Chem 454
Feb 28, 2001
X-Rays and Atomic Spectra
X-rays defined 0.1-100 A
non-optical (no lenses, mirrors)
source: inner electron transitions
- typically to vacant n=1 (1s)
- or to vacant n=2 (2s, 2p)
- becomes vacant by high energy electron impact
- perhaps vacant by radioactive decay
- perhaps vacant due to exposure to radioactive element
- (no possibility of thermal or chemical reaction as source)
rough rule: Bohr Atom
- E = -13.6 eV Z2 / n2
-
really want Z-0.3 for 1s (screening)
- want about Z- 3 for 2s, 2p
- but really those changes won't affect our estimates
for Ca, Z=20
- E(1s) = 400 x 13.6 = 5440 eV
- E(2p) = (400) x 13.6 /2 = 1000 eV
- 2p-->1s is about 4400 eV
- wavelength = 12398 A / (V or eV)
- wavelength is about 3 A
- this is a K transition (into n=1 shell)
- 3p-->1s is a bit more energetic
- E(3p) = "400"X13.6 / 9 = 400 eV
- transition is 5000 eV
- wavelength is with shorter
- Kb
- for Z=40 can expect about 4x energy, 1/4 wavelength
- generally wavelength, energy unique to atomic species
L transitions are much lower in energy
- from 3p or 4 p
- into 2s
- E(2s) = 1/4 E (1s)
- E(3s) = 1/9 E (1s)
- 3p-->2s is (1/4-1-/9) Es =0.15 E(1s)
- 2p -->1s was 0.75 E(1s)
- so La is about 1/5 energy or 5* wavelength
Uses of X-rays
-
diffraction-- important, later in text
- molecule or crystal is diffraction grating
- pattern gives spacing (mol dimension, geometry)
- absorption
- some, but very specialized
- imaging
- based on relatively low absorption, but some
- ionization sources
monitoring emission by samples
must be able to produce
- must be able to detect
- must be able to measure wavelength or energy
Detection-- through ionization
- directly: gas, high voltage, measure current
- directly: gas, high voltage, one current pulse/particle
- directly: solid state, measure pulse
- indirectly: photographic film, phosphors (scintillation)
-
- generally E(X-ray) >> Ionization potential
- get many electrons
- solids, could absorb completely
- energy is proportional to pulse height
- energy discriminating detection
- Typical detector Si or Ge, cooled with liq N2, 2-6" in size
Dispersive methods
- grating (based on a crystal)
- wavelength selection, then detection
Cleaning Up X-Rays
- Absorption spectra typically show sharp edges
- Represent onset of a transition
- Filter made of lower MW metal
- can remove lower energy radiation
- can isolate a K lines (remove L and background)
- simple, helpful, but crude
- Grating to select wavelength
- Live with the background (corrections)
Producing X-Rays
- Some radioactive elements
- produce their own X-rays
- or beat up target atoms
- X-Ray tubes
- accelerate electrons beam (4-20 KV)
- electrons slam into target
- produce complex radiation
- Bremstrahlen (continuum)
- Atomic Emission lines
- characteristic of the target
- X-Ray Fluorescence
- short wavelength X-ray source; aim at sample
- monitor longer wavelengths from sample
- Scanning Electron Microscopes
- again, electron beam
- carefully focused
- Particle Accelerators
- important research sites
- high energy, intense, focused, more monochromatic
X-ray Fluorescence
- Generally use an Energy Dispersive Detector
- Portable units often use radioactive source
- Lab Units often favor an X-Ray source
SEM Scanning Electron Microscope
- Tightly focused electron beam
- maneuvered by magnetic coils (lenses)
- scanned across sample
- raster scan (image pixel by pixel)
- Mode 1-- Backscattered electrons
- electrons collected, current measured
- made brightness at that pixel
- plotted as 2D image
- shows morphology
- Mode 2 -- Energy dispersive Detector
- measures X-rays produced
- decides which signals to display
- all, all above xxx A
- only that for one element
- produces a more discriminating image
-
- Intensity is measure of composition of sample
- Analysis in area of 10-50 A is possible
-
- Analysis limited to near surface
- X-rays penetrate
- Electrons stopped in first few atoms
- So X-rays originate in first few atomic layers
-
- Sometimes, etch surface to see successive layers
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