X-ray Sources



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Origin of X-rays

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:

  1. It bumps into atoms and slows down, creating radiation of a continuous distribution of wavelengths (``bremstrahlung'')
  2. It causes sharp atomic transitions, resulting in x-rays with definite wavelengths.

Generic X-ray Tube

Problems with Traditional X-ray Generators

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.

Synchrotron

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.

``Insertion Devices:'' Wigglers and Undulators

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.

What can you do with an x-ray synchrotron?

X-ray Facilities at the University of Pennsylvania Materials Research Laboratory



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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. However, you may not further disseminate copies in electronic, printed, or any other form without the express permission of the author, and this copyright notice must appear on any copy.

Last updated December 30, 1996

Paul A. Heiney, heiney@dept.physics.upenn.edu