x-rays 10 12 10 6 10 3 10 1 10 -1 10 -3 long wave ir visible uv x-rays gamma rays wavelength (nm)...
TRANSCRIPT
![Page 1: X-rays 10 12 10 6 10 3 10 1 10 -1 10 -3 Long Wave IR Visible UV X-rays Gamma rays wavelength (nm) Frau Röntgen's hand](https://reader035.vdocument.in/reader035/viewer/2022070307/551b86cb550346942b8b4b11/html5/thumbnails/1.jpg)
X-raysX-rays
1012 106 103 10 1 10-1 10-3
Long Wave IR Visible UV X-rays Gamma rays
wavelength (nm)
Frau Röntgen's handFrau Röntgen's hand
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1012 106 103 10 1 10-1 10-3
Long Wave IR Visible UV X-rays Gamma rays
wavelength (nm)
X-raysX-rays
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X-ray tubeX-ray tube
water inlet
filament (cathode)
target (anode)
x-ray window
focusing cup
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water inlet
filament (cathode)
target (anode)
x-ray window
focusing cup
X-ray tubeX-ray tube
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X-raysX-rays
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X-raysX-rays
White radiation
Produced upon "collisions" with electrons in target
Any amount of energy can be lost up to a max. amount
Continuous variation of wavelength
Characteristic radiation
Specific energies absorbed
Specific x-ray wavelengths emitted
Wavelengths characteristic of target atom type
White radiation
Produced upon "collisions" with electrons in target
Any amount of energy can be lost up to a max. amount
Continuous variation of wavelength
Characteristic radiation
Specific energies absorbed
Specific x-ray wavelengths emitted
Wavelengths characteristic of target atom type
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X-raysX-rays
Mechanism
Decelerating charges give off radiation
Mechanism
Decelerating charges give off radiation
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X-raysX-rays
Mechanism
Decelerating charges give off radiation
Mechanism
Decelerating charges give off radiation
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X-raysX-rays
Mechanism
Decelerating charges give off radiation
Mechanism
Decelerating charges give off radiation
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X-raysX-rays
Mechanism
Decelerating charges give off radiation
Mechanism
Decelerating charges give off radiation
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X-raysX-rays
Mechanism
Decelerating charges give off radiation
Mechanism
Decelerating charges give off radiation
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X-raysX-rays
Typical tube spectrumTypical tube spectrum
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X-rays - vary tube voltageX-rays - vary tube voltage
Inte
nsi
ty
Wavelength
E ≈ hc/Kedge
E >> hc/Kedge
E > hc/Kedge
Iconts = AiZV~2
Ichar = Ai(V-Vcrit)~1.5
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X-raysX-rays
More electron transitionsMore electron transitions
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X-raysX-rays
Cu spectrumCu spectrum
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X-raysX-rays
Al spectrumAl spectrum
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X-raysX-rays
Au L spectrumAu L spectrum
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X-raysX-rays
Moseley's law - energy vs. atomic numberMoseley's law - energy vs. atomic number
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X-ray sourcesX-ray sources
Sealed tubes - Coolidge typecommon - Cu, Mo, Fe, Cr, W, Ag
Sealed tubes - Coolidge typecommon - Cu, Mo, Fe, Cr, W, Ag
Ka = (2 Ka1 + Ka2)/3Ka = (2 Ka1 + Ka2)/3
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X-ray sourcesX-ray sources
Sealed tubes - Coolidge typecommon - Cu, Mo, Fe, Cr, W, Agintensity limited by cooling requirements (2-
2.5kW)(~99% of energy input converted to
heat)
Sealed tubes - Coolidge typecommon - Cu, Mo, Fe, Cr, W, Agintensity limited by cooling requirements (2-
2.5kW)(~99% of energy input converted to
heat)
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X-ray sourcesX-ray sources
Intensity changes with take-off angleIntensity changes with take-off angle
But resolution decreases with take-off angleBut resolution decreases with take-off angle
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X-ray sourcesX-ray sources
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Other X-ray sourcesOther X-ray sources
Rotating anode
high power - 40 kWdemountablevarious anode types
Rotating anode
high power - 40 kWdemountablevarious anode types
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Other X-ray sourcesOther X-ray sources
Synchrotron need electron or positron beam orbiting in a
ringbeam is bent by magnetic field
x-ray emission at bend
Synchrotron need electron or positron beam orbiting in a
ringbeam is bent by magnetic field
x-ray emission at bend
Advantages
10-4 - 10-5 radians divergence (3-5 mm @ 4 m)
Advantages
10-4 - 10-5 radians divergence (3-5 mm @ 4 m)
high brilliancewavelength tunablehigh brilliancewavelength tunable
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Other X-ray sourcesOther X-ray sources
Synchrotron
Advantages
10-4 - 10-5 rad divergence (3-5 mm @ 4 m)
high brilliancewavelength tunable
Synchrotron
Advantages
10-4 - 10-5 rad divergence (3-5 mm @ 4 m)
high brilliancewavelength tunable
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Other X-ray sourcesOther X-ray sources
Synchrotron need electron or positron beam orbiting in a
ringbeam is bent by magnetic field
x-ray emission at bend
Advantages
10-4 - 10-5 rad divergence (3-5 mm @ 4 m)
high brilliancewavelength tunable
high signal/noise ratio
Synchrotron need electron or positron beam orbiting in a
ringbeam is bent by magnetic field
x-ray emission at bend
Advantages
10-4 - 10-5 rad divergence (3-5 mm @ 4 m)
high brilliancewavelength tunable
high signal/noise ratio
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X-ray sourcesX-ray sources
Synchrotron
Advantages
10-4 - 10-5 rad divergence (3-5 mm @ 4 m)
high brilliancewavelength tunable
Synchrotron
Advantages
10-4 - 10-5 rad divergence (3-5 mm @ 4 m)
high brilliancewavelength tunable
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X-ray sourcesX-ray sources
Synchrotron
Advantages
10-4 - 10-5 rad divergence (3-5 mm @ 4 m)
high brilliancewavelength tunable
Synchrotron
Advantages
10-4 - 10-5 rad divergence (3-5 mm @ 4 m)
high brilliancewavelength tunable
![Page 29: X-rays 10 12 10 6 10 3 10 1 10 -1 10 -3 Long Wave IR Visible UV X-rays Gamma rays wavelength (nm) Frau Röntgen's hand](https://reader035.vdocument.in/reader035/viewer/2022070307/551b86cb550346942b8b4b11/html5/thumbnails/29.jpg)
Beam conditioningBeam conditioning
CollimationCollimation
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Beam conditioningBeam conditioning
Monochromatization
-filters – materials have atomic nos. 1 or 2 less than anode
50-60% beam attenuationplacing after specimen/before detector
filters most of specimen fluorescenceallows passage of high intensity & long
wavelength white radiation
Monochromatization
-filters – materials have atomic nos. 1 or 2 less than anode
50-60% beam attenuationplacing after specimen/before detector
filters most of specimen fluorescenceallows passage of high intensity & long
wavelength white radiation
X-raysX-rays
detectordetectorfilterfilter
specimenspecimen
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Beam conditioningBeam conditioning
Monochromatization
-filters – materials have atomic nos. 1 or 2 less than anode
50-60% beam attenuationplacing after specimen/before detector
filters most of specimen fluorescenceallows passage of high intensity & long
wavelength white radiation
Monochromatization
-filters – materials have atomic nos. 1 or 2 less than anode
50-60% beam attenuationplacing after specimen/before detector
filters most of specimen fluorescenceallows passage of high intensity & long
wavelength white radiation
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Beam conditioningBeam conditioning
Monochromatization
Crystal monochromators – LiF, SiO2, pyrolytic graphite
critical – reflectivity ex: for MoK, LiF 9.4% graphite 54 %
Monochromatization
Crystal monochromators – LiF, SiO2, pyrolytic graphite
critical – reflectivity ex: for MoK, LiF 9.4% graphite 54 %
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Beam conditioningBeam conditioning
Monochromatization
Crystal monochromators – LiF, SiO2, pyrolytic graphite
critical – reflectivity ex: for MoK, LiF 9.4% graphite 54 %
resolution – determines peak/bkgrd ratio & spectral purity best - Si – 10"
graphite – 0.52°
Monochromatization
Crystal monochromators – LiF, SiO2, pyrolytic graphite
critical – reflectivity ex: for MoK, LiF 9.4% graphite 54 %
resolution – determines peak/bkgrd ratio & spectral purity best - Si – 10"
graphite – 0.52°
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Beam conditioningBeam conditioning
Monochromatization
Monochromator shape
usually flat – problems with divergent beams
concentrating type – increases I by factor of 1.5-2
Monochromatization
Monochromator shape
usually flat – problems with divergent beams
concentrating type – increases I by factor of 1.5-2