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X-ray sources and optics Dimosthenis Sokaras SLAC National - - PowerPoint PPT Presentation
X-ray sources and optics Dimosthenis Sokaras SLAC National - - PowerPoint PPT Presentation
X-ray sources and optics Dimosthenis Sokaras SLAC National Accelerator Laboratory Electromagnetic Waves Spectrum: X-rays Energy 0.1-100 keV Wavelength X-rays Interaction with Matter Properties for the interaction of X-ray with
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X-rays Interaction with Matter
Properties for the interaction of X-ray with matter are theoretically described with this Hamiltonian interaction absorption/ emission scattering
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X-ray Sources: Motivation – Aim in Research
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X-ray Sources: Principles for X-ray Emission Main Mechanisms for X-ray Sources Ø Characteristic X-rays
Ø Relaxation of atomic excited states
Ø Acceleration of charged particles
Ø Synchrotron Radiation Ø Bremsstrahlung Radiation Ø Plasma sources
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Properties for an X-ray source
Performance Properties
- energy content
- flux
- Beam size
- angular convergence
- stability
- polarization
- time domain
- Coherence
Practical Properties
- Cost
- Availability/Access
- Portability ?
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X-ray Sources: X-ray Tubes Characteristic X-rays based Sources: Ø Ionization of Primary Targets by means of irradiation:
Ø Heavy ions (Electrostatic Accelerators) Ø Electrons (X-ray Tubes, e- accelerators)
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X-ray Sources: X-ray Tubes Characteristic X-rays based Sources: Ø X-ray Tubes Ø 1% of power becomes x-rays Ø Limitation = heat of the anode Ø Few W to several kW Ø Few to tens of keV photons Ø 4π emission
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X-ray Sources: X-ray Tubes Characteristic X-rays based Sources: Ø X-ray Tubes
Ø Fixed anode tube Ø Rotating Anode Ø Liquid Metal Anode
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X-ray Sources: X-ray Tubes Characteristic X-rays based Sources: Ø X-ray Tubes
Ø Fixed tube Ø Rotating Anode Ø Liquid Metal
Acta Cryst. (2013). D 69 , 1283–1288
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X-ray Sources: Synchrotron Radiation Synchrotron Radiation based Sources: Ø Storage Rings
Ø Large Scale Laboratories Ø Relativistic Electrons/Positrons (1-7 GeV) Ø Acceleration Magnetic Field Ø Insertion Devices Ø Emission cone in forward angles
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X-ray Sources: Synchrotron Radiation Synchrotron Radiation based Sources: Ø Storage Rings
Ø Bending Magnets (~1011 photons/s) Ø Wigglers (~1013 photons/s) Ø Undulators (~1014 photons/s)
Ø Properties
Ø Unprecedented flux Ø Very broad energy range Ø Forward emission / small divergence Ø Polarization
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X-ray Sources: Synchrotron Radiation Synchrotron Radiation based Sources: Ø Storage Rings
Ø Bending Magnets (~1011 photons/s) Ø Wigglers (~1013 photons/s) Ø Undulators (~1014 photons/s)
Ø Properties
Ø Unprecedented flux Ø Broad Energy range Ø Forward emission Ø Polarization
1.0E+12 1.0E+13 1.0E+14 1.0E+15 1.0E+16 2000 4000 6000 8000 10000 12000 14000 16000 18000 20000 flux (cps/0.1% bp 1.0x0.2mrad or central cone) energy (eV) BL12 ¡ BL6 ¡ BL4 ¡ BL14 ¡ SSRL, T. Rabedeau
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X-ray Sources: X-ray Free Electron Laser
Undulator Very long Undulator - XFEL Uncorrelated electron positions / radiated fields Microbunching by own radiated fields strongly correlated waves of electron and fields
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X-ray Sources: X-ray Free Electron Laser Ø X-ray Free Electron Laser
Ø (~1025 photons/s)
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X-ray Sources: Brilliance Quality Factor for X-ray Sources Brilliance = Radiated power per unit area per unit solid angle per unit spectral bandwidth Unit → photons/s/mrad2/mm2/0.1%bandwith
Brilliance → ¡ ¡Invariant quantity ¡
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X-ray Sources: Brilliance
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X-ray Sources: Natural Sources Natural X-ray Sources: Ø Radioisotopes (241Am, 55Fe, 109Cd, etc.) Ø Stars, Super Novas, Cosmic Background
An X-ray image of the Sun, T~2·106K
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X-ray Sources: Motivation – Aim in Research
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X-ray Optics: Delivering X-rays for Experiments
Transferring x-ray photons (beam) to the sample:
- focus size
- energy content
- angular convergence
- stability
- polarization
The job of x-ray optics is to transform the source beam characteristics to provide the best possible match to the sample requirements.
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X-ray Optics: Principles X-rays Interaction Mechanisms for Optics:
Ø X-ray Diffraction ( monochromatizing x-rays) Ø X-ray Refraction/Reflection (guiding/collimating)
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X-ray Optics: Refractive Index
Refractive index
phase term attenuation term
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X-ray Optics: Refraction
Snell Law:
n<1
Refraction
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X-ray Optics: Total External Reflection
Total external reflection δ ~ 10-5-10-6 θc< 3o-4o
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X-ray Optics: X-ray Mirrors
Focusing
condense beam to source dimensions on sample demagnify source image to better couple photons on small sample at the expense of greater angular convergence
- n sample)
Collimation
collimate divergent beam to improve energy resolution of a monochromator
Power filter
absorb waste power at low power density on grazing incident optic
Harmonic filter
suppress higher energy contamination of beam (low pass filter)
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X-ray Optics: X-ray Mirrors
Focusing
condense beam to source dimensions on sample demagnify source image to better couple photons on small sample at the expense of greater angular convergence
- n sample)
Collimation
collimate divergent beam to improve energy resolution of a monochromator
Power filter
absorb waste power at low power density on grazing incident optic
Harmonic filter
suppress higher energy contamination of beam (low pass filter)
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X-ray Optics: X-ray Mirrors
Focusing
condense beam to source dimensions on sample demagnify source image to better couple photons on small sample at the expense of greater angular convergence
- n sample)
Collimation
collimate divergent beam to improve energy resolution of a monochromator
Power filter
absorb waste power at low power density on grazing incident optic
Harmonic filter
suppress higher energy contamination of beam (low pass filter)
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X-ray Optics: X-ray Mirrors
Focusing
condense beam to source dimensions on sample demagnify source image to better couple photons on small sample at the expense of greater angular convergence
- n sample)
Collimation
collimate divergent beam to improve energy resolution of a monochromator
Power filter
absorb waste power at low power density on grazing incident optic
Harmonic filter
suppress higher energy contamination of beam (low pass filter)
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X-ray Optics: X-ray Mirrors
Focusing
condense beam to source dimensions on sample demagnify source image to better couple photons on small sample at the expense of greater angular convergence
- n sample)
Collimation
collimate divergent beam to improve energy resolution of a monochromator
Power filter
absorb waste power at low power density on grazing incident optic
Harmonic filter
suppress higher energy contamination of beam (low pass filter)
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X-ray Optics: X-ray Mirrors
Focusing
condense beam to source dimensions on sample demagnify source image to better couple photons on small sample at the expense of greater angular convergence
- n sample)
Collimation
collimate divergent beam to improve energy resolution of a monochromator
Power filter
absorb waste power at low power density on grazing incident optic
Harmonic filter
suppress higher energy contamination of beam (low pass filter)
0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 5 10 15 20 25 30 35 40
energy (keV) reflectivity
Si Rh Pt 2.7mrad alpha
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X-ray Optics: X-ray Diffraction
Bragg Diffraction: Constructive interference of radiation reflections from sequential planes. ) sin( = θ d λ m 2
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X-ray Optics: X-ray Diffraction
- Diffraction Gratings
- Bragg-type x-ray crystal optics
soft x-rays hard x-rays
2dhkl sin θ = λ mλ d = (sin α + sin β)
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X-ray Optics: X-ray Diffraction - Darwin Width
- Energy Resolution- Darwin width (dynamical diffraction
theory) and geometrical factors
- Darwin width curves
2d sin θ = λ λ ∆λ = tan θ ∆θ
(arcsec)
kin
- 100
- 50
50 100 150 200
reflectivity
0.2 0.4 0.6 0.8 1
Darwin width for Si(440) @ 88 deg
65meV @ 6462eV
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X-ray Optics: Double Crystal monochromators
Liquid Nitrogen Cooled Monochromators cooling channel bundle
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X-ray Optics: Double Crystal Monochromators - Dupond and Acceptance Diagram
12380 12400 12420 12440 12460 12480 12500 14.98 15 15.02 15.04 15.06 15.08 15.1 15.12 angle energy
- T. Rabedeau, SSRL
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X-ray Optics: Double Crystal Monochromators - Dupond and Acceptance Diagram
12380 12400 12420 12440 12460 12480 12500 14.98 15 15.02 15.04 15.06 15.08 15.1 15.12 angle energy
Darwin
- T. Rabedeau, SSRL
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X-ray Optics: Double Crystal Monochromators - Dupond and Acceptance Diagram
12380 12400 12420 12440 12460 12480 12500 14.98 15 15.02 15.04 15.06 15.08 15.1 15.12 angle energy
Darwin
- T. Rabedeau, SSRL
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X-ray Optics: Double Crystal Monochromators - Dupond and Acceptance Diagram
12380 12400 12420 12440 12460 12480 12500 14.98 15 15.02 15.04 15.06 15.08 15.1 15.12 angle energy
beam convergence/divergence
- T. Rabedeau, SSRL
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X-ray Optics: Double Crystal Monochromators - Dupond and Acceptance Diagram
12380 12400 12420 12440 12460 12480 12500 14.98 15 15.02 15.04 15.06 15.08 15.1 15.12 angle energy
Darwin beam convergence/divergence energy resolution:
- Darwin = 32.4
- total = 64.7
- T. Rabedeau, SSRL
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X-ray Optics: Monochromatizing Divergent Sources
Ø Based on Bragg Diffraction Ø Monochromator & Focusing Curved vs. Plate Crystal Ø Increased beam area that meets Bragg condition. Ø Improve Energy resolution Ø Focusing Effect
Rowland circle
Doubly Curved Crystals
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X-ray Optics: Monochromatizing Divergent Sources
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X-ray Optics: X-rays transmission in waveguides
Analytical description of waveguide Angle of incidence at point Α(x,y,z) Angle of incidence at Geometrical Parameters constrain
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X-ray Optics: X-rays transmission in waveguides
Reflectivity
Photon energy: 8 keV
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X-ray Optics: Polycapillary X-ray lenses
Bundles of thousands glass mono-capillaries in certain arrangements can be used for: Ø Directing Ø Focusing Ø Parallelizing
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X-ray Optics: Polycapillary X-ray lenses
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X-ray Optics: Polycapillary X-ray lenses
Polycapillary lens Functionality: Spot focusing of diverging x-ray beam. Main Applications: Focusing x-ray tubes beams .
d1, d2 0.3…1 mm dmax 1…2 mm l ¡ 40…50 mm f1,f2 ¡ 15…100 mm FWHM 15…100 µm ¡
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X-ray Optics: Polycapillary-based XRF
X-ray tube
detector sample polycapillary
X-ray tube based Micro-XRF setup
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Summary X-ray Sources
X-ray Tubes
Synchrotron Radiation Beamlines
X-ray Optics
Mirrors
Monochromators Double Curved Crystals Polycapillary lenses
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