How can we relate the wavefunctions for indistinguishable particles?
(Hint: Phase factor, K)
What does it mean for a phase factor of -1 or 1?
K = exp(-ia)
Probability denisities must stay the same for indistinguishable particles.
-1 for anti-symmetric, +1 for symmetric wavefunctions.
What are particles with symmetric wavefunctions called? Give examples
What are particles with antisymmetric wavefunctions called? Give examples
State the degeneracy of quantum states for a particle with total spin quantum number l.
Question on image: FOR BOSON!
Where i and j represent any eigenfunction.
For non-interacting particles, what is the energy of this state?
What is the form of the wavefunction for two fermions?
What does i=j show?
i=j shows that fermions can not exist in the same state, PAULI EXCLUSION PRINCIPLE.
If i=j, Psi = 0, Pauli exclusion principle.
For a large reservoir, how do we treat the chemical potential and Temperature if a small number of particles is added/removed?
What is the temperature of the reservoir by definition?
1.By integrating the chemical potential and/or the temperature of a reservoir, find the number of microstates in the reservoir.
2.Now consider a system connected to a reservoir, forming a grand canonical ensemble, re-write in terms of the total number of particles and energy.
Hint: Consdider the fact that energy and number of particles is conserved.
DON’T LOOK AT IMAGE AS IT GIVES WORKED INTEGRATION
Suppose at some instant System A is in a particular quantum state, state β,
comprising of Nb identical particles, distributed amongst the system’s singleparticle energy levels so that their total energy [of the form in Eq. (11.2)] =Eβ.
What is the number of accesible quantum states/microstates for the TOTAL system, W_b?
(eq 12.6 in ans)
Working on from the image, what is the OVERALL number of states for the TOTAL system, corresponding to all possible different states (j) of system A.
*Total system = System A + Reservoir
State the GRAND partition function (12.6 + 12.7)
Next, find the probability of being in a state Beta.
Find the probability that a state is occupied.
What is the Gibbs definition of entropy of system A (that is connected to a reservoir)?
Given the probability that System A is in a state, Beta, find an expression for the entropy of the system, expressing in terms of averages.
Re-arranging this, find an expression for the GRAND POTENTIAL.
What is the grand potential an analogue of?
Derive the thermodynamic properties of systems with varying particle number, starting witht he Grand Potential.
Write in terms of the grand canonical ensemble.
Applying the differential to the grand potential and using the fact that dE = mu dN - p dV + T dS,
we get to this equation.
Given this information, find the probability that state i is occupied.
For the Fermi-Dirac distribution, when T=0 K, how many states with energy E < mu are occupied, and how many states with energy E> mu are occupied?
What does Ef equal at T=0?
For Fermi-Dirac distribution, all states with E<mu> mu are occupied.
At T=0, chemical potential = Ef (fermi energy, energy of highest occupied state at T=0 K)</mu>
Using the information provided, find the average number of particles in state i.
How do we find the chemical potential?
** Give a qualitative and quantitative description/idea/method.
Don’t forget spin degeneracy!! 2 Fermions can exist in the same state as long as they have opposite spins!
Use the density of states for a 3D box to find an integral expression for the total Number of particles in a box, N.
Give the grand potential of a Fermi gas made by the 2 quantum states with energy E(n,l,s), choosing the state i to be the state with quantum numbers n,l,s, as a function of the Grand partition function.
Then, using summation form, give the total Grand potential of a fermi gas (for all energy levels).