|
Charge breeding system |
Charge breeding system | REXTRAP
| REXEBIS | Mass separator
|
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|
|
Figure
1. |
A
schematic layout of the charge |
In the EBIS the 1+ to n+ ion conversion takes
place by electron bombardment by a high-energetic electron beam. However, the ISOLDE
beam can not be injected into the EBIS with high efficiency without beam
preparation. By introducing a Penning trap in front of the EBIS, which
accumulates, bunches and phase space cools the semi-continuous beam, a
considerably higher injection and trapping efficiency into the EBIS is obtained
compared with continuous injection, and ISOL emittances up to >30 p•mm•mrad (at
60 kV) can be accepted.
|
|
|
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Figure 2. |
Photo
showing the complete charge breeding |
Moreover, the mass selectivity of the side-band
cooling technique in the Penning trap could in principle be employed for a
further purification of the incoming beam. At extraction of the n+ ions from the EBIS the
radioactive ions are separated from stable ion peaks originating from the
residual gas ionisation in an achromatic mass separator. The total cycle time
for ions inside the mass separator ranges from 5 ms for light elements to a few
100 ms for heavier elements (A~150).
The efficiency for trapping, beam transport, charge
breeding and mass selection is normally between 5 and15%. Sub-pA beams can be
handled and the upper throughput limit is a few 109 ions per second.
|
Cooling time < 20 ms Breeding time = 3-200 ms Trap efficiency > 40% EBIS efficiency Beam intensity < 109 ions/s |
1. O. Kester and Dieter Habs, 8th Int. Symposium
EBIS/T 2000, Upton NY, 5-8 Nov.,
AIP conf. proc v572 (2001) 217-223.
2. F. Ames et al. , Int. Workshop on JHF Science: JHF-98-2
v2 400-403.
3. F. Wenander, Nucl Phys. A701 (2002) 528-536c.
4. F. Wenander, P. Delahaye, R. Scrivens, R. Savreux, ‘The REX-ISOLDE charge breeder as an
operational machine’
Rev. Sci. Instrum., vol.77 (2006)
03B104-1-5.
5. F. Wenander, ‘Charge
breeding of radioactive ions with EBIS and EBIT’, Journal of
Instrumentation, vol5 (2010) C10004