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Michael Jentschel Institut Laue-Langevin ELI-NP, March 2011, Bucharest.

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Presentation on theme: "Michael Jentschel Institut Laue-Langevin ELI-NP, March 2011, Bucharest."— Presentation transcript:

1 Michael Jentschel Institut Laue-Langevin ELI-NP, March 2011, Bucharest

2 Good Resolution: Perfect crystals Angle measurement Perfect crystals Gradient crystals Good for high resolution Good as high efficiency band pass filter

3 Dynamical Diffraction theory: Each el. cell is scattering center Scattering from indiv. Atoms is summarized via structure factor interference of forward/backward reflected partial waves from periodically arranged scattering centers Line profile Diffraction Angle Resolution is independent of Gamma Ray Energy Zachariasen, 1967

4  B 10 -2 rad   10 -8 rad Diffraction process allows to have ppm resolution!

5 Double crystal Geometry ILL geometry: 4  source ELI case: 10 -6 ~10 -7 I 0 10 16 10 -5 10 -2 10 3

6 22% 3 rd order How does a crystal reflect, if the beam divergence fits its acceptance width ?

7 Adapting divergence via refractive optics M. Wegener Karlsruhe Institute of Technology A. Sinigrev, ESRF, Grenoble www.X-ray-optics.com To be tested for gamma rays in 2011

8 Source Spectrometer Table with angle interferometers Detector 1.Crystal 2.Crystal Beam Collimation Movable Collimation These beams need to be separated Large distances needed 21 m0.7 m3 m 0.002 m

9 All fixations free of epoxy: optical bonding silica bonding mechanical clemping All fixations free of epoxy: optical bonding silica bonding mechanical clemping

10 GAMS 5 GAMS 6 (comissioning) 200 prad resolution 20 prad resolution

11 (n,) of 188 Re Complete spectra =220 +180 -30 Dynamic range of 10 6 Broadening due to: Atomic motion Lifetime Zero Point Fluctuation … 1.1MeV

12 Nuclear Structure Physics: Complete Spectroscopy Level Density/Chaos ,n), (,f), (,) reactions Fundamental Physics Fine structure constant Diffraction process Solid state Physics Atomic interaction Phase transitions Many others


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