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Physics 451
Quantum mechanics I
Fall 2012
Nov 5, 2012
Karine Chesnel
Homework this week:
• HW #17 Tuesday Nov 6 by 7pm
• HW #18 Thursday Nov 8 by 7pm
Announcements
Quantum mechanics
Quantum mechanics
The hydrogen atom
What is the density of probability of the electron?
The hydrogen atom
2
2 2
1 1 1sin ( 1)
sin sin
Y Yl l
Y
The angular equation (same)
, , ,r R r Y
Angular function (same) , cosm im m
l lY Ae P
Azimutal quantum number
Magnetic quantum number
l
m0l m l
Phys 451
, , ,r R r Y
The radial equation
( )u rR r
2 2 2
2 2
( 1)( )
2 2
d u l lV r u Eu
m dr m r
The hydrogen atom
Coulomb’s law:
2
0
1( )
4
eV r
r
2 2 2 2
2 20
( 1)
2 4 2
d u e l lu Eu
m dr r m r
Phys 451
kr
Asymptotic behaviors
The hydrogen atom
The radial equation2
02 2
( 1)1
d u l lu
d
2mEk
2
2
d uu
d 0
2
2 2
( 1)d u l lu
d
u Ae 1lu B
Phys 451
2
0 202
me
k
The hydrogen atom
1 ( )lu e v
Peeling off the asymptotic behaviors
2
022( 1 ) 2( 1) 0
d v dvl l v
d d
Power expansion0
( ) jj
j
v c
Recursion formula:0
1
2( 1) 2
( 1)( 2 2) 1j j j
j lc c c
j j l j
Phys 451
The hydrogen atom
1 ( )lu e v
The series must terminate
0
( ) jj
j
v c
02( 1)0
( 1)( 2 2)
j l
j j l
max 02( 1)j l
Principal quantum number0
max 12
n j l
Phys 451
Quantum mechanics
Quiz 23a
A. one
B. two
C. n
D. n -1
E. An infinity
For a given quantum number n,how many values of l can exist?
Quantum mechanics
The hydrogen atom
Ground state: “binding energy”
22
1 20
13.62 4
m eE eV
Quantization of the energy22
2 20
1
2 4n
m eE
n
Bohr 1913
Principal quantum number
0 2n
Quantum mechanics
The hydrogen atom
2
20
1
4
mek
n
1~
tank
dis ce
Bohr radius2
1002
40.529 10a m
me
nak
1
Quantum mechanics
The hydrogen atom
21
n
EEn na
kn1
Energies levels
Stationary states ),()(,, mlnlnlm YrRr
n: principal quantum number
l: azimuthal quantum number 1nl
m: magnetic quantum number lm
Degeneracy of nth energy level:
1
0
12n
l
l
Quantum mechanics
Quiz 23b
A. 5
B. 9
C. 11
D. 25
E. 50
What is the degeneracy of the 5th energy bandof the hydrogen atom?
Quantum mechanics
The hydrogen atom
21
n
EEn Energies levels
Spectroscopy
221
11
fi nnE
hcE
Energy transition
22
111
if nnR
Rydberg constant
E0
E1
E2
E3
E4
Lyman
Balmer
Paschen