Quantum Mechanics Flashcards

1
Q

integral limits of a function contained within|x|< b

A

-b to b

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2
Q

What happens if after measuring E1, you repeat the measurement on the same system

A

Measurement collapses the wavefunction and so repeated measurments will always yield E1

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3
Q

what is coulomb potential (V(r)) proportional to

A

1/r (and therefore equal to A/r)

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4
Q

what property of the energy levels of the harmonic oscillator follows from the commutator [H,a+] = hwa+
(assume h=h-bar)

A

the energy levels are equally spaced with spacing hw

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5
Q

radial probability distribution,
how do you find the the most probable value of r for an electron to be found

A

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

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6
Q

how to calculate first order correction (aka perturbation to energy) for all energy levels

given perturbation potential V’(x) and wavefuntion ψn(x).

A

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.

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7
Q

non-degenerate perturbation theory

A

En1/En0 = (1/En0)<ψn0|H’|ψn0>

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8
Q

potential energy of hydrogen

A

V(r) = -e^2/4π(epsilon)r

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9
Q

superposition of eigenstates, form of function
(time-dependent)

A

Ψ(x,t) = ψ1(x)e^(-iE1t/h) + ψ2(x)e^(-iE2t/h)
where h=h_bar

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10
Q

what is another way of writing |E|^2

A

E*E

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11
Q

how does the hamiltonian relate to energy

A

n = Enψn

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12
Q

ψ1 * ψ2 dx = ?
(aka conjugate of 1 times regular 2, if they were the same n would equal 1)

A

0

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13
Q

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?

A
  • 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
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14
Q

spherical coordinate system

A

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.

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15
Q

expectation value of energy

A

<ψ|H|ψ>
insert the hamiltonian into centre of integral.
H = (-h^2/2m) d^2/dx^2

(where h=h_bar)

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16
Q

schodinger equation

A

(-h^2/(2mr^2)) d/dr(r^2(dψ/dr)) + V(r)ψ = Eψ

(note: can ignore constants when subbing in ψ)

17
Q

explain the significance of the quantum numbers n,l,m

A

n: principal/radial, determines energy of the state
l: total angular momentum
m: magnetic, labels the z-component of the angular momentum

l<n, -l</=m</=l (</= less than or equal to)

18
Q

quality of states and angular momentum

A

states have non-zero angular momentum

19
Q

what does the commutator [x_hat, xPz] equal

A

0, because P is not x based (if it was would equal xih_bar)

20
Q

probability of E1

A

|c1|^2

21
Q

En relation to E1

A

En = n^2 E1

22
Q

what does the stern-gelach apparatus do?
equation for number of beams

A

produces a force on a beam of particles that depends on the z-component of the particles’ magnetic moment

beams split into = 2s+1

23
Q

degeneracy of states general equation

A

n^2 sequence
eg. n=1, degeneracy = 1
n=2, degenracy = 4

24
Q

angular momentum operator

A

J_hat = L_hat + S_hat
J^2 = j(j+1)h_bar
= L^2 + S^2 + 2S*L

25
Q

semi-infinite well potential sketch key points, effect of slightly reducing V0

A

0 @ x=0, continuous positve gradient @ x=L,
peaks/troughs shifted slightly to right compared to infinite well,
exponential decay of excited states is longer/slower than ground state.

if V0 is reduced, wavelength increases with much larger decay. Peaks/troughs stay within L

26
Q

how to integrate powers of trig
cos^n(x)sin^m(x) dx

A

if n is odd, sub u=sinx
if m is odd, sub u=cosx

27
Q

what is the result when an angular momentum operator is applied to its corresponding eigenfunction

A

scalar multiple of the same eigenfunction

28
Q

how to integrate e^(iθ)

A

= -i e^(iθ)
from 0 to 2(pi), use euler:
e^(ix) = cos(x) +isin(x)

29
Q

what to do when x_hat or p_hat in in question

A

times by x_bar = x or p_bar = -ih_bar(d/dx)
not <x> or <p>
no need to integrate</x>

30
Q

energy of harmonic oscillator

A

En = hw((1/2) + n)
odd values of n give solution to potential

(where h = h_bar)

31
Q

what does the imaginary part of the wavevector represent

A

decay of amplitude of wave

(for calculations of real things jusst take real part)