Quantum Mechanics Flashcards
integral limits of a function contained within|x|< b
-b to b
What happens if after measuring E1, you repeat the measurement on the same system
Measurement collapses the wavefunction and so repeated measurments will always yield E1
what is coulomb potential (V(r)) proportional to
1/r (and therefore equal to A/r)
what property of the energy levels of the harmonic oscillator follows from the commutator [H,a+] = hwa+
(assume h=h-bar)
the energy levels are equally spaced with spacing hw
radial probability distribution,
how do you find the the most probable value of r for an electron to be found
P(r) dr = r^2R(r)^2 dr
(techincally proportional to not equals, so can ignore constants given with R(r))
electron is most likely to be found at dP/dr = 0
how to calculate first order correction (aka perturbation to energy) for all energy levels
given perturbation potential V’(x) and wavefuntion ψn(x).
En = <ψn|V’(x)|ψ>
(intregral between given limits for ψ squared times V)
Results in a funtion concerning n. Determine solution for even and odd n to find correction to all levels.
non-degenerate perturbation theory
En1/En0 = (1/En0)<ψn0|H’|ψn0>
potential energy of hydrogen
V(r) = -e^2/4π(epsilon)r
superposition of eigenstates, form of function
(time-dependent)
Ψ(x,t) = ψ1(x)e^(-iE1t/h) + ψ2(x)e^(-iE2t/h)
where h=h_bar
what is another way of writing |E|^2
E*E
how does the hamiltonian relate to energy
Hψn = Enψn
ψ1 * ψ2 dx = ?
(aka conjugate of 1 times regular 2, if they were the same n would equal 1)
0
for a finite potential well with a lower potential on the left than right, what do the wavefunction sketch’s look like for E1 and E2?
- E1 has 1 turning point, E2 has 2
- functions should decay to zero more gradually on the left than the right (there should be bleeding out the fucntion on both sides)
- turning points should be slightly displaced to the left relative to the symmetric case
spherical coordinate system
r^2 sinθ dθdφdr
x = rcosθcosφ
y = rsinθsinφ
z = rcosθ
typically, integrate θ between pi and 0, φ between 2pi and 0, and r between infinity and 0.
expectation value of energy
<ψ|H|ψ>
insert the hamiltonian into centre of integral.
H = (-h^2/2m) d^2/dx^2
(where h=h_bar)