Matrix Representations - 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: Matrix Representations, Normalization Constant, Magnetic Field of Strength, Particle with Charge, Basis of Eigenstates, Spin Quantum Number, Spin Hamiltonian, Simultaneous Eigenstates

Typology: Exams

2012/2013

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Introduction to Quantum Mechanics 171.303
Midterm Exam 11/3/05 1-2
Check the attached formula pages. Start each problem on a fresh page and please give
detailed reasoning. Please ask your proctor for clarification if the text is unclear.
Problem 1 (30 points)
Consider a spin-1/2 particle with charge q and mass m, in a magnetic field of strength B
oriented in the z
ˆ direction. At t=0, the particle is in the state
(
)
(
)
zx += A0
ψ
(a) Compute the normalization constant A. (10 points)
(b) Compute z
S at t=0. (10 points)
(c) Compute y
S as a function of t. (10 points)
Problem 2 (20 points)
Consider a spin-3/2 particle which we shall describe in the basis of eigenstates for z
S
ˆ.
(a) Write the matrix representation for z
S
ˆ and +
S
ˆ (10 points)
(b) Write the matrix representations for x
S
ˆ (10 points)
Problem 3 (20 points)
Consider two particles with spin quantum number S1=3/2 and S2=1 respectively. Their
interaction can be described by a spin Hamiltonian 21
2ˆˆ
2
ˆSS = J=H.
(a) Show that there exist simultaneous eigenstates of H
ˆ and
(
)
2
21
2ˆˆˆ SS +=
tot
S (10 points)
(b) Compute the eigenvalues of H
ˆ and the number of degenerate states for each energy
level. (10 points)
Problem 4 (30 points)
Consider a spin-1/2 particle that we describe in two different bases. The basis B1 consists
of eigenstates for z
S
ˆ and basis B2 consists of eigenstates for n
S
ˆ. The spherical
coordinates for the unit vector n
ˆ are
(
)
(
)
θφ
θφ
1
=
r so that a rotation of
φ
about z
ˆ
followed by a rotation of
θ
about y
ˆ brings z
ˆ into coincidence with n
ˆ.
(a) Write the representation of 2
ˆ
Sand n
S
ˆ in basis B2. (8 poins)
(b) Compute the transformation from the representation of a general state
ψ
in basis B1
to the representation of
ψ
in basis B2. (12 points)
(c) Compute the representation of z
S
ˆ in basis B2 and check your result by selecting
appropriate values of
θ
and
φ.
(10 points)
+Q
pf2

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Introduction to Quantum Mechanics 171.

Midterm Exam 11/3/05 1-

Check the attached formula pages. Start each problem on a fresh page and please give

detailed reasoning. Please ask your proctor for clarification if the text is unclear.

Problem 1 (30 points)

Consider a spin-1/2 particle with charge q and mass m , in a magnetic field of strength B oriented in the z ˆ direction. At t=0, the particle is in the state

ψ ( 0 ) = A ( − x − + z )

(a) Compute the normalization constant A. (10 points)

(b) Compute S (^) z at t =0. (10 points)

(c) Compute S (^) y as a function of t. (10 points)

Problem 2 (20 points)

Consider a spin-3/2 particle which we shall describe in the basis of eigenstates for S ˆ z.

(a) Write the matrix representation for S ˆ z^ and S ˆ+^ (10 points)

(b) Write the matrix representations for S ˆ^ x (10 points)

Problem 3 (20 points)

Consider two particles with spin quantum number S 1 =3/2 and S 2 =1 respectively. Their

interaction can be described by a spin Hamiltonian (^12)

ˆ = 2 S ⋅ S

− H = J.

(a) Show that there exist simultaneous eigenstates of Hˆ^ and ( )

2 1 2

ˆ 2 = S ˆ + S ˆ

S (^) tot (10 points)

(b) Compute the eigenvalues of Hˆ^ and the number of degenerate states for each energy

level. (10 points)

Problem 4 (30 points)

Consider a spin-1/2 particle that we describe in two different bases. The basis B 1 consists

of eigenstates for S ˆ z^ and basis B 2 consists of eigenstates for S ˆ n^. The spherical

coordinates for the unit vector n ˆ^ are ( r θφ ) =( 1 θφ)so that a rotation of φ about z ˆ

followed by a rotation of θ about y ˆ brings z ˆ into coincidence with n ˆ.

(a) Write the representation of S ˆ^2 and S ˆ^ n in basis B 2. (8 poins)

(b) Compute the transformation from the representation of a general state ψ in basis B 1

to the representation of ψ in basis B 2. (12 points)

(c) Compute the representation of S ˆ^ z in basis B 2 and check your result by selecting

appropriate values of θ and φ. (10 points)

+Q

Formulae

Raising and lowering operators

S ˆ^ (^) ± sm == s ( s + 1 ) − m ( m ± 1 ) s , m ± 1

Spin-1/2 eigenstates

  • x = ( + z + − z ) 2
  • y = ( + z + iz ) 2

Spin-1/2 Representations

S (^) x , (^) ⎟⎟ ⎠

i

i S (^) y

S z

Pauli Matrices

σ x , ⎟⎟

i

i

σ y , ⎟⎟

σ z

Representation of rotation operator for spin-1/2 states

( n ) 1 ( n ˆ) 2

sin 2

ˆ = cos − σ⋅

G

R i

Spin-1 Representations

S (^) x , ⎟

i

i i

i S (^) y

S z

A table of Clebsch-Gordan coefficients is attached.