de Broglie Waves de Broglie argued

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Presentation transcript:

de Broglie Waves de Broglie argued Light exhibits both wave and particle properties Wave – interference, diffraction Particle – photoelectric effect, Compton effect Then matter (particles) should exhibit both particle and wave properties He predicted the wavelength to be

de Broglie Waves Consider the E, p relations for a photon Guided by this, de Broglie proposed the same relation for matter

de Broglie Waves

de Broglie Waves Let’s apply de Broglie waves to the Bohr model If the electron is represented as a standing wave in an orbit about the proton This apparently justifies Bohr’s assumption

de Broglie Waves de Broglie wavelength of a person running de Broglie wavelength of a 50 eV electron

X-ray Scattering Before examining electron scattering from a (large) crystal, let’s first look at x-ray scattering from a crystal Spacing of atoms in a crystal ~ 1A Wavelength of “hard” x-rays ~ 0.1-1A Laue therefore expected that interference patterns should be observed And they were! Today, the Laue technique can be used to determine crystal orientation and assess crystal perfection from the size and shape of the spots

X-ray Scattering

X-ray Scattering Laue diffraction of salt

X-ray Scattering Whale myoglobin Of ~35,000 known protein structures, ~29,000 have been identified using x-ray diffraction

X-ray Scattering

X-ray Scattering Powder diffraction Using many small crystals Sometimes single crystals are not available Sometimes materials naturally occur in a polycrystalline state Using many small crystals Their orientation will be random At least a few of the small crystals in the sample will be in the correct orientation to diffract for each of the possible planes The resulting rings are called the Debye-Scherrer pattern The powder diffraction method is frequently used to fingerprint crystals via a large database

X-ray Scattering

X-ray Scattering Debye-Scherrer pattern from powder diffraction for NaCl and KCL

X-ray Scattering Bragg simplified Laue’s three dimensional analysis by considering x-ray scattering as the reflection of the incident beam from successive lattice planes in the crystal If the scattered angle = incident angle (reflection), there is no phase change between the incident and reflected waves Waves scattered at equal angles from atoms in two different planes will constructively interfere if the path length difference is an integral number of wavelengths

X-ray Scattering Crystal structure of NaCl

X-ray Scattering Crystal structure of NaCl

X-ray Scattering Bragg condition The intensity pattern of the scattered waves of a known wavelength gives information about the structure of the crystal The intensity pattern of the scattered waves from a known crystal spacing gives information about the incoming wavelengths Laue and Bragg scattering effectively started the field of solid state physics

X-ray Scattering Crystal structure of NaCl

X-ray Scattering Crystal structure of NaCl

X-ray Scattering Bragg spectrum of NaCl Intensity 2q

X-ray Scattering To determine d To determine n

X-ray Scattering To check d The volume of one atom is d3 for a face-centered cubic crystal

Electron Scattering If x-rays of wavelength ~ 1A produce an diffraction pattern when scattered off a crystal so should matter waves of comparable wavelength For example, 50 eV electrons Davisson and Germer verified this (accidentally)

Electron Scattering Davisson-Germer experiment

Electron Scattering Davisson-Germer data

Electron Scattering

Electron Scattering Bragg’s law applies for electrons too

Electron Scattering Analyzing the Davisson-Germer data Experimental evidence that electrons behave as waves with the de Broglie wavelength

Electron Scattering Aside, these results hold true for even a low intensity electron beam This means that the interference pattern does not result from interference between waves from two electrons, but from waves associated with a single electron Aside, diffraction patterns are also observed using neutrons, H, and He atoms

Electron Scattering Thomson observes diffraction patterns in electron transmission experiments similar to Laue’s in x-ray transmission experiments