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CRYRING@ESR - Facility for Antiproton and Ion Research

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26 Chapter 6. Proposed Construction Cycle<br />

• Six quadrupole magnets (types SQ010-SQ030), <strong>and</strong><br />

• Two H/V steering magnets.<br />

All magnets are components of the beam distribution system behind the UNILAC designed <strong>for</strong><br />

a maximum magnetic rigidity of 4.4 Tm. Hence they are well suited <strong>for</strong> the maximum value of<br />

1.44 Tm rigidity of the beam from the ESR. It should be noted that the power consumption will<br />

be below 10% of the nominal values <strong>and</strong> the required amount of cooling water is correspondingly<br />

small.<br />

6.6.2 Power Converters<br />

Power converters will have to be made available <strong>for</strong> all magnets of the two injection beam lines.<br />

Fortunately all required supplies are available at GSI, except a pulsed 2940 A supply <strong>for</strong> the<br />

injection septum magnet which has to be purchased from an industrial company. It is necessary<br />

<strong>for</strong> the injection of ions from the ESR at the maximum magnetic rigidity of 1.4 Tm.<br />

The power supplies <strong>for</strong> all ring <strong>and</strong> electron cooler magnets shall be reinstalled on the concrete<br />

cover of the new cave. The peak power of about 2.6 MVA <strong>for</strong> the operation of CRYRING with a<br />

ramp rate of 7 T/s requires a corresponding intermediate 20/10.5 kV trans<strong>for</strong>mer, if the existing<br />

oil-filled 10.5 kV/880–400 V trans<strong>for</strong>mer <strong>for</strong> silicon controlled rectifiers SCR application is used.<br />

The alternative solution of a new 20 kV/880–400 V dry trans<strong>for</strong>mer <strong>for</strong> SCR will be investigated<br />

later.<br />

6.6.3 Beam Diagnostics<br />

From the discussion with MSL colleagues it is clear that the beam diagnostic equipment will<br />

not be ready <strong>for</strong> use ‘out of the box’, because of several reasons.<br />

• Data acquisition systems were in most cases purpose-built by MSL experts <strong>and</strong> GSI will<br />

not be able to service <strong>and</strong> maintain the devices.<br />

• Often the applied techniques are somewhat outdated (e.g. PC interfacing <strong>for</strong> residual gas<br />

ionization profile monitor) <strong>and</strong> will have to be renewed <strong>for</strong> future usability.<br />

• In general, the degree of control system integration is relatively low: only Faraday-cups<br />

<strong>and</strong> scintillating screens have interfaces to the control system at MSL.<br />

As a consequence, more or less the complete data acquisition part of the diagnostic systems has<br />

to be renewed, whereas the detectors <strong>and</strong> mechanics would remain unchanged wherever possible.<br />

Additionally, it is emphasized that no spare parts exist <strong>for</strong> the diagnostic components, which<br />

introduces some risk <strong>for</strong> future operation of the devices.<br />

It has to be mentioned that the replacement of the existing data acquisition (DAQ) systems<br />

with state-of-the-art techniques will consume the major part of the man power required <strong>for</strong> the<br />

commissioning of CRYRING beam diagnostics at GSI. The renewal of the DAQ is a project<br />

in its own <strong>and</strong> requires manpower <strong>for</strong> technical coordination, <strong>for</strong> adaptations of the existing<br />

hardware (digital <strong>and</strong> analog electronics), as well as <strong>for</strong> programming DAQ software.<br />

6.6.4 Radio-Frequency Components<br />

108.48 MHz RFQ <strong>and</strong> debuncher The 108.48 MHz end stage <strong>for</strong> the RFQ accelerator requires<br />

a new 2–5 kW solid state driver amplifier. The same type can be applied also to operate the<br />

debuncher cavity to reduce the momentum spread of the 300 keV/u RFQ beam from ±1% to<br />

±0.5% in order to increase the efficiency of multiturn injection to CRYRING.<br />

Wideb<strong>and</strong> drift tube The present wideb<strong>and</strong> generator <strong>for</strong> the drift tube accelerating gap of<br />

CRYRING allows a dipole ramp rate of 1 T/s <strong>for</strong> acceleration or deceleration in the frequency

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