Title: Last Time
1Last Time
- Bohr model of Hydrogen atom
- Wave properties of matter
- Energy levels from wave properties
2Hydrogen atom energies
- Quantized energy levels
- Each corresponds to different
- Orbit radius
- Velocity
- Particle wavefunction
- Energy
- Each described by a quantum number n
3Quantum Particle in a box
- Particle confined to a fixed region of spacee.g.
ball in a tube- ball moves only along length L - Classically, ball bounces back and forth in tube.
- This is a classical state of the ball.
- Identify each state by speed, momentum(mass)x(sp
eed), or kinetic energy. - Classical any momentum, energy is
possible.Quantum momenta, energy are quantized
4Classical vs Quantum
- Classical particle bounces back and forth.
- Sometimes velocity is to left, sometimes to right
- Quantum mechanics
- Particle represented by wave p mv h / ?
- Different motions waves traveling left and right
- Quantum wave function
- superposition of both at same time
5Quantum version
- Quantum state is both velocities at the same time
- Ground state is a standing wave, made equally of
- Wave traveling right ( p h/? )
- Wave traveling left ( p - h/? )
- Determined by standing wave condition Ln(?/2)
Quantum wave function superposition of both
motions.
6Different quantum states
- p mv h / ?
- Different speeds correspond to different ?
- subject to standing wave condition integer
number of half-wavelengths fit in the tube.
Wavefunction
n1
n2
7Particle in box question
- A particle in a box has a mass m. Its energy is
all kinetic p2/2m. Just saw that momentum in
state n is npo. Its energy levels -
- A. are equally spaced everywhere
- B. get farther apart at higher energy
- C. get closer together at higher energy.
8Particle in box energy levels
- Quantized momentum
- Energy kinetic
- Or Quantized Energy
nquantum number
9Question
- A particle is in a particular quantum state in a
box of length L. The box is now squeezed to a
shorter length, L/2. - The particle remains in the same quantum state.
- The energy of the particle is now
- A. 2 times bigger
- B. 2 times smaller
- C. 4 times bigger
- D. 4 times smaller
- E. unchanged
10Quantum dot particle in 3D box
CdSe quantum dots dispersed in hexane(Bawendi
group, MIT) Color from photon absorption Determine
d by energy-level spacing
- Energy level spacing increases as particle size
decreases. - i.e
11Interpreting the wavefunction
- Probabilistic interpretation
- The square magnitude of the wavefunction ?2
gives the probability of finding the particle at
a particular spatial location
Wavefunction
Probability (Wavefunction)2
12Higher energy wave functions
n
p
E
Wavefunction
Probability
n3
n2
13Probability of finding electron
- Classically, equally likely to find particle
anywhere - QM - true on average for high n
Zeroes in the probability!Purely quantum,
interference effect
14Quantum Corral
D. Eigler (IBM)
- 48 Iron atoms assembled into a circular ring.
- The ripples inside the ring reflect the electron
quantum states of a circular ring (interference
effects).
15Scanning Tunneling Microscopy
Tip
Sample
- Over the last 20 yrs, technology developed to
controllably position tip and sample 1-2 nm
apart. - Is a very useful microscope!
16Particle in a box, again
Particle contained entirely within closed tube.
Open top particle can escape if we shake hard
enough. But at low energies, particle stays
entirely within box. Like an electron in metal
(remember photoelectric effect)
17Quantum mechanics says something different!
Low energy Classical state
- Quantum Mechanics
- some probability of the particle penetrating
walls of box!
Low energy Quantum state
Nonzero probability of being outside the box.
18Two neighboring boxes
- When another box is brought nearby, the electron
may disappear from one well, and appear in the
other! - The reverse then happens, and the electron
oscillates back an forth, without traversing
the intervening distance.
19Question
Suppose separation between boxes increases by a
factor of two. The tunneling probability
- Increases by 2
- Decreases by 2
- Decreases by lt2
- Decreases by gt2
- Stays same
20Example Ammonia molecule
- Ammonia molecule NH3
- Nitrogen (N) has two equivalent stable
positions. - Quantum-mechanically tunnels 2.4x1011 times per
second (24 GHz) - Known as inversion line
- Basis of first atomic clock (1949)
21Atomic clock question
- Suppose we changed the ammonia molecule so that
the distance between the two stable positions of
the nitrogen atom INCREASED.The clock would - A. slow down.
- B. speed up.
- C. stay the same.
22Tunneling between conductors
- Make one well deeper particle tunnels, then
stays in other well. - Well made deeper by applying electric field.
- This is the principle of scanning tunneling
microscope.
23Scanning Tunneling Microscopy
Tip, sample are quantum boxes Potential
difference induces tunneling Tunneling extremely
sensitive to tip-sample spacing
Tip
Sample
- Over the last 20 yrs, technology developed to
controllably position tip and sample 1-2 nm
apart. - Is a very useful microscope!
24Surface steps on Si
- Images courtesy M. Lagally, Univ. Wisconsin
25Manipulation of atoms
- Take advantage of tip-atom interactions to
physically move atoms around on the surface
- This shows the assembly of a circular corral by
moving individual Iron atoms on the surface of
Copper (111). - The (111) orientation supports an electron
surface state which can be trapped in the corral
D. Eigler (IBM)
26Quantum Corral
D. Eigler (IBM)
- 48 Iron atoms assembled into a circular ring.
- The ripples inside the ring reflect the electron
quantum states of a circular ring (interference
effects).
27The Stadium Corral
D. Eigler (IBM)
- Again Iron on copper. This was assembled to
investigate quantum chaos. - The electron wavefunction leaked out beyond the
stadium too much to to observe expected effects.
28Some fun!
Carbon Monoxide man Carbon Monoxide on Pt (111)
- Kanji for atom (lit. original child)
- Iron on copper (111)
D. Eigler (IBM)
29Particle in box again 2 dimensions
Motion in y direction
Motion in x direction
- Same velocity (energy), but details of motion
are different.
30Quantum Wave Functions
- Ground state same wavelength (longest) in both x
and y - Need two quantum s,one for x-motionone for
y-motion - Use a pair (nx, ny)
- Ground state (1,1)
Probability(2D)
Wavefunction
Probability (Wavefunction)2
One-dimensional (1D) case
312D excited states
(nx, ny) (2,1)
(nx, ny) (1,2)
These have exactly the same energy, but the
probabilities look different. The different
states correspond to ball bouncing in x or in y
direction.
32Particle in a box
- What quantum state could this be?
- A. nx2, ny2
- B. nx3, ny2
- C. nx1, ny2
33Next higher energy state
- The ball now has same bouncing motion in both x
and in y. - This is higher energy that having motion only in
x or only in y.
(nx, ny) (2,2)
34Three dimensions
- Object can have different velocity (hence
wavelength) in x, y, or z directions. - Need three quantum numbers to label state
- (nx, ny , nz) labels each quantum state (a
triplet of integers) - Each point in three-dimensional space has a
probability associated with it. - Not enough dimensions to plot probability
- But can plot a surface of constant probability.
35Particle in 3D box
- Ground state surface of constant probability
- (nx, ny, nz)(1,1,1)
2D case
36(121)
(112)
(211)
All these states have the same energy, but
different probabilities
37(222)
(221)
38The principal quantum number
- In Bohr model of atom, n is the principal
quantum number. - Arise from considering circular orbits.
- Total energy given by principal quantum number
39Other quantum numbers?
- Hydrogen atom is three-dimensional structure
- Should have three quantum numbers
- Special consideration
- Coulomb potential is spherically symmetric
- x, y, z not as useful as r, ?, ?
Angular momentum warning!
40Sommerfeld modified Bohr model
- Differently shaped orbits
All these orbits have same energy but
different angular momenta Energy is same as Bohr
atom, but angular momentum quantization altered
41Angular momentum question
- Which angular momentum is largest?
42The orbital quantum number l
- In quantum mechanics, the angular momentum can
only have discrete values ,
l is the orbital quantum number - For a particular n,l has values 0, 1, 2, n-1
- l0, most elliptical
- ln-1, most circular
- These states all have the same energy
43Orbital mag. moment
- Since
- Electron has an electric charge,
- And is moving in an orbit around nucleus
- it produces a loop of current,and hence a
magnetic dipole field, very much like a bar
magnet or a compass needle. - Directly related to angular momentum
44Orbital magnetic dipole moment
Can calculate dipole moment for circular orbit
Dipole moment µIA
45Orbital mag. quantum number ml
- Possible directions of the orbital bar magnet
are quantized just like everything else! - Orbital magnetic quantum number
- m l ranges from - l, to l in integer steps
- Number of different directions 2l1
Example For l1, m l -1, 0, or -1,
corresponding to three different directionsof
orbital bar magnet.
l1 gives 3 states
46Question
- For a quantum state with l2, how many different
orientations of the orbital magnetic dipole
moment are there?A. 1B. 2C. 3D. 4E. 5
47- Example For l2, m l -2, -1, 0, 1, 2
corresponding to three different directionsof
orbital bar magnet.
48Interaction with applied B-field
- Like a compass needle, it interacts with an
external magnetic field depending on its
direction. - Low energy when aligned with field, high energy
when anti-aligned - Total energy is then
This means that spectral lines will splitin a
magnetic field
49(No Transcript)
50Summary of quantum numbers
- n describes the energy of the orbit
- l describes the magnitude of angular momentum
- m l describes the behavior in a magnetic field
due to the magnetic dipole moment produced by
orbital motion (Zeeman effect).
51Additional electron properties
- Free electron, by itself in space, not only has a
charge, but also acts like a bar magnet with a N
and S pole. - Since electron has charge, could explain this if
the electron is spinning. - Then resulting current loops would produce
magnetic field just like a bar magnet. - But
- Electron in NOT spinning.
- As far as we know, electron is a point particle.
52Electron magnetic moment
- Why does it have a magnetic moment?
- It is a property of the electron in the same way
that charge is a property. - But there are some differences
- Magnetic moment has a size and a direction
- Its size is intrinsic to the electron, but the
direction is variable. - The bar magnet can point in different
directions.
53Electron spin orientations
Only two possible orientations
54(No Transcript)
55Spin another quantum number
- There is a quantum associated with this
property of the electron. - Even though the electron is not spinning, the
magnitude of this property is the spin. - The quantum numbers for the two states are
- 1/2 for the up-spin state
- -1/2 for the down-spin state
- The proton is also a spin 1/2 particle.
- The photon is a spin 1 particle.
56Include spin
- We labeled the states by their quantum numbers.
One quantum number for each spatial dimension. - Now there is an extra quantum number spin.
- A quantum state is specified four quantum
numbers - An atom with several electrons filling quantum
states starting with the lowest energy, filling
quantum states until electrons are used.
57Quantum Number Question
How many different quantum states exist with
n2? 1 2 4 8
58Pauli Exclusion Principle
- Where do the electrons go?
- In an atom with many electrons, only one electron
is allowed in each quantum state (n,l,ml,ms). - Atoms with many electrons have many atomic
orbitals filled. - Chemical properties are determined by the
configuration of the outer electrons.
59Number of electrons
Which of the following is a possible number of
electrons in a 5g (n5, l4) sub-shell of an
atom? 22 20 17
l4, so 2(2l1)18. In detail, ml -4, -3, -2,
-1, 0, 1, 2, 3, 4and ms1/2 or -1/2 for
each. 18 available quantum states for
electrons 17 will fit. And there is room left
for 1 more !
60Putting electrons on atom
- Electrons are obey exclusion principle
- Only one electron per quantum state
61Other elements Li has 3 electrons
n2 states, 8 total, 1 occupied
n1 states, 2 total, 2 occupiedone spin up, one
spin down
62Electron Configurations
Atom Configuration
H 1s1
He 1s2
1s shell filled
(n1 shell filled - noble gas)
Li 1s22s1
Be 1s22s2
2s shell filled
B 1s22s22p1
etc
(n2 shell filled - noble gas)
Ne 1s22s22p6
2p shell filled
63The periodic table
- Elements are arranged in the periodic table so
that atoms in the same column have similar
chemical properties. - Quantum mechanics explains this by similar
outer electron configurations. - If not for Pauli exclusion principle, all
electrons would be in the 1s state!
64Wavefunctions and probability
- Probability of finding an electron is given by
the square of the wavefunction.
65Hydrogen atom Lowest energy (ground) state
- Spherically symmetric.
- Probability decreases exponentially with radius.
- Shown here is a surface of constant probability
1s-state
66n2 next highest energy
2s-state
2p-state
2p-state
Same energy, but different probabilities
67n3 two s-states, six p-states and
3p-state
3s-state
3p-state
68ten d-states
3d-state
3d-state
3d-state
69Electron wave around an atom
- Electron wave extends around circumference of
orbit. - Only integer number of wavelengths around orbit
allowed.
70Emitting and absorbing light
Zero energy
n4
n4
n3
n3
n2
n2
Photon emittedhfE2-E1
Photon absorbed hfE2-E1
n1
n1
Absorbing a photon of correct energy makes
electron jump to higher quantum state.
- Photon is emitted when electron drops from one
quantum state to another
71The wavefunction
- Wavefunction ? moving to rightgt moving
to leftgt - The wavefunction is an equal superposition of
the two states of precise momentum. - When we measure the momentum (speed), we find one
of these two possibilities. - Because they are equally weighted, we measure
them with equal probability.
72Silicon
- 7x7 surface reconstruction
- These 10 nm scans show the individual atomic
positions
73Particle in box wavefunction
Prob. Of finding particle in region dx about x
Particle is never here
Particle is never here
74Making a measurement
- Suppose you measure the speed (hence, momentum)
of the quantum particle in a tube. How likely
are you to measure the particle moving to the
left? - A. 0 (never)
- B. 33 (1/3 of the time)
- C. 50 (1/2 of the time)