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Abstracts Brochure - CERN

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MOPCH — Poster Session 26-Jun-06 16:00 - 18:00<br />

Initial Experience Tuning the SNS Superconducting Linac<br />

The Spallation Neutron Source (SNS) accelerator<br />

includes a pulsed superconducting linac<br />

that accelerates H − from 186 MeV to 1000<br />

MeV. The initial experience in setting the 81<br />

J. Galambos, A.V. Aleksandrov, C. Deibele, S. Henderson, D.-O.<br />

Jeon, T.A. Pelaia, Y. Zhang (ORNL)<br />

independently powered cavities comprising the SCL is discussed. A model based time-of-flight method is used to<br />

determine the cavity phase setpoints, the actual cavity voltages and beam output energy for each cavity. As the<br />

cavities are turned on and set to the proper phase, different quadrupole settings are periodically loaded to facilitate<br />

transport of the increasing energy beam. The SCL is quite flexible to running with various numbers of missing cavities<br />

and operating cavities at different amplituides. Lattice configurations have been generated with final beam energies<br />

ranging from 550 to 950 MeV.<br />

Status of the SNS Beam Power Upgrade Project<br />

The baseline Spallation Neutron Source<br />

(SNS) accelerator complex, consisting of an<br />

H − injector, a 1 GeV linear accelerator, an<br />

accumulator ring and associated transport<br />

lines, will provide a 1 GeV, 1.44 MW proton<br />

beam to a liquid mercury target for neutron<br />

production. Upgrades to the SNS accelerator<br />

and target systems to increase the beam<br />

S. Henderson, A.V. Aleksandrov, D.E. Anderson, S. Assadi, I.E.<br />

Campisi, F. Casagrande, M.S. Champion, R.I. Cutler, V.V. Danilov,<br />

G.W. Dodson, D.A. Everitt, J. Galambos, J.R. Haines, J.A. Holmes,<br />

N. Holtkamp, T. Hunter, D.-O. Jeon, S.-H. Kim, D.C. Lousteau, T.L.<br />

Mann, M.P. McCarthy, T. McManamy, G.R. Murdoch, M.A. Plum,<br />

B.R. Riemer, M.P. Stockli, D. Stout, R.F. Welton (ORNL)<br />

power to at least 2 MW, with a design goal of 3 MW, are in the planning stages. The increased SNS beam power<br />

can be achieved primarily by increasing the peak H − ion source current from 38 mA to 59 mA, installing additional<br />

superconducting cryomodules to increase the final linac beam energy to 1.3 GeV, and modifying injection and extraction<br />

hardware in the ring to handle the increased beam energy. The mercury target power handling capability<br />

will be increased to 2 MW or greater by i) mitigating cavitation damage to the target container through improved<br />

materials/surface treatments, and introducing a fine dispersion of gas bubbles in the mercury, and ii) upgrading the<br />

proton beam window, inner reflector plug and moderators. The upgrade beam parameters will be presented and the<br />

required hardware modifications will be described.<br />

Simulations for SNS Ring Commissioning<br />

In preparation for SNS ring commissioning, a<br />

number of operational issues have been stud- J.A. Holmes, S.M. Cousineau, S. Henderson, M.A. Plum (ORNL)<br />

ied using ORBIT Code simulations. These<br />

include beam injection without the use of time-dependent painting, beam accumulation and transport to the extraction<br />

dump and to the target, optimal painting schemes for various beam intensities, detailed tracking through<br />

the extraction septum with fully correct geometry, quadrupole current constraints in the ring-to-target transfer line<br />

(RTBT), and detailed modeling of H minus carbon foil stripping at injection. All these studies incorporated detailed<br />

physics including beam-foil interactions, symplectic single particle tracking, space charge and impedances, and losses<br />

due to apertures and collimation.<br />

85<br />

MOPCH128<br />

MOPCH129<br />

MOPCH130

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