j
i
J
J
ε
=
where i,j,k can be any of the directions x,y,z.
a.) Show that the z-component of the angular momnetum
z
J
and the angular
momentum squared
2
2
2
z
y
x
J
J
+
+
commute with each other and therefore
have simultaneaus eigenvalues m and j(j+1). Show from the
commutation relations of the ladderoperators
y
x
iJ
J
±
=
±
that these
can be used to raise and lower the z-component of the angular
momentum. Derive which are the allowed values for m and j(j+1).
b.) Derive the constants
±
jm
c
in the equations
1
,
,
±
=
±
±
J
jm
. (Result:
)
1
)(
(
+
±
=
±
c
jm
).
c.) Use the result of b.) to explicitly construct the matrix
m
j
j
y
,
'
,
'
,
for
j=j=1 and m,m=-1,0,1. Find the eigenvalues and eigenvectors of
y
J
in
the basis where
z
J
is diagonal.
pf2

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Midterm Exam 30.Oct.2001 Quantum Mechanics

Intructions: Please read all questions carefully before attempting to answer them. Write your name and number on top of every answersheet. No books, calculators or materials other than blank paper and pencils/pens are allowed on the desks. If you need a formula or integral from the book to solve an exercise, which you cannot remember please ask and it will be given to you (for a possible small point penalty). You have until 19:00 to answer all questions in Swedish or English. The exam counts for 30% of your total grade (1 point=0.5%). 1.) (15 points) Consider a one-dimensional simple harmonic oscillator. Do the following algebraically in the energy basis (i.e. without using wavefunctions). Hint: a =( m ω X + iP )/ 2 m ω a.) Construct a linear combination of 0 and 1 such that X is as large as possible. b.) Suppose at t=0 the oscillator is in the state contructed in a.). What is the state vector for t >0 in the Schrödinger picture? c.) Evaluate the expectation values X and X^2 as a function of time t>. 2.) (18 points) Consider the angular momentum operators with the commutation

relations [ J i , Jj ] i ε ijkJk ,

 = where i,j,k can be any of the directions x,y,z. a.) Show that the z-component of the angular momnetum J (^) z and the angular momentum squared J (^) x^2 + Jy^2 + J z^2 commute with each other and therefore have simultaneaus eigenvalues m and j(j+1). Show from the commutation relations of the “ladder” operators J (^) ± = Jx ± iJy that these can be used to raise and lower the z-component of the angular momentum. (^) Derive which are the allowed values for (^) m and (^) j(j+1). b.) Derive the constants c ± jm in the equations J (^) ± j , m = c ± jm j , m ± 1. (Result: c ± jm^ = ( j m )( j ± m + 1 )  ). c.) Use the result of b.) to explicitly construct the matrix j (^) , ', m ' Jy j , m for j’=j=1 and m,m’=-1,0,1. Find the eigenvalues and eigenvectors of J (^) y in the basis where J (^) z is diagonal.

3.) (12 points) A particle of mass M and charge q in a uniform magnetic field B  has a magnetic moment q McL   μ = (^) / 2 and energy H B   =− μ ⋅. The particle is confined to move on the surface of a sphere of radius b. a.) What are the energy eigenstates and eigenvalues of this particle? Calculate the splitting of the energy levels whose angular momentum quantum number is l= 1 due to the magnetic field_._ b.) If the above particle was subjected to an additional interaction proportional to 2 ( L + (^) + L − ) , between which of the states with l= 1 would this interaction cause transitions (i.e. which states are “connected” by this operator). 4.) (8 points) Two angular momentum operators J 1  and J 2  are added together to form the total angular momentum J J 1 J 2    = +. Given that j 1 (^) = 2 and j 2 (^) = 3 / 2 , find the total angular momentum state j = (^5) / 2 , m = 5 / 2 in terms of the product basis j 1 (^) m 1 , j 2 m 2. 5.) (7 points) Explain in words and equations the key concepts of the Schrödinger picture and the Heisenberg picture descriptions of Quantum Mechanics.