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Kapitza-Dirac Effect: Electron Diffraction from a Standing Light Wave

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... mercury lamp only allows 10-14 electrons to diffract. 1960. Invention of Laser ... Electrons diffract from a standing wave of light (laser bouncing off mirror) ... – PowerPoint PPT presentation

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Title: Kapitza-Dirac Effect: Electron Diffraction from a Standing Light Wave


1
Kapitza-Dirac EffectElectron Diffraction from a
Standing Light Wave
Physics 138 SP05 (Prof. D. Budker)
Victor Acosta
2
Contents
  • History
  • Introduction
  • Basic Setup/Results
  • Theory
  • Multi-Slit Analogy
  • Particle Interaction Picture
  • QM Treatment
  • U. Nebraska 2001 Results
  • Applications

3
History
  • 1804
  • Young Proposes Double Slit Experiment
  • Wave nature of Light
  • 1905
  • Einstein Photoelectric Effect
  • Particle nature of Light
  • 1927
  • Davisson and Germer Electron Diffraction
    (crystalline metal)
  • Wave nature of matter
  • 1930
  • Kapitza and Dirac propose KDE
  • Light Intensity of mercury lamp only allows 10-14
    electrons to diffract
  • 1960
  • Invention of Laser
  • First Real Attempts at KDE
  • All 4 were unsuccessful (poor beam quality?
    Undeveloped Theory?)
  • 2001
  • KDE seen by U. Nebraska group

4
Introduction to Kapitza-Dirac Effect (KDE)
Figure 1. Adapted from Kapitza and Dirac's
original paper. Electrons diffract from a
standing wave of light (laser bouncing off
mirror). Figure from Bataleen group (U.
Nebraska).
Analogy) KDE Multi-Slit Diffraction Electron
Beam incident wave Light Source grating
5
Basic Setup/Results
Data for atom diffraction from a grating of
light taken at the University of Innsbruck.
Diffraction peak separation 2 photon recoil
momenta. Figure from Bataleen group (U.
Nebraska).
6
Analogy Multiple-Slit Diffraction
Detector
?
d
d
Assume outgoing waves propagate at ? w.r.t
grating axis (zgtgtd).
Path Length Difference (PLD) dSin? Bragg
Condition satisfied iff PLD n? ? dSin? n?
z
7
Figure from Bataleen group (U. Nebraska).
8
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9
Quantum Mechanical Theory
  • Need full QM treatment to understand nature of
    diffraction peaks
  • First find H using Classical EM
  • Then solve Time-Dependent Schroedinger Equation

10
Figure from Bataleen group (U. Nebraska).
11
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12
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13
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14
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15
Legend Bragg Regime (Top) Raman-Nath
(Bottom) n0 (red) n1 (blue) n2 (green)
16
Figure from Bataleen group (U. Nebraska).
17
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18
Figure from Bataleen group (U. Nebraska).
19
U. Nebraska 2001 Results Raman-Nath Regime
Laser off (Top) and Laser on (bottom) Plaser 10
W Ilaser 271 GW/cm2 Vp 7.18 meV. Eo 5.31
µeV Ve.0367c
20
U. Nebraska 2001 Results Bragg Regime
Laser off (Top) and Laser on (bottom) Plaser
1.4 W Ilaser 0.29 GW/cm2 Vp 7.66 µeV. Eo
5.31 µeV Ve.0367c
21
Applications
  • Coherent Electron Beam Splitter
  • Electron Interferometry
  • Greater Sensitivity than Atomic Version
  • ?electron 10-11 gt .1?atom
  • Low electron energies possible
  • Microscopic Stern-Gerlach Magnet?
  • Would separate Electrons by spin
  • Need light grating that isnt standing wave
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