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Develop and write down the expressions of L^2, L_z and L_z^2 in angular momentum operator algebra.

IFoS 2013Paper II10 marksifos-2013-subject-05-006

Show that the spherical harmonics Y_{lm}(\theta, \phi) are simultaneous eigenfunctions of L^2, L_z and L_z^2. What are their corresponding eigenvalues?

IFoS 2013Paper II30 marksifos-2013-subject-05-005

Write down Schrödinger equations for a particle of energy E < V_0, incident on a step potential height V_0. Solve them to find out the transmission and reflection coefficients in terms of k and k', where k = \sqrt{\frac{2mE}{\hbar^2}} and k' = \sqrt{\frac{2m(V_0 - E)}{\hbar^2}}. Show that in this case, there is a finite probability of finding the particle in a classically forbidden region.

IFoS 2013Paper II35 marksifos-2013-subject-05-004

The particle in a box has a ground state wave function given as \psi(x) = \frac{1}{\sqrt{l}} \cos \frac{\pi x}{2l} The box width is 2l and the particle is confined within (-l, +l). Calculate the expectation value of x^2.

IFoS 2013Paper II8 marksifos-2013-subject-05-003

(i) Enumerate the possible values of quantum numbers j and m_j for state in which l = 2 and s = 1/2.

(ii) Draw the corresponding vector model diagram.

IFoS 2013Paper II8 marksifos-2013-subject-05-002

A particle is bound in a potential well given by V(x) = \begin{cases} \infty & \text{for } x \le 0 \\ cx & \text{for } x > 0 \end{cases} Estimate the ground state energy of the system from uncertainty principle.

IFoS 2013Paper II8 marksifos-2013-subject-05-001

The normalized wave function for the electron in the ground state of the hydrogen atom is given by \psi(r)=\dfrac{1}{\sqrt{\pi a_0^3}}e^{-r/a_0}, where a_0 is the radius of the first Bohr orbit. Calculate the probability of finding the electron within a distance r_0 of the proton in the ground state.

CSE 2013Paper II10 markscse-2013-subject-05-005

Using the definition \vec{L}=\vec{r}\times\vec{p} of the orbital angular momentum operator, evaluate [L_x,L_y].

CSE 2013Paper II10 markscse-2013-subject-05-004

Use the uncertainty principle to estimate the ground state energy of a linear harmonic oscillator.

CSE 2012Paper II12 markscse-2012-subject-05-001

(i) Solve the radial part of the time-independent Schrödinger equation for a hydrogen atom. Obtain an expression for the energy eigenvalues.

(ii) What is the degree of degeneracy of the energy eigenvalues? What happens if the spin of the electron is taken into account?

CSE 2012Paper II45 markscse-2012-subject-05-003

Consider the one-dimensional wavefunction \psi(x)=Axe^{-kx}, (0\leq x\leq\infty;\,k>0)

(i) Calculate A so that \psi(x) is normalized.

(ii) Using Schrödinger's equation find the potential V(x) and energy E for which \psi(x) is an eigenfunction. (Assume that as x \to \infty, V(x) \to 0).

CSE 2012Paper II4+8=12 markscse-2012-subject-05-002

What do you understand by expectation value ? Prove that \frac{d}{dt}\langle x\rangle = \frac{1}{m}\langle p_x\rangle

IFoS 2012Paper II10 marksifos-2012-subject-05-001

A lead ball of mass 0\cdot 1\text{ g} is thrown with a velocity of 10^3\text{ cm/sec} through a hole 1\text{ cm} in radius. Calculate the uncertainty in the angle of emergence.

IFoS 2012Paper II10 marksifos-2012-subject-05-002

Starting from Schrödinger equation obtain an expression for the probability current density. Hence give an interpretation to the wave function.

IFoS 2012Paper II10 marksifos-2012-subject-05-003

Solve the Schrödinger equation to obtain the energy levels and eigenfunctions of a particle in a one dimensional infinitely deep potential well given by \begin{aligned} V(x) &= 0 \text{ for } 0 < x < a \\ &= \infty \text{ for } x < 0 \text{ and for } x > a \end{aligned} Show that they form an orthonormal set of functions. What do you understand by completeness condition ? Show that they form a complete set of functions.

IFoS 2012Paper II20+10=30 marksifos-2012-subject-05-004

Solve the Schrödinger equation for a gas of non interacting electrons enclosed in a cube of volume L^3. What do you mean by density of states ? Calculate the density of states and Fermi energy for the above system.

IFoS 2012Paper II20 marksifos-2012-subject-05-005

(i) Show that the orientation of the spin angular momentum vector of an electron with respect to the z-axis is less than one radian for spin up electron. (ii) When the orbital angular momentum vector \vec{L} has the magnitude \sqrt{6}\hbar, calculate the L_z components. What angles does the \vec{L} vector make with the z-axis ?

IFoS 2012Paper II20 marksifos-2012-subject-05-006

Given that \sigma_x,\sigma_y,\sigma_z are Pauli spin operators, prove the following relationships:

(i) \sin(\sigma_x\varphi)=\sigma_x\sin\varphi

(ii) \cos(\sigma_z\varphi)=\cos\varphi

CSE 2012Paper II6 markscse-2012-subject-05-004

For a quantum mechanical system prove that all energy eigen-values E_n are real and if E_n \neq E_k, then the corresponding eigen functions are orthogonal.

IFoS 2011Paper II10 marksifos-2011-subject-05-002

Solve the Schrodinger equation for a potential step function given by \begin{aligned} v(x) &= 0 \text{ for } x < 0 \\ &= v_0 \text{ for } x > 0 \end{aligned} and calculate the reflection and transmission coefficients. Show that for E < v_0 there is a finite probability of finding the particle in a classically forbidden region.

IFoS 2011Paper II20+10=30 marksifos-2011-subject-05-003

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