Interference and Wave-Particle Duality in Quantum Mechanics, Lecture notes of Quantum Mechanics

The concepts of interference, energy quantization, wave-particle duality, and Heisenberg's uncertainty principle in the context of quantum mechanics. Topics include standing waves, nodes and antinodes, beats, and the two-slit interference experiment. New states such as Bose-Einstein condensates are also discussed.

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2021/2022

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INTERFERENCE(&(DIFFRACTION(OF(WAVES(+(3(BASIC(TENETS(OF(QUANTUM(MECHANICS(
What%does%interference%mean?%(Sec3ons%17.1%&%17.5)%
:Construc3ve%and%Destruc3ve%interference%
:Both%Transverse%and%Longitudinal%Waves%interfere%
%%
Standing%Waves%&%the%1st$basic$tenet$of$QM:%Energy%Quan3za3on%
:Standing%Waves%created%by%2%traveling%waves%in%opposite%direc3on;%Nodes%and%An3nodes%%
%(Sec3ons%17.2,%17.3,%Figs.%17.5,%17.6,%17.9)%
:The%energy:levels%of%an%atom%are%quan3zed%(Bohr%model)%because%the%electron%is%a%wave!%(classnotes)%
%%
Beats%&%the%2nd$basic$tenet$of$QM:%Wave:Par3cle%Duality%
:% %Waves%can%behave%like%Par3cles%
oConsider%Beats%(Demo%with%tuning%forks)%(Sec3on%17.8).%
oMany%sinusoidal%waves%added%together%yield%a%wavepacket.%
oTime:dura3on%of%wavepacket%and%frequency%bandwidth%of%the%source%are%related.%
oSpa3al%extent%of%wavepacket%–%deBroglie%wavelength%(Sec3on%38.4%and%39.5)%
oCan%the%deBroglie%wavelength%of%an%electron,%or%of%an%atom,%equal%the%op3cal%wavelength?%
:% %Par3cles%can%behave%like%Waves%
oConsider%the%two:slit%interference%experiment%(Remember%the%“Fabric%of%Cosmos”%video?)%
oElectrons%interfere!%Demo:%Davisson:Germer%expt%
oAtoms%interfere!%New%state%of%Maber%–%Bose:Einstein%condensate%(1997,%2001%Physics%Nobels)%
%
Diffrac3on%and%the%3rd$basic$tenet$of$QM:%Heisenberg%Uncertainty%Principle%(Sec.%39.6)%
:Waves%diffract,%i.e.,%bend%around%obstacles%
Defining%signature%of%waves!%
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INTERFERENCE & DIFFRACTION OF WAVES + 3 BASIC TENETS OF QUANTUM MECHANICS
  • What does interference mean? (Sec3ons 17.1 & 17.5) -­‐ Construc3ve and Destruc3ve interference -­‐ Both Transverse and Longitudinal Waves interfere
  • Standing Waves & the 1 st^ basic tenet of QM: Energy Quan3za3on -­‐ Standing Waves created by 2 traveling waves in opposite direc3on; Nodes and An3nodes (Sec3ons 17.2, 17.3, Figs. 17.5, 17.6, 17.9) -­‐ The energy-­‐levels of an atom are quan3zed (Bohr model) because the electron is a wave! (classnotes)
  • Beats & the 2 nd^ basic tenet of QM: Wave-­‐Par3cle Duality -­‐ Waves can behave like Par3cles o Consider Beats (Demo with tuning forks) (Sec3on 17.8). o Many sinusoidal waves added together yield a wavepacket. o Time-­‐dura3on of wavepacket and frequency bandwidth of the source are related. o Spa3al extent of wavepacket – deBroglie wavelength (Sec3on 38.4 and 39.5) o Can the deBroglie wavelength of an electron, or of an atom, equal the op3cal wavelength? -­‐ Par3cles can behave like Waves o Consider the two-­‐slit interference experiment (Remember the “Fabric of Cosmos” video?) o Electrons interfere! Demo: Davisson-­‐Germer expt o Atoms interfere! New state of Maber – Bose-­‐Einstein condensate (1997, 2001 Physics Nobels)
  • Diffrac3on and the 3 rd^ basic tenet of QM: Heisenberg Uncertainty Principle (Sec. 39.6) -­‐ Waves diffract, i.e., bend around obstacles Defining signature of waves!
INTERFERENCE & DIFFRACTION OF WAVES + 3 BASIC TENETS OF QUANTUM MECHANICS
  • What does interference mean? (Sec3ons 17.1 & 17.5) -­‐ Construc3ve and Destruc3ve interference -­‐ Both Transverse and Longitudinal Waves interfere
  • Standing Waves & the 1 st^ basic tenet of QM: Energy Quan3za3on -­‐ Standing Waves created by 2 traveling waves in opposite direc3on; Nodes and An3nodes (Sec3ons 17.2, 17.3, Figs. 17.5, 17.6, 17.9) -­‐ The energy-­‐levels of an atom are quan3zed (Bohr model) because the electron is a wave! (classnotes)
  • Beats & the 2 nd^ basic tenet of QM: Wave-­‐Par3cle Duality -­‐ Waves can behave like Par3cles o Consider Beats (Demo with tuning forks) (Sec3on 17.8). o Many sinusoidal waves added together yield a wavepacket. o Time-­‐dura3on of wavepacket and frequency bandwidth of the source are related. o Spa3al extent of wavepacket – deBroglie wavelength (Sec3on 38.4 and 39.5) o Can the deBroglie wavelength of an electron, or of an atom, equal the op3cal wavelength? -­‐ Par3cles can behave like Waves o Consider the two-­‐slit interference experiment (Remember the “Fabric of Cosmos” video?) o Electrons interfere! Demo: Davisson-­‐Germer expt o Atoms interfere! New state of Maber – Bose-­‐Einstein condensate (1997, 2001 Physics Nobels)
  • Diffrac3on and the 3 rd^ basic tenet of QM: Heisenberg Uncertainty Principle (Sec. 39.6) -­‐ Waves diffract, i.e., bend around obstacles Defining signature of waves!

Sec. 17.5: 1D Wave Interference in Space w/ Sinusoidal waves

We’ve seen that when two waves add together (superpose), there is a possibility of: Wave 1 Wave 2

Add together perfectly:

ConstrucDve Interference

Or, Wave 1 Wave 2

+ =^

Cancel perfectly:

DestrucDve Interference

In general, when two waves add together, you don’t get anything interes3ng, but these two condiDons are worth a closer look. Twice the amplitude Wave disappears crest to crest crest to trough CHAPTER17_LECTURE17.1 4

Consider two waves with the same amplitude, frequency, and wavelength that both travel in the +x direc3on. x Observer Wave 1 Wave 2 The cat observes the combined wave, and the way the waves combine at his loca3on is totally determined by the phase difference. Perfect ConstrucDve Interference for: Perfect DestrucDve Interference for: At the loca3on of the cat: Sec. 17.5: 1D Wave Interference in Space w/ Sinusoidal waves CHAPTER17_LECTURE17.1 5

x / 0. Can do either or

Whiteboard Problem 1

Δ CHAPTER17_LECTURE17.^

8

CHAPTER17_LECTURE17. 10

Sec. 17.7 Interference in Space in 2D and 3D

Observer Source 1 Source 2 As we did for 1D, consider two waves of the same amplitude and frequency in 2D: wavefronts Again, the cat observes the combined wave and, the way the waves combine depends on their phase. The phase difference depends on the path difference and the ini3al phase. ConstrucDve Interference: DestrucDve Interference: Note: these are the same condi3ons that we had for 1D, but x is replaced with r. The big difference here is in the geometry. CHAPTER17_LECTURE17.1^11

Sec. 17.7 Whiteboard Problem 3

wavefronts r 1 r 2 r C / D P 3 4 C Q 3.5 2 1.5 D R 2.5 3.5 C r = 0 along this line The fact that construc3ve interference is seen along this line indicates the 2 sources are in phase.

λ λ^ λ

λ λ^ λ

Δ Δ CHAPTER17_LECTURE17.1 13

Sec. 17.7: 2D Interference PaZerns in Space

If you extend WB Problem 3 over the en3re 2D plane, you get paberns of interference. Shown below are interference paberns for Two In-­‐Phase Sources : an3nodes nodes Remember, these are waves, so they’re moving! CHAPTER17_LECTURE17.1 14