Quantum Questions Flashcards
Why can we use the results derived for the hydrogen atom to work out the orbital angular momentum, z component of orbital angular momentum and the orbital magnetic moment for any atom, but not for the energy?
The radial component has a Z dependence, the angular parts do not.
Explain any limitations of the Schrodinger equation
Does not include spin orbit effects and so fails to predict sodium doublet and other phenomena due to energy level splitting
Explain any limitations of the bohr model
Guesses quantisation, breaks heisenbergs uncertainty principle as it assumes fixed orbits and fixed trajectories, its derived assuming no uncertainty in the electrons position and velocity. Does not include any spin. Does not have any indication of degeneracy of each energy level.
What are the Conditions for a quantum Harmonic Oscillator to be in its classical limit?
E»(Hbar)*w
List the differences between Classical and Quantum Harmonic Oscillators
Quantum has a Zero Point energy, classically the lowest energy state is zero
Quantum energy states are discrete, classical is continuos
PDF’s for classical systems have maximums at either side, a ground state has a maximum at the centre of the potential
Why can you not define mj unless you have an external magnetic field?
mj represents the total angular momentums projection onto the Z axis. We need an external B field to define the Z axis, else due to spherical symmetry as the Z axis is not well defined, neither is mj.
Explain what |ψ|^2 is a measure of
|ψ|^2 Is a measure of the particles PDF. It is integrated to give the probability of finding a particle within a certain region.
Why it is incorrect to say P(r)dr = |ψ|^2dr and why the correct expression is P(r)dr = |ψ|^2 dV where P(r) is the probability density function of the particle.
|ψ|^2 dr returns the probability of finding the particle at some distance r away from the origin WITHOUT taking into account the whole shell of points at that distance.
|ψ|^2 dV returns the same probability, but factoring in the shell of points which the particle could be at if it was at a distance r away.
How many radial zeros does a wave function have with quantum numbers n and l
n-l-1
How do we measure the energy of the electronic states?
Spectroscopy - Look at the light emitted from electrons transitions between particular states
What is the balmer series
One of the 6 named sets hydrogen spectral emission lines. Describes any transition where the final state is n = 2 - All light in this series is visible.
Describe what determines whether an emission line in the emission spectrum of hydrogen will be strong or weak.
Strong if changes in the following quantum numbers are:
L = +-1
J= +- 1, 0
mj=+-1 , 0
Explain what natural or lifetime broadening is and the physical reason for the natural relaxation of excited electrons.
Natural or lifetime broadening:
This is the most fundamental mechanism and derives from the uncertainty principle that links the
uncertainty in energy ∆E_N (N for natural broadening) with the uncertainty in time ∆t,
∆E_N ∆t ∼ h bar
• A perfectly defined energy level for which ∆E = 0 must have an infinite lifetime.
• This may be true of the ground state, but not the excited states where given time they relax
back to the ground state, hence ∆t < ∞ and so ∆E > 0.
Physical reason:
Short lived Particle Antiparticle pairs constantly being created which can perturb our excited electron causing it to de excite.
Derive an expression for the total broadening of a transition and show it is equal to:
hbar(1/ tau_ f + 1/tau _i) where tau is the average lifetime of an excited state, f is the final state and i is the initial state.
Start with the HUP:
delta E * tau = h bar
delta E _ transition = delta E _f + delta E _ i
Explain Pressure or collision broadening and how it can be minimised.
The time between collisions of gas atoms can be shorter than the natural lifetime. This can cause
premature relaxation and emission of a photon. This reduces the lifetime and hence increases the
uncertainty ∆E_C in the energy.
At higher pressures the time τ_C between collision will be shorter than at lower pressures. (C for collision)
Minimise P to minimise delta E.
Explain doppler broadening and how it can be minimised
If a transition of an atom that is stationary with respect to a photo detector has frequency f0
then atoms travelling towards (+) and away from (−) a detector with a velocity v will have an
apparent Doppler modified emission frequency.
Minimise T to minimise delta E
If quantum states of the hydrogen atom have a φ dependence of the form exp(iαφ) where α is a
constant, explain why α must be an integer (i.e., the quantum number ml)
Need exp(iα(φ+2pi))=exp(iαφ) as φ +2pi returns us back to the same point in space, the wave function must be single valued and so must have the same value at this point and so the above equation must be satisfied. It is only satisfied if α is an integer as sin / cos ( α (x + 2pi) ) only returns the same value i
Why cant you measure all 3 components of L at the same time?
Fundamental QM- measurement collapses the wavefunction to an eigen state with the measured value Eg measure the Lz component of a wave function. Wave function collapses to one of its eigen states with the measured value of Lz. This eigen state is not an eigen function of the Lx operator or the Ly operator and so measuring Lx or Ly subsequently will change the eigen state to a different one, which will mean we have lost all knowledge about what Lz is now.
What happens when take an isolated electron and apply a weak magnetic field along the Z axis?
The magnetic moment due to spin of the electron will try to align with the B field but will fail due to the quantisation of Sz. There will be a net torque on the system as such and the electron will begin to precess about the Z axis.