31.
$${{\bf{\hat A}}}$$ and $${{\bf{\hat B}}}$$ are two quantum mechanical operators. If $$\left[ {{\bf{\hat A}},\,{\bf{\hat B}}} \right]$$  stands for the commutator of $${{\bf{\hat A}}}$$ and $${{\bf{\hat B}}}$$ then $$\left[ {\left[ {{\bf{\hat A}},\,{\bf{\hat B}}} \right],\,\left[ {{\bf{\hat B}},\,{\bf{\hat A}}} \right]} \right]$$    is equal to

33.
The commutator $$\left[ {{L_z},\,{Y_{lm}}\left( {\theta ,\,\phi } \right)} \right],$$    where Lz is the z component of the orbital angular momentum and $${{Y_{lm}}\left( {\theta ,\,\phi } \right)}$$   is a spherical harmonic, is

34.
A particle is in the normalized state $$\left| \psi \right\rangle $$ which is a superposition of the energy eigen states $$\left| {{E_0} = 10\,eV} \right\rangle $$   and $$\left| {{E_1} = 30\,eV} \right\rangle .$$   The average value of energy of the particle in the state $$\left| \psi \right\rangle $$ is 20 eV. The state $$\left| \psi \right\rangle $$ is given by

35.
If Lx, Ly and Lz are respectively the x, y and z components of angular momentum operator L, the commutator [Lx, Ly, Lz] is equal to

36.
The wave function of a particle in a one-dimensional potential at time t = 0 is $$\psi \left( {x,\,t = 0} \right) = \frac{1}{{\sqrt {15} }}\left[ {2{\psi _0}\left( x \right) - {\psi _1}\left( x \right)} \right]$$       where, $${\psi _0}\left( x \right)$$  and $${\psi _1}\left( x \right)$$  are the ground arid the first excited states of the particle with corresponding energies E0 and E1. The wave function of the particle at a time t is

37.
An electron in a time independent potential is in a state which is the superposition of the ground state (E0 = 11 eV) and the first excited state (E1 = 1 eV). The wave function of the electron will repeat itself with a period of

38.
Consider the combined system of proton and electron in the hydrogen atom in its (electronic) ground state. Let $$I$$ denotes the quantum number associated with the total angular momentum and let \[ < \mathfrak{M} > \] denote the magnitude of the expectation value of the net magnetic moment in the state. Which of the following pairs represents a possible state of the system (\[{\mu _B}\] is Bohr magneton)?

40.
Three operators X, Y and Z satisfy the commutation relations, $$\left[ {X,\,Y} \right] = i\hbar Z,\,\left[ {Y,\,Z} \right] = i\hbar X$$     and $$\left[ {Z,\,X} \right] = i\hbar Y.$$   The set of all possible eigen values of the operator Z, in units of $$\hbar $$ is