Apparatus for the production of short-wave electromagnetic radiation
AssigneeMax-Planck-Gesellschaft zur Forderung der Wissenschaften e.V. Berlin
InventorGerd Buschhorn
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AssigneeMax-Planck-Gesellschaft zur Forderung der Wissenschaften e.V. Berlin
InventorGerd Buschhorn
Estimating the term…
Apparatus for the production of short-wave electromagnetic radiaion, especially in the x-ray and gamma-ray region, by means of the interaction between accelerated charged particles, especially electrons or positrons, and a crystal lattice, with a charged-particle source for the production of a beam of energetic charged particles and with a crystal arrangement which is so arranged in the path of the charged particle radiation beam that the charged particles traverse the crystal lattice of the crystal arrangement parallel to a predetermined lattice direction ("channeling-condition"). In order to produce an electromagnetic radiation beam with predetermined convergence or divergence, there are used a correspondingly convergent or divergent charged particle radiation beam (212) as well as a crystal arrangement (214) which is so bent that the channeling condition is at least approximately fulfilled for all charged particle paths in the crystal. (FIG. 1)
Apparatus for the production of short-wave electromagnetic radiaion, especially in the x-ray and gamma-ray region, by means of the interaction between accelerated charged particles, especially electrons or positrons, and a crystal lattice, with a charged-particle source for the production of a beam (212, 312, 412, 512) of energetic charged particles and with a crystal arrangement (214, 314, 414, 514) which is so arranged in the path of the charged particle radiation beam that the charged particles traverse the crystal lattice of the crystal arrangement parallel to a predetermined lattice direction (lattice plane, lattice axis) ("channeling-condition"), comprising in combination a crystal arrangment (214, 314, 414, 514) and means for directing charged particles through said crystal arrangement in at least one plane passing through the axis of the charged particle radiation beam (212, 312, 412, 512) in directions which essentially converge into a predetermined point (220, 320, 520), said crystal arrangement having a side facing away from said charged particle source and a side facing toward said charged particle source, said crystal arrangement being so arranged in an arc about the predetermined point, that the channeling condition is substantially fulfilled for all charged particle beam paths.
Dependencies are inferred from the claim text.