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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

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