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Spectroscopy, continued

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Spectroscopy, continued. S = T4. Planck: Wien: Stefan-Boltzmann: Continuum 'Thermal radiation' ... Heisenberg uncertainty non-zero natural line width ... – PowerPoint PPT presentation

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Title: Spectroscopy, continued


1
Spectroscopy, continued
2
  • Continuum
  • Thermal radiation

Planck
Wien
S ? T4
Stefan-Boltzmann
3
  • Continuum
  • Thermal radiation
  • Bremsstrahlung (free-free)
  • Free-bound, bound-free
  • Synchrotron
  • Multi-temperature population

4
Line formation
5
Line emission
6
Line absorption
7
Spectral lines delta functions? Energies are
discrete, right?
Heisenberg uncertainty ? non-zero natural line
width
But also, what else affects the width/structure
of the spectral line?
8
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9
  • Observing
  • Dispersive element prism/grating/Bragg crystal
  • Dispersion, resolution
  • Detection
  • Signal/noise ratio
  • Ghosts
  • Curvature

10
  • Reflections from crystal lattice planes result in
    interference, yielding monochromatic light.
  • What good is monochromatic? We wanted a
    spectrum.
  • Vary the angle!

11
Na
12
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13
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14
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15
If y.jgt0, j-increases when q increases.
(a, m, l, and j constant)
1
curvature is does not depend on parameters of
grating
qq
16
prism
grating
  • ghosts (due to periodic variations in gratings
    spacing)
  • Lyman (near spectral line)
  • Rowland (at large distance)

17
Order overlap
18
Hg
19
Order overlap
Cross-dispersion!
20
Other observational considerations
  • Slit-filling
  • Multi-slit
  • Slitless

21
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