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Abstracts Brochure - CERN

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TUPLS056<br />

TUPLS057<br />

TUPLS058<br />

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

A Prototype of 3-11 MEV RFQ-DTL Accelerating Structure for <strong>CERN</strong> SPL Project<br />

S.V. Ivanov, O.K. Belyaev, Yu.A. Budanov, V.G. Kudryavtsev, O.P.<br />

Lebedev, A.P. Maltsev, E.V. Mazurov, S.R. Salakhutdinov, V.B.<br />

Stepanov, V.A. Teplyakov, A.A. Timopheev, E.F. Troyanov, N.E.<br />

Tyurin, I.A. Zvonarev (IHEP Protvino) V.F. Basmanov, D.V. Boudnikov,<br />

I.D. Goncharov, N.I. Moskvin, S.T. Nazarenko, V.T. Punin,<br />

S.A. Putevskoy, M.L. Smetanin, A.V. Telnov, V.N. Yanovsky, N.V.<br />

Zavyalov, S.A. Zhelezov (VNIIEF)<br />

236<br />

A prototype of 3-11 MeV H ion linac with<br />

spatially periodic RFQ focusing to be run<br />

under a 14% heavy duty factor is presented.<br />

Outcomes of beam dynamic studies for particles<br />

traversing accelerating & focusing channel<br />

with accelerating gap voltage ramped<br />

downstream of beam are specified. Geometry<br />

of a two-vane cavity, of accelerating and<br />

focusing electrodes, and of an RF power in-<br />

put coupler is adopted in compliance with 3D electrodynamical calculations. Results of experimental studies for<br />

electrodynamical parameters of a full-scale cold model of the prototype are given. Thermal stress and deformation<br />

analysis data is presented. Ultimate design developed of the H ion linac structure prototype to be manufactured is<br />

outlined.<br />

Linac4, a New Injector for the <strong>CERN</strong> PS Booster<br />

R. Garoby, F. Gerigk, K. Hanke, A.M. Lombardi, M. Pasini, C. Rossi,<br />

E.Zh. Sargsyan, M. Vretenar (<strong>CERN</strong>)<br />

The first bottle-neck towards higher beam<br />

brightness in the LHC injector chain is due<br />

to space charge induced tune spread at injection<br />

in the <strong>CERN</strong> PS Booster (PSB). A new<br />

injector called Linac4 is proposed to remove this limitation. Using RF cavities at 352 and 704 MHz, it will replace the<br />

present 50 MeV proton Linac2, and deliver a 160 MeV, 40 mA H − beam. The higher injection energy will reduce space<br />

charge effects by a factor of 2, and charge exchange will drastically reduce the beam losses at injection. Operation will<br />

be simplified and the beam brightness required for the LHC ultimate luminosity should be obtained at PS ejection.<br />

Moreover, for the needs of non-LHC physics experiments like ISOLDE, the number of protons per pulse from the PSB<br />

will increase by a significant factor. This new linac constitutes an essential component of any of the envisaged LHC<br />

upgrade scenarios, which can also become the low energy part of a future 3.5 GeV, multi-megawatt superconducting<br />

linac (SPL). The present design has benefited from the support of the French CEA and IN2P3, of the European Union<br />

and of the ISTC (Moscow). The proposed machine and its layout on the <strong>CERN</strong> site are described.<br />

New Prestripping Section of the MILAC Linear Accelerator Designed for Accelerating a<br />

High Current Beam of Light Ions<br />

A.P. Kobets, V.A. Bomko, O.F. Dyachenko, Ye.V. Ivakhno, M.S.<br />

Lesnykh, Z.O. Ptukhina, V.N. Reshetnikov, S.S. Tishkin, V.P. Yashin,<br />

A.V. Zabotin, B.V. Zajtsev, Yu.G. Zalesskij (NSC/KIPT)<br />

In the Kharkov Institute of Physics and Technology,<br />

the works on construction of a new<br />

prestripping section of the multicharge ion<br />

linear accelerator (MILAC) is performed.<br />

The task is set to provide acceleration of high<br />

current beams of light ions for research works on radiation material engineering and applied investigations. The<br />

new prestripping section is designed for accelerating ions with A/q=4 up to the energy of 1 MeV/u; after stripping<br />

they will be accelerated in the main section up to the energy of 8.5 MeV/u. Special operational mode will allow to<br />

increase noticeably the repetition rate with the same power consumption. The calculation results on beam dynamics<br />

in the structure with alternating phase focusing in the version with the stepped change of the synchronous phase, and

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