Paper |
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TUCP03 |
Pilot Studies on Optical Transition Radiation Imaging of Non-relativistic Ions at GSI |
130 |
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- B. Walasek-Höhne, C.A. Andre, F. Becker, P. Forck, A. Reiter, M. Schwickert
GSI, Darmstadt, Germany
- A.H. Lumpkin
Fermilab, Batavia, USA
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For relativistic particles optical transition radiation (OTR) is a well established method of transverse profile monitoring. Within a pilot experiment the applicability of OTR even for non-relativistic heavy ions was evaluated for the first time using an uranium beam of 11.4 MeV/u (corresponding to β=0.15) of different charge states. This study aimed to find a thermally stable OTR target for highly-ionizing heavy-ions and to detect reliable transverse profiles, taking advantage of high particle charge q. The exact gating feature of an image-intensified CCD camera was used to select the prompt OTR signal versus any background sources with a longer emission time constant like e.g. blackbody radiation. To test the q-dependence of the light yield, a moveable stripping foil upstream of the target was installed to increase the mean charge. During initial tests, a stainless steel target proved superior thermal behaviour and q2 dependence was observed. Profile comparison with SEM-Grid data as well as the analysis of spectroscopic measurements will be presented.
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Slides TUCP03 [6.112 MB]
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TUPG022 |
Transverse Beam Profile Monitoring using Scintillation Screens for High Energy Ion Beams |
183 |
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- K. Renuka, W. Ensinger
TU Darmstadt, Darmstadt, Germany
- C.A. Andre, F. Becker, P. Forck, R. Haseitl, A. Reiter, B. Walasek-Höhne
GSI, Darmstadt, Germany
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The systematic studies of transverse profile measurement were carried out with scintillation screens such as single crystals (CsI:Tl, YAG:Ce), powder screens (P43, P46), ceramics (Al2O3, Al2O3:Cr, Y and Mg doped ZrO2), Ce doped (0.3%) and undoped glasses (Herasil). Different ion beams like C, Ne, Ta, and U accelerated to energy of 300 MeV/u were extracted from the heavy ion synchrotron at GSI within 0.3 s for intensities from 104 to 109 particles per pulse. The image of each beam pulse was recorded by a CCD camera and individually evaluated. The recorded image profiles show a reproducible dependence on scintillation screen. A difference in image width up to 50% is noticed between CsI:Tl and Herasil. The detailed investigation shows that the powder screens P43 and P46, ceramics Al2O3 and Al2O3:Cr reproduce the beam width within a difference of ± 4% for all intensities. The light yield from the screens scales linearly over 5 orders of magnitude of particle intensity. The light yield per energy deposition by a single ion was calculated for different ion beams. This normalized light yield is a factor of 2 higher for Carbon ions compared to Uranium.
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