The wave function of a particle moving in a one-dimensional time independent potential V(x) is given by ψ(x)=e−iax+b, where a and b are constants. This means that the potential V(x) is of the form
The Hamiltonian of a particle is given by H=2mp2+V(r)+ϕ(+r)L.S, where S is the spin, V(r) and ϕ(r) are potential functions and L(=r×p) is the angular momentum. The Hamiltonian does not commute with
The radial wave function of the electrons in the state of n = 1 and 1 = 0 in hydrogen atom is R10=a0232exp(−a0r),a0 is the Bohr radius. The most probable value of r for an electron is
A particle is in the normalized state ∣ψ⟩ which is a superposition of the energy eigen states ∣E0=10eV⟩ and ∣E1=30eV⟩. The average value of energy of the particle in the state ∣ψ⟩ is 20 eV. The state ∣ψ⟩ is given by
The wave function of a particle in a one-dimensional potential at time t = 0 is ψ(x,t=0)=151[2ψ0(x)−ψ1(x)] where, ψ0(x) and ψ1(x) 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
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
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 <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 (μB is Bohr magneton)?
Three operators X, Y and Z satisfy the commutation relations, [X,Y]=iℏZ,[Y,Z]=iℏX and [Z,X]=iℏY. The set of all possible eigen values of the operator Z, in units of ℏ is