Compact imaging Bragg spectrometer for fusion devices

Bertschinger, G.; Biel, W.; Jaegers, H.; Marchuk, O.

doi:10.1063/1.1781755

Journal Article

PreJuSER-41431

Compact imaging Bragg spectrometer for fusion devices

Bertschinger, G.FZJ* ; Biel, W.FZJ* ; Jaegers, H.FZJ* ; Marchuk, O.FZJ*

2004
American Institute of Physics [S.l.]

Review of scientific instruments 75, 3727 - 3729 (2004) [10.1063/1.1781755]

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Please use a persistent id in citations: http://hdl.handle.net/2128/1848 doi:10.1063/1.1781755

Abstract: A compact imaging x-ray spectrometer has been designed for tokamaks and stellarators to measure the plasma parameters at different spatial chords. It has been optimized for high spectral resolution and high sensitivity. High spectral resolution is obtained by using solid state detectors and minimizing the imaging errors of the spherical crystals. It is shown, that using spherical crystals the solid angle and hence the throughput can be increased significantly, without compromising the spectral resolution. The design is useful for the measurement of the spectra of He- and H-like ions from Si to Kr. The spectral resolution is sufficient for the measurement of plasma parameters. The temporal resolution is high enough for transport studies by gas puff and laser ablation experiments. The design is based on a modified Johann spectrometer mount, utilizing a spherically bent crystal instead of the cylindrically bent crystal in the traditional Johann mount. The astigmatism of the wavelength selective reflection on the spherical crystal is applied to obtain imaging of an extended plasma source on a two-dimensional detector. For each element, a separate crystal is required, only in few cases, a crystal can be used for the spectra of two elements. For the spectra of most of the He-like ions from Si up to Kr, suitable crystal cuts have been found on quartz, silicon and germanium crystals with Bragg angles in a small interval around the design value of 53.5degrees. All of the crystals have the same radius. They are fixed on a rotational table. The distance to the detector is adjusted by an x-y table to fit to the Rowland circle. (C) 2004 American Institute of Physics.

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