ee138 chapter 8-slides
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UCR EE138TRANSCRIPT
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Chapter 8 1
OutlineReading: Livingston, Chapter 8.1-8.7
• Planck’s Constant• Wave-Particle Duality of Light• Wave-Particle Duality of Electrons• Wave-Particle Duality: Momentum and Energy• Schrodinger’s Equation• Probability Density• Case 1: Free Electron• Heisenberg’s Uncertainty Principle• Case 2: Potential Barrier (E<V)• Case 3: Potential Barrier (E>V)• Case 4: Tunneling• Case 5: Infinite Potential Well• Case 6: Finite Potential Well
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Chapter 8 22
DiffractionWhat if wavelength of light ~ periodic atomic spacing?
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Chapter 8 3
Planck: Energy of Electromagnetic Wave
λυ hchE ==
ω=E
Planck’s Constant: 6.626 x 10-34 J-s
""2
barhh −==π
Relationship between energy and frequency:
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Chapter 8 4
Wave-Particle Duality of Light
http://phet.colorado.edu/en/simulation/photoelectric
1. Photoelectric Effect: e- ejected from mat’l surface when exposed to light
2. Compton Scattering: increase in the wavelength of light scattered by an e-
Effects which are NOT explained by wave properties:
particle-particle collision:electron and photon (light particle)
increase λ, decrease in EλhcE =
λhp =
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Chapter 8 5
Wave-Particle Duality of ElectronsIf light can act as particles, can electrons act as waves?
de Broglie’s Hypothesis: e- can have wave-like nature defined by p = mvand p = h/λDavisson and Germer Experiment:
θλ sin2dn =Bragg’s Law of Diffraction:If e- is a wave and λ~d, diffraction should be observed.
For an e- with an applied V, the energy is E= eV.
Need to apply correct V.
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Chapter 8 6
Wave-Particle Duality: Momentum and Energy
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Chapter 8 7
Example: Wave-Particle Duality
Calculate the wavelength of a 50 g golf ball traveling at a velocity of 20 m/s.
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Chapter 8 8
Schrodinger’s Equation: Electron Wave Equation
dtdiV
mΨ=Ψ+Ψ∇−
22
2z
ky
jx
i∂∂+
∂∂+
∂∂=∇
)(),,(),,,( tzyxtzyx ωψ=ΨManipulate equation so that it is easier to use:
Remember:
Separate variables:
dtdiV
mωψψωψω
=+∇− 22
2
Divide by ωψ:dtdiV
mω
ωψ
ψ =+∇− 2
2
2
LHS and RHS must equal constant, “E”:dtdiE ω
ω=
= ωω
diEdt
tiiEt
eet ωω −−
== )(
ω=E
ψψψ EVm
=+∇− 22
2 Time-independent Schrodinger’s Equation
(stationary states)
Multiply by ψ:
m = mass of electronV = potential energy of electron
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Chapter 8 9
Schrodinger’s Equation: Electron Wave Equation (cont.)
ψψψ EVm
=+∇− 22
2 Time-independent Schrodinger’s Equation
(stationary states)
ψψψ EEPEK =+ ....
mpEK2
..2
=
∇−= ipMomentum operator:
Please just believe for now…
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Chapter 8 10
Probability DensityElectron is BOTH particle AND wave = “fuzzy” in time and space
z
ΨΨ *
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Chapter 8 11
Case 1: Free ElectronE
V(z)=0
z
ΨΨ *
1 Dimension
ψψψ EVm
=+∇− 22
2
)(),,(),,,( tzyxtzyx ωψ=Ψ Time-dependent Scrodinger’s Equation
)()(),( kztikzti BeAetx +−−− +=Ψ ωω
22* BA +=ΨΨ
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Chapter 8 12
Heisenberg’s Uncertainty Principle
z
ΨΨ *infinite uncertainty in position
hzp ≥ΔΔ
Electron is BOTH particle AND wave = “fuzzy” in time and space
mkE
2
22=kp =
Other forms of uncertainty principle:
≥ΔΔ zp
htE ≥ΔΔ
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Chapter 8 13
Example
Laser light is normally monochromatic. However, when the pulse time becomes sufficiently short, the energy range can broaden to cover the entire range of visible light (and a laser beam becomes white). Below what pulse time will this phenomenon occur?
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Chapter 8 14
Case 2: Potential Barrier (E<V)
14
1 Dimension
ψψψ EVm
=+∇− 22
2
EV=Vo
z=0
Region 1 Region 2
Region 1:zikzik BeAex 11)(1
−+=ψ
mEk 21 =
Solutions to time-independent Schrodinger’s Equation
Region 2:zikzik DeCex 22)(2
−+=ψ ( )
oVEmk
−=
22
Boundary conditions:
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Chapter 8 1515
Case 2: Potential Barrier (E<V) (cont.)
ψψψ EVm
=+∇− 22
2
EV=Vo
z=0
Region 1 Region 2
Interface Continuity
1 Dimension
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Chapter 8 16
Case 3: Potential Barrier (E>V)
16
1 Dimension
ψψψ EVm
=+∇− 22
2
EV=Vo
z=0
Region 1 Region 2
Region 1:zikzik BeAex 11)(1
−+=ψ
mEk 21 =
Solutions to time-independent Schrodinger’s Equation
Region 2:zikzik DeCex 22)(2
−+=ψ ( )
oVEmk
−=
22
Boundary conditions: E>Vo , no reflected wave from right side, D=0zikCex 2)(2 =ψ
K2 is REAL!!!
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Chapter 8 17
Case 3: Potential Barrier (E>V)
17
1 Dimension
ψψψ EVm
=+∇− 22
2
EV=Vo
z=0
Region 1 Region 2
Interface Continuity
@ x = 0, ψ1=ψ2 CBA =+
@ x = 0,dz
ddz
d 21 ψψ = ( ) CkBAk 21 =−
VEEVEE
kkkk
AB
−+−−=
+−=
21
21
VEEE
kkk
AC
−+=
+= 22
21
1
)*()*(
1
1
AAkBBkR =
)*()*(
1
2
AAkCCkT =
zikzikzik CeBeAe 211 =+ −
zikzikzik eCikeBikeAik 211211 =− −
Ratio of reflected toincident amp
Reflection Coeff
Transmission CoeffRatio of transmitted toincident amp
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Chapter 8 18
Example• What do you expect
classically?• What do you expect based
on quantum mechanics?• Calculate the reflection
coefficient for the matter wave.
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Chapter 8 19
Example (cont.)• What do you expect
classically?• What do you expect based
on quantum mechanics?• Calculate the reflection
coefficient for the matter wave.
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Chapter 8 20
Case 4: Tunneling (E<V)
20
1 Dimension
ψψψ EVm
=+∇− 22
2
Region 1:zikzik BeAex 11)(1
−+=ψ
mEk 21 =
Solutions to time-independent Schrodinger’s Equation
Region 2:( )
oVEmk
−=
22
Region 3:zikFex 1)(3 =ψ
mEk 21 =
zikzik DeCex 22)(2−+=ψ
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Chapter 8 21
Review
E
V(z)=0
EV=Vo
z=0
Region 1 Region 2
EV=Vo
z=0
Region 1 Region 2
1. What would you expect to happen classically?2. What happens quantum mechanically?
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Chapter 8 22
Case 5: Infinite Potential Well
22
z=0 z=L
V=infinity V=infinityV=0
ψψψ EVm
=+∇− 22
2
Solutions to time-independent Schrodinger’s Equation
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Chapter 8 23
Case 5: Infinite Potential Well (cont.)
2
22
8mLhnEn =
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Chapter 8 24
Example
1. Sketch a plot of n versus E for an infinite potential well.2. If the width of the well increases by a factor of 2, how
does the energy change?
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Chapter 8 25
Pauli’s Exclusion PrincipleRule of quantum mechanics that allows only two electrons (one spin up and one spin down) to fill each energy level
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Chapter 8 26
Case 6: Finite Potential Well (Quantum Well) How do energy wavelength and energy levels change qualitatively if potential barriers are not infinite?
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Chapter 8 27
Review Questions
1. Name and explain two experiments that showed photons are particles.
2. Name and explain an experiment that showed electrons are waves.3. What relationship did Planck find between frequency and energy?
Momentum and wavelength?4. How are momentum and energy treated differently for particles and
waves?5. What is the physical meaning of wave function?6. What is Schrodinger’s Equation (S.E.)? What does each term
represent?7. What are general solutions to the time-dependent and time-
independent S.E.? What is the relationship between E and k?8. Give the general procedure for solving S.E. for a potential profile.9. What is Heisenberg’s Uncertainty Principle tell us?
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Chapter 8 28
More Review Questions
1. What are the allowed energies for an infinite potential well?
2. What is the ground state energy?3. What are the excited energy levels?4. How many electrons per energy level?5. How to electrons move and down in energy levels?6. If the potential barriers are made finite, how do the
energy levels and wavelength change?
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Chapter 8 29
Important Equations
λυ hchE ==ω=E
Planck’s Constant: 6.626 x 10-34 J-s
π2h=
λhp = vmp =
2v2mE =
θλ sin2dn =
dtdiV
mΨ=Ψ+Ψ∇−
22
2ψψψ EV
m=+∇− 2
2
2
tiiEt
eet ωω −−
== )(
mE
2p2
=
ψψ *_ =distribprob
kp =
mkE
2
22=
hzp ≥ΔΔ htE ≥ΔΔ
zikzik BeAex 11)(1−+=ψ
VEEVEE
kkkk
AB
−+−−=
+−=
21
21
VEEE
kkk
AC
−+=
+= 22
21
1
)*()*(
1
1
AAkBBkR =
)*()*(
1
2
AAkCCkT =
mLhnEn 8
22
=
= z
LnAnn
πψ sin ( )2228 fiif nn
mLh
hE −=Δ=ν...3,2,1=n