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Abstracts Brochure - CERN

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TUPCH138<br />

TUPCH139<br />

TUPCH140<br />

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

Longitudinal Beam Dynamics Optimization in the Booster Synchrotron of ITEP-TWAC Facility<br />

The booster synchrotron of ITEP-TWAC Fa-<br />

P.N. Alekseev, A.D. Milyachenko, V.P. Zavodov (ITEP)<br />

cility (named UK) is used for acceleration of<br />

carbon ions delivered by linear injector I3<br />

with energy of 1.5 MeV/amu, up to the maximum energy of 400 MeV/amu. Speciality of longitudinal beam<br />

dynamics in the UK ring arises from the super high local charge density at low bunching factor of a linac beam at<br />

injection to the synchrotron ring, requiring debunching in the coasting beam, following the RF ramping for the ideal<br />

adiabatic trapping and acceleration of the captured beam up to the maximum energy. Results of the low-level RF<br />

hardware and software optimisation based on the longitudinal beam dynamics simulation and experiments with the<br />

beam are presented.<br />

Coupling Strength Calculation with Galerkin Method for Microtron Resonator<br />

Galerkin method is used to calculate integral<br />

V.G. Kurakin (LPI)<br />

parameters of rf network consisting or regular<br />

waveguide with the a resonator connected<br />

to it. These parameters are standing wave ratio and cavity detuning due to waveguide coupling. In this method,<br />

Maxwell equations are solved in quite usual method by expanding the fields in series of eigenfunctions. The key<br />

feature of the method is the fact that eigenfunctions used are not forced to satisfy to the boundary conditions, and this<br />

simplifies significantly the problem solution. The proofs of the method one can find in special literature, while here<br />

we want emphasize that integral parameters for many cases may be calculated with predicted accuracy. Necessary<br />

expressions for coupling area conductivities are derived followed by computer calculations. Formulae for a cavitywaveguide<br />

coupling strength and for cavity detuning are derived as well. To the end, plots are presented thus<br />

simplifying microtron resonator designing.<br />

Studies of Thermal Fatigue Caused by Pulsed RF Heating<br />

S.V. Kuzikov, N.S. Ginzburg, N.Yu. Peskov, M.I. Petelin, M.E.<br />

Plotkin, A. Sergeev, A.A. Vikharev, N.I. Zaitsev (IAP/RAS) A.V.<br />

Elzhov, A. Kaminsky, O.S. Kozlov, E.A. Perelstein, S. Sedykh, A.P.<br />

Sergeev (JINR) I. Syratchev (<strong>CERN</strong>)<br />

200<br />

A future linear collider with a multi-TeV level<br />

of energies of the collided particles in the<br />

center of masses is naturally associated with<br />

high frequencies and a high power RF level.<br />

One of the interfering factors in this way is an<br />

effect of copper damage due to multi-pulse<br />

mechanical stress caused by high-power microwaves. In order to get new information about this effect, we started an<br />

experiment with the test cavity fed by 30 GHz FEM oscillator (15-30 MW, 100-200 ns, 0.5 - 1 Hz). Now we finished the<br />

second phase of this experiment where the test cavity was irradiated by 0.1 millions of RF pulses with temperature<br />

rise ∼140 C in each pulse. The third phase is the experiment with 1 million pulses. In the next planned experiment<br />

with 36 GHz magnetron (0.1-0.15 MW, 1-2 mks, 0.01 - 1 kHz) we are going to investigate the thermal fatigue in most<br />

interesting for collider application region of temperatures (30-50 C). It is expected that these two experiments will<br />

supply necessary statistical information for the developed theory of the thermal fatigue in order to extrapolate lifetime<br />

numbers to other values of the temperature rise and pulse duration.

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