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TUPLS050<br />

TUPLS051<br />

TUPLS052<br />

TUPLS053<br />

27-Jun-06 16:00 - 18:00 TUPLS — Poster Session<br />

The Development of SFRFQ Structure in Peking University<br />

X.Q. Yan, J.-E. Chen, J.X. Fang, Z.Y. Guo, Y.R. Lu, Z. Wang (PKU/<br />

IHIP)<br />

234<br />

The accelerating field in the conventional<br />

RFQ is originated by the surface modulation<br />

of the quadruple electrodes. However, the<br />

axial accelerating field generated in this way<br />

is quite limited. To enhance the energy gain, an alternative structure called Separated Function RFQ (SFRFQ) was<br />

proposed. The principles of the structure had been proved by simulations and model measurements. To further<br />

explore the feasibility of SFRFQ, a 10 cell SFRFQ cavity was built and power test was carried out. All the preliminary<br />

results of the power test are presented and discussed in the paper.<br />

Development of PEFP 20 MeV Proton Accelerator<br />

Y.-S. Cho, H.M. Choi, S.-H. Han, I.-S. Hong, J.-H. Jang, H. S. Kim,<br />

K.Y. Kim, Y.-H. Kim, H.-J. Kwon, K.T. Seol, Y.-G. Song (KAERI)<br />

A 20 MeV proton accelerator has been developed<br />

as a low energy part of PEFP (Proton<br />

Engineering Frontier Project) 100 MeV accelerator.<br />

The 20 MeV accelerator consists of ion<br />

source, LEBT (Low Energy Beam Transport), 3 MeV RFQ (Radiofrequency Quadrupole) and 20 MeV DTL (Drift Tube<br />

Linac). After the field tuning and high power RF conditioning of the accelerating cavities, the first beam test of the 20<br />

MeV accelerator is underway. During the test, the pulsed proton beam was extracted from the ion source by pulsing<br />

the high voltage power supply. Two 1.1 MW, 350MHz RF systems were used to drive the 20 MeV accelerator. The<br />

current transformers between DTL tanks and Faraday cup at the end of 20 MeV DTL were used to measure the beam<br />

current. In this paper, the development of 20MeV accelerator are summarized and the first beam test results are<br />

discussed.<br />

Beam Dynamics of the PEFP Linac<br />

The PEFP Linac consists of a 50 keV ion<br />

J.-H. Jang, Y.-S. Cho, K.Y. Kim, Y.-H. Kim, H.-J. Kwon (KAERI) source, LEBT, 3 MeV RFQ, 20 MeV DTL<br />

called DTL1, MEBT, and 100 MeV DTL called<br />

DTL2. The MEBT includes two small DTL tanks, which match the 20 MeV proton beams into the DTL2, and a bending<br />

magnet, which extracts the 20 MeV proton beams to the experimental hall. We will present the full beam dynamics<br />

study from the entrance of the DTL1 to the end of DTL2 with the initial beam parameters obtained from a simulation<br />

study of the RFQ. Our study focuses on the longitudinal beam matching in order to compensate the missing RF effect<br />

between every neighboring DTL tanks as well as the full beam matching between DTL1 and DTL2.<br />

Beam Dynamics of a High Current IH-DTL Structure for the TWAC Injector<br />

S. Minaev, T. Kulevoy, B.Y. Sharkov (ITEP) U. Ratzinger, R. Tiede<br />

(IAP)<br />

A powerful ion injector based on a laser ion<br />

source is needed for an efficient operation of<br />

the Tera Watt Accumulator (TWAC) complex<br />

including a heavy ion synchrotron and a stor-<br />

age ring, which is under progress now at ITEP, Moscow. The Interdigital H-type drift tube linac (IH-DTL) structure<br />

operating at 162 MHz is proposed for the second stage of the injector linac behind of a 81 MHz RFQ. Consisting

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