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MPH 8: Quantum Mechanics-II

Title Name IGNOU MPH 8 SOLVED ASSIGNMENT
Type Soft Copy (E-Assignment) .pdf
University IGNOU
Degree MASTER DEGREE PROGRAMMES
Course Code MSCPH
Course Name Master of Science (Physics)
Subject Code MPH 8
Subject Name Quantum Mechanics-II
Year 2026
Session -
Language English Medium
Assignment Code MPH 8/Assignment-1/2026
Product Description Assignment of MSCPH (Master of Science (Physics)) 2026. Latest MPH 008 2026 Solved Assignment Solutions
Last Date of IGNOU Assignment Submission Last Date of Submission of IGNOU BEGC-131 (BAG) 2025-26 Assignment is for January 2026 Session: 30th September, 2026 (for December 2025 Term End Exam).

Semester Wise
January 2025 Session: 30th March, 2026 (for June 2026 Term End Exam).
July 2025 Session: 30th September, 2025 (for December 2025 Term End Exam).
FormatReady-to-Print PDF (.soft copy)

📅 Important Submission Dates

  • January 2026 Session: 31st March, 2026
  • July 2026 Session: 30th September, 2026

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MPH 8 2025 - English

Tutor Marked Assignment QUANTUM MECHANICS-II

Course Code: MPH-008

Assignment Code: MPH-008/TMA/2025

Max. Marks: 100

Note: Attempt all questions. The marks for each question are indicated against it.

PART A

1. a) Write the space translation operator in quantum mechanics ) ˆT for an infinitesimal translation (a). Hence evaluate the commutators:equation andequation

b) Show that for a Hamiltonian equation to commute with the time reversal operator the potential function V(x) must be real. 

2. a) Construct the wave function equation for a system of 3 identical fermions in the states equation respectively of an one-dimensional box of size A 

b) Calculate the ground state energy for a system of five identical spin equation particles placed In a one-dimensional simple harmonic oscillator potential of frequencyequation

3. For a system of two particles each with angular momentum oneequation

(i) Construct the normalized states of highest and second highest Jz for total angular momentum 2.

(i) Construct the normalized state of highest J₂ for total angular momentum 1. 

4. Consider the following symmetric two-dimensional infinite potential well equation otherwise

Determine the first order perturbation correction to the energy eigenvalue of the two-fold degenerate first excited state, for the following perturbation: equation

 

5. Determine the upper bound to the ground state energy for a particle in a one-dimensional box of length L. using the trial wave function:equation

PART B

6. Consider the motion of a quantum particle in a potential V(x)-ax. Use the WKB approximation to determine how the energy of the bound state E, varies with n and a for large values of n.

7. A particle is in the ground state of the simple harmonic oscillator of frequency. A t =0 frequency of the oscillator changes from particle to remain in the ground state at equation Calculate the probability for the particle to remain in the ground state at t > 0.

8. For a static (time-independent) perturbation V suddenly switched on at time t=0:

equation

show that the transition probability for a transition of the system from a state equation

equation up to first order in perturbation theory is just: equation How does the transition probability change if the time of application is doubled in the limit t→0. (6+4)

9. For a Dirac particle moving in a central potential, show that the orbital angular momentum is not a constant of motion.

equation

10. Consider the scattering of a particle of mass m by the following potential  equation Assuming that the scattering is mainly due to s-waves (1-0), calculate the s-wave phase shift. 


MPH 008 (January 2026 - July 2026) - ENGLISH

Tutor Marked Assignment
QUANTUM MECHANICS-II

Course Code: MPH-008
Assignment Code: MPH-008/TMA/2026
Max. Marks: 100

Note: Attempt all questions. The marks for each question are indicated against it.


PART A

1. a) Write the space translation operator in quantum mechanics equation for a finite translation a along the x direction. Calculate the commutator equation. You may use the Baker-Campbell-Hausdorff formula: equation 

b) Consider an operator equation for which equation. Show that the expectation value of equation in a parity eigenstate is zero. 

2. a) Determine the wave function and energy of the ground state and first excited state for a system of two identical bosons in 1D simple harmonic oscillator. 

b) Define the action of the permutation operator equation for a system of two particles 1 and 2 and two states equation and equation. Show that equation and determine the eigenvalues of equation

3. a) Write down the eigenkets equation for equation with equation.

b) Calculate the matrix elements for J2 for a system of two spin half particles. 

4. Determine the first and second order perturbation correction to the ground state energy eigenvalue of the one-dimensional infinite potential well of width L (equation) with the perturbation: equation

5. Consider the following one-dimension simple harmonic oscillator Hamiltonian operator
equation$
Use a trial wave function equation with a variational parameter equation to estimate the upper bound to the ground state energy. 

PART B

6. Determine the WKB approximation for the bound state energy of a particle of mass m in the potential:

equation

7. Consider the two state problem in which the unperturbed Hamiltonian equation has just two eigenkets, equation and equation with: equation; equation, and E2 > E1. The system is subjected to a time-dependent perturbation: equation.
Calculate the probability for the system to be in the state equation at time t, given that it is in the state equation at equation.

8. A charged particle of mass m and charge q, is confined to a one-dimensional box of side L with equation. At t > 0, an electric field equation acts on the particle where equation is a constant. If the particle is in the ground state when t < 0, calculate the probability that it will be in the first excited state for t > 0.

9. Using the Born Approximation, calculate the differential cross-section for a beam of particles of mass m scattered by a potential: equation. You may use:
equation$

10. a) Explain how the expression for the energy levels obtained by solving Klein Gordon equation for a Coulomb field differs from the results derived from Schrödinger equation. Why is this solution not able to explain the fine-structure splitting of the energy levels?
b) Derive the current conservation equation from the Dirac equation.
 

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