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In general, light is created by accelerating electrical
charges, or equivalently (but less obviously) by quantum
transitions of charged particles from one energy state to
another.
Examples: radio (electrons oscillate in antenna),
mercury lamp (transitions between atomic states).
When an electron hits an anode:
- It bumps into atoms and slows down, creating
radiation of a continuous distribution of wavelengths
(``bremstrahlung'')
- It causes sharp atomic transitions, resulting
in x-rays with definite wavelengths.
- X-rays emitted isotropically, so
you only utilize a small fraction of the radiation.
- Radiation only intense at well-defined wavelength.
- If you turn up the current, the anode melts.
Fix: water cool the anode.
But...itt still melts when you turn up the power a bit more.
Fix: rotate the anode so that the electron beam
travels over the surface .
You can increase the power by a factor of 20, but you
still run into heating problems. Also,
your x-ray machine is more complicated and breaks
down a lot.
Fix: think of a completely new way of making x-rays.
A way of keeping high energy charged particles going
in a circle.
Particles are accelerated, and therefore they radiate.
Radiation is intense, continuous (tunable),
intrinsically collimated, pulsed and polarized.
Disadvantages: big facility mode, heating of optical
elements, sample damage by x-rays.
Wiggler: line of bending magnets which enhances the
signal but leaves the net direction of the electron beam
unchanged.
Wiggler: strong magnetic field, large excursion, short wavelength.
Undulator: weak magnetic field, small excursion, partial coherence.
- Spectroscopy (EXAFS)--yields local structure
- X-ray lithography--the silicon connection
- Traditional crystallography--very fast
- Time-resolved structural studies (t between
100 ps and one week)
- Crystallography using very small samples--e.g.,
protein crystallo-graphy, 100 micron sample, 10**4 peaks
- High resolution diffraction and diffuse scattering
with small or unstable samples--e.g. metal or semiconductor
surfaces, liquid surfaces, membranes
- Novel applications--magnetic scattering, inelastic
scattering, speckle interferometry, ...?
- Fixed-tube generators (6-8 at around $80K).
Routine characterization. Low maintenance.
- Rotating-anode generators (3-4 at around $200K).
For in-house, high-precision structural studies.
High maintenance.
- Synchrotron XRD at
NSLS (Brookhaven National
Laboratory). Partial ownership of one line +
collaborative research on 2-3 other lines. A
beamline costs around $1000K to construct.
- Synchrotron XRD at the
Advanced Photon Source,
at Argonne National Laboratory.
Part of a consortium building a beam-line.
Estimated cost $3,500K.
Next: Instrumentation for XRD:
Diffractometers and Detectors
Up: High Resolution X-ray Diffraction
Previous: What is X-ray Diffraction
Copyright 1995, 1996, Paul A. Heiney. Individuals should feel free to
make links to this document or any images contained in it,
or to make a copy for their own personal use.
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must appear on any copy.
Last updated December 30, 1996
Paul A. Heiney,
heiney@dept.physics.upenn.edu