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Abstracts Brochure - CERN

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MOPCH057<br />

MOPCH058<br />

MOPCH059<br />

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

A Design of 1.8 keV Compton X-ray Generator for the KAERI SC RF LINAC<br />

A.V. Bondarenko, S.V. Miginsky (BINP SB RAS) Y.H. Han, Y.U.<br />

Jeong, B.C. Lee, S. H. Park (KAERI)<br />

62<br />

A quasi-monochromatic X-ray source based<br />

on the KAERI SC linac system has been designed<br />

and is being manufactured now. A 10<br />

MeV 10 mA electron beam together with a 20<br />

W 1.06 ?m laser beam will be used for 1.8 keV Compton X-ray generation with a few percentage of energy spread and<br />

107 photons per second. A simple straight beamline was designed to deliver the electron beam with no degradation<br />

of its emittance and energy spread and to focus it to a proper size to produce the desired X-rays. We expect the first<br />

demonstration of 1.8 keV Compton X-ray generation in autumn 2006.<br />

RF Photogun as Ultra Bright Terahertz Source<br />

W.P.E.M. Op ’t Root, M.J. Loos, O.J. Luiten, M.J. Van der Wiel, T.<br />

van Oudheusden, S.B. van der Geer (TUE)<br />

Recently research into new terahertz (0.3 to<br />

30 THz) light sources has gained a lot of interest.<br />

Especially compact sources capable of<br />

delivering high peak fields (∼ 1 MV/cm), in<br />

a short pulse. To achieve this, we will use short relativistic electron bunches, created by photoemission and accelerated<br />

in an rf-photogun, to create THz light by means of coherent transition radiation. Because wavelengths smaller and<br />

comparable to the bunch length add up coherently, the intensity scales with N 2 , with N the number of electrons in<br />

the bunch. In the first experiments we expect to create THz light pulses with a bandwidth of 1 THz and 1 µJ per<br />

pulse. If such a light pulse is focused on a spot of radius 250 µm, this corresponds to peak electrical fields of 1 MV/<br />

cm. The eventual goal is to increase the bandwidth of the source, by creating shorter electron bunches. This will be<br />

accomplished by choosing a suitable radial laser profile, leading to ellipsoidal electron bunches, which can be focused<br />

and compressed very effectively. Eventually this will lead to THz pulses with a bandwidth of 10 THz and energy of<br />

100 µJ. This corresponds to peak electrical fields of 10 MV/cm and higher.<br />

From Pancake to Waterbag: Creation of High-brightness Electron Bunches<br />

T. van Oudheusden, O.J. Luiten, W.P.E.M. Op ’t Root, M.J. Van der<br />

Wiel, S.B. van der Geer (TUE)<br />

Our recent insight is that, when creating<br />

high-brightness electron bunches, the major<br />

problem is not space charge density itself,<br />

but its distribution. Non-linear space charge<br />

effects lead to a decrease of brightness. We have a novel recipe of creating waterbag bunches (uniformly charged<br />

3D ellipsoids), which have linear space charge fields. Because of these linear fields we have control of the Coulomb<br />

explosion of the bunches. Furthermore, using linear charged particle optics, waterbags can be compressed and focussed<br />

with conservation of brightness. Our recent simulations prove that it is possible to create such ideal waterbag<br />

bunches in practice. The recipe is to create at the cathode a pancake-like electron bunch with a "hemisphere" charge<br />

density distribution. During acceleration this pancake will evolve into a waterbag by its own space charge forces, if<br />

two conditions on the acceleration field and the surface charge density are fulfilled. These two conditions are leading<br />

to a parameter space, which is explored by simulations. We will present numerical simulations and the present status<br />

of the experimental realization.

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