Formulae Flashcards

1
Q

the overlap of the same state

A

<n|n> = 1

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2
Q

commutator

A

[A,B] = [AB-BA]

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3
Q

something is minimised when

A

the derivative is set equal to zero i.e. d/dx = 0

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4
Q

reduced mass

A

µ = (me mN)/(me+mN) = (m1 m2)/(m1+m2)

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5
Q

spherical harmonics are correctly normalised if

A

(2π ∫ 0) (π ∫ 0) |(Y^m l)|^2 sinθdθdφ

Remember to square everything in the wave function

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6
Q

a wave function is normalised in general if

A

( ∞ ∫ 0) |Ψ|^2 dr^3 = 1

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7
Q

expectation value of <r^3>

A

calculate ∫dr^3 |Ψ|^2 r^3 as before with extra expectation value multiplied in

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8
Q

Rydberg equation

A

E = Ry (1/n2^2 - 1/n1^2)

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9
Q

Planck’s equation

A

E = hf = hλ/c

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10
Q

Derive the angular momentum operators Lx, Ly and Lz

A

L = r x p

p = (-iℏ∇)

and r = (x,y,z)

take the cross product

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11
Q

lowering operator for L

A

L- = Lx - iLy

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12
Q

the conjugate of |x>

A

<x|

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13
Q

total angular momentum quantum number

A

j = l ± 1/2

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14
Q

how is mj related to ms and ml

A

mj = ml + ms

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15
Q

how is J related to L and S

A

J = L + S

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16
Q

first order pertubation theory

A

|Ψn(λ)> = |Ψn(0)> + λ|Ψn(1)> + O(λ^2)

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17
Q

to show something is orthonormal

A

take the conjugate

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18
Q

hydrogen atom wavefunction

A

Ψnlm on formula sheet

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19
Q

virial theorem

A

<V> = -2<T>
</T></V>

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20
Q

Write the Hamiltonian in the form of its kinetic and potential energy

A

<H> = <T> + <V>
</V></T></H>

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21
Q

how are the relativstic corrections and the spin-orbit coupling related

A

En^(0) = E^(1) rel + E^(1) SO

on the formula sheet = En (Zα)^2/n^2 …

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22
Q

in the stark effect z can be written as

A

z = rcosθ

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23
Q

energy shift in the Paschen-back regime

A

strong magnetic field

∆E = ωlℏ(m+2ms) on formula sheet

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24
Q

how is m related to l

A

-l ≤ m ≤ l

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25
what does >JJ mean
j,mj>
26
what does >LS mean
ml,ms>
27
how is >JJ related to >LS
|jmax,jmax>JJ = l,s>LS
28
how does n relate to l
n = 1,2,3,... l = 0,1,2,...
29
the total energy of two electrons to first order pertubation
Etot = E(0) + E(1)
30
binding energy
En ~ - Ry Z^2/n^2
31
transition energy
E(gamma) = Ry(Z^2/n1^2 - Z^2/n2^2)
32
labelling of shells and subshells
K, L, M, N n = 1,2,3,4 l = 0,1,2,3 s, p, d, f n = 1,2,3,4 l = 0,1,2,3
33
[p,x] =
iℏ
34
quantum harmonic oscillator ladder operators
a-|n> = √n|n-1> a+|n> = √n+1|n+1>
35
harmonic oscillator restoring force
F = -kx = - mω^2x
36
force constant
k = mω^2
37
what is the first order perturbation
H(1)
38
what is the energy of the first order perturbation
E(1) =
39
rotational energy
E = 1/2ℏω
40
reduced mass for hydrogen
µ = 1/2 mp
41
Operator L^2 and S^2 and J^2
J = h(bar)^2 j(j+1) similarly for L and S
42
Zeroth order perturbation
H(0)|n> = En(0)|n>
43
δnm
44
Standard deviation
Δr = ( -^2)^(1/2)
45
Stark energy shift
ΔEstark = eEz.z Hstark = εE.z eε ∫ z dr^3 |psi|^2
46
Diagonalisation of the matrix of eigenvalues
det|H(1) - λI| gives the energy splitting
47
Applying the lowering operator to the ground state
a-|n0> = 0
48
K alpha
n = 2 to n= 1
49
K beta
n = 3 to n = 1
50
Energy levels for harmonic oscillators.
En = ℏω(n+1/2)
51
The number of spin states for para spin states
N = (s+1)(2s+1)
52
The number of spin states for ortho spin states
N = s(2s+1)
53
In a weak magnetic field
(L . 2S) . B is small
54
Re write Lz + 2Sz in terms of Jz and Sz
Lz + Sz + Sz => Jz + Sz
55
x(hat)
x(hat) = i (ℏ/2mω)^1/2 (A- - A+)
56
p(hat)
p(hat) = (mℏω/2)^1/2 (a+ + a-)
57
Screening factors
Z1 ~ (Z-a) and Z2 ~ (Z-b)
58
Parity
Pr = r Pθ = π - θ PΦ = Φ + π
59
the orbital magnetic moment
mL = -e/2me L
60
L x L
iℏL
61
S x S
iℏS
62
spin magnetic moment
ms = -eg/2me S
63
nuclear magneton
μN = eℏ/2mN
64
{A,B}
AB + BA
65
energy of a multielectron states
Ex(0) = -Z^2 Ry (1/n1^2 - 1/n2^2)
66
state labelling the the L-S coupling scheme (diatomic molecules)
2S+1 XJ where X = S,P,D,F
67
S1 . S2
S(1,+)S(2,-) + S(1,-)S(2,+) + 2S(1,z)S(2,z)
68
L . S
L+S- + L-S+ + 2LzSz
69
[Lz,z]
=0
70
[Lz,L±]
±ħL±
71
[L^2,L ±]
=0
72
[L,S]
=0
73
A probability distribution is maximised
When x tends to infinity
74
Energy shift to First order perturbation of the stark effect
En < psi | eεz | psi > = eε ∫ dr^3 z |psi|^2
75
Probability density
|Rnl|^2 |Yml|^2 r^2 sin theta d theta d phi dr
76
Property of factorials
n! = n x (n-1)!
77
|jmax, -jmax> JJ
= | -l, -s>LS
78
|jmax,jmax>JJ
|l,s>