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The Supersonic Gasjet Target and its Experimental Enviroment at the ESR Storage Ring
The Supersonic Gasjet Target |
Target species and densities The supersonic jet provides target atoms with a very narrow momentum spread. For a detailed description of the jet-target see: The Hydrogen Cluster Target at the ESR |
Experimental Enviroment at the ESR Jet-Target
For
experiments at the supersonic jet-target two experimental reaction
chambers are available, one dedicated to spectroscopy and collision
studies by means of x-ray detection the other devoted to recoil ion
spectroscopy. The two set-ups can be interchanged at typical time
intervalls of approximately one year. The 0-deg electron spectrometer,
now available at the ESR, serves as a permanent experimental
installation.
a) X-Ray Detector Chamber Combined with 0-deg Electron Spectrometer
Angular Distribution Studies of the Time-Reversed Photoionization Process for decelerated high-Z ions
 Supersonic
jet-target with the x-ray detection chamber. Downstream from the target
zone, the 0-deg electron spectrometer is mounted. |
 Schematic view of the x-ray detection chamber. |
b) Recoil Ion Chamber with Reaction Microscope and 0-deg Electron Spectrometer
The
reaction microscope at the ESR gas jet consists of a set of guiding
fields, a longi-tudinal magnetic B-field (along the projectile axis)
combined with a flexible configuration of electrostatic-extraction
E-fields extending over the entire target zone also including recoil-
and low-momentum electron detectors. Recoiling target ions and low
momentum electrons (pe < 10 a.u.) emanating from the
target zone can be extracted onto multihit capable 2D position
sensitive detectors at opposite ends of the target region. Electrons
emitted from collision partners in the target region with 0° ±2° with
respect to the beam direction and velocities around the projectile
velocity will be momentum analyzed and guided onto a 2D position
sensitve detector while permitting to reconstruct their primordial
emission charcteristics.
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