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Atomic X-Ray Spectrometry - Ch12

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Presentation on theme: "Atomic X-Ray Spectrometry - Ch12"— Presentation transcript:

1 Atomic X-Ray Spectrometry - Ch12
Electron Beam Source – a metal target bombarded with a beam of hi-E electrons to produce either a continuum or line spectrum

2 Continuum Source (W target)
Line Source (Mo target) Relationship between o and V (Duane-Hunt Law) Short wavelength limit, o 1. 2. 3.

3 X-Ray Line Spectra Originate From Inner Shell Electrons

4 Radioactive Sources of X-Rays
Radioactivity  electron capture

5 X-Ray Fluorescence (XRF)
X-Ray h from electron beam or radioactive source n=1 n=2 n=3 e-

6 Bragg's Law Used in Wavelength Dispersive instrumentation to construct an x-ray monochromator For constructive interference of scattered beam (wavefront OCD) --

7 Wavelength Dispersive Instrumentation (requires scanning)
X-ray monochromator (“goniometer”)

8 X-ray Detectors Gas-filled Transducers Semi-conductor Transducers
Scintillation Counters Ionization Chambers Proportional Counters Geiger Tubes

9 Wavelength Dispersive Spectrum

10 Single photon counting circuit
Energy Dispersive Instrumentation (no scanning – entire spectrum at once) Single photon counting circuit

11 Photon Counting The output from the detector is fed into a single photon counter circuit - great for the weak signals found with XRF

12 Energy Dispersive Spectrum

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