STUDIES OF ENERGY RECOVERY LINACS AT ... - CASA
STUDIES OF ENERGY RECOVERY LINACS AT ... - CASA
STUDIES OF ENERGY RECOVERY LINACS AT ... - CASA
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decelerated beam energy. A spectrometer in the injector region was used to measure<br />
the injected energy and the magnet which deflects the beam to the dump was used<br />
to measure the decelerated beam energy.<br />
2.3 Transporting Beam to the Energy Recovery<br />
Dump<br />
The CEBAF-ER experiment started in earnest on March 25, 2003 using a<br />
56 MeV injector setup and by the following day energy recovered beam was suc-<br />
cessfully transported to the beam dump. That in itself satisfied the primary goal of<br />
the experiment - to demonstrate the feasibility of energy recovery on a large-scale<br />
machine and at high energy.<br />
The experiment started by balancing the linac energy as described in Sec-<br />
tion 2.2.4. After the linac energies were balanced, the RF ganged phases in the<br />
south linac were returned to their nominal settings to accelerate the first pass beam.<br />
The arc 2 optics, with the spreader and recombiner set to match the beam into the<br />
north linac for deceleration, were then loaded into the machine.<br />
2.3.1 Setting the Path Length<br />
To achieve good performance with energy recovery, the decelerated pass must<br />
be exactly 180 ◦ out of phase with respect to the accelerating pass. Operationally,<br />
the proper path length differential was achieved in the following way [35]: first, note<br />
that the energy of the first pass beam through arc 1 is<br />
E (1)<br />
A1 = Einj + ENL cos θNL<br />
33<br />
(2.2)<br />
where Einj is the injected beam energy, ENL is the energy gain through the north