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Spectroscopic Light Sources
1. Continuum Sources 2. Line Sources 3. Quasi-continuum Sources
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Source Types
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Source Characteristics
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Continuum Sources Emit radiation over a broad spectral range.
Continuum in Wavelength, not necessarily in time. Most of these are “black body emitters. The spectral range depends upon the temperature of the black body.
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Spectral Radiance of a Black Body
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Continuum Sources
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Continuum Sources
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Tungsten Lamps
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1. Absorption Filters Optical material containing an absorber that permits transmission only at certain wavelengths
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Reflection Grating:
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Linear Dispersion Dl Dl = f × Da = dx/dλ where: f = focal length (of monochromator) x = distance (along focal plane)
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Spectral Bandpass (s or Δλ) s = RLD × w where: w = slit width (mm) s in nm Reciprocal Linear Dispersion (RLD) RLD = Dl-1 =dλ/dx nm/mm
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3. Si Photodiode Si: 3s23p2 Covalent Bonds in Solid
Therefore 1/2–filled sp3 ΔE ≤ 2.5 eV (semiconductor) 4 electrons fill a valence band at 0K At higher T an electron can move to conduction band Leaving a positive hole behind (both are mobile)
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3. Si Photodiode Doping Si with a group 5 element (As or Sb) results
in extra electrons (n-type). Doping with a group 3 element (In, Ga) results in extra holes (p-type)
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3. Si Photodiode
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3. Si Photodiode Forward bias (not very useful for spectroscopy)
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3. Si Photodiode Reversed Bias: Depletion zone at the junction.
Photons may eject electrons and form holes Current proportional to number of photons
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3. Si Photodiode 200 – 1000 nm 1-10 ns response time 0.05 A/W
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4. Linear Photodiode Array
200 – 1000 nm 1-10 ns response time 0.05 A/W
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4. Linear Photodiode Array
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