Borrmann Effect
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The Borrmann effect (or Borrmann–Campbell effect after Gerhard Borrmann and Herbert N. Campbell) is the anomalous increase in the intensity of X-rays transmitted through a crystal when it is being set up for Bragg reflection. The Borrmann effect—a dramatic increase in transparency to X-ray beams—is observed when X-rays satisfying
Bragg's law In many areas of science, Bragg's law — also known as Wulff–Bragg's condition or Laue–Bragg interference — is a special case of Laue diffraction that gives the angles for coherent scattering of waves from a large crystal lattice. It descr ...
diffract through a perfect crystal. The minimization of absorption seen in the Borrmann effect has been explained by noting that the electric field of the X-ray beam approaches zero amplitude at the crystal planes, thus avoiding the atoms.


References

* * * Borrmann, Gerhard; ''Über Extinktionsdiagramme von Quarz'', Physikalische Zeitschrift 42, 157–162 (1941)
''Die Absorption von Röntgenstrahlen im Fall der Interferenz'', Zeitschrift für Physik 127, 297–323 (1950)
- original articles on Borrmann effect * Campbell, Herbert N.
''X-Ray Absorption in a Crystal Set at the Bragg Angle''
Journal of Applied Physics 22, 1139 (1951) * von Laue, Max
''Die Absorption der Röntgenstrahlen in Kristallen im Interferenzfall'', Acta Crystallographica 2, 106–113 (1949)
- original explanation of Borrmann effect X-ray crystallography {{Crystallography-stub