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Abstracts Brochure - CERN

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THPLS — Poster Session 29-Jun-06 16:00 - 18:00<br />

Next Generation Light Source Storage Ring at SPring-8<br />

A linac-based XFEL and an ERL are widely<br />

accepted as next-generation light sources. K. Tsumaki, N. Kumagai (JASRI/SPring-8)<br />

But they still have many technologically difficult<br />

problems to overcome. In contrast, electron beams in a storage ring are very stable. Thus, we examined the<br />

possibility of the storage ring as a next-generation light source. We designed a storage ring with an energy of 6 GeV<br />

and a circumference of 1436 m. The ring consists of 24 ten-bend achromat cells and has a natural emittance of 83<br />

pm·rad. The circumference is equal to that of SPring-8 storage ring and the cell length is two times, which enables us<br />

to replace the existing storage ring with this new one in the SPring-8 tunnel and use the photon beam-lines without<br />

constructing new ones. Particle tracking simulation showed that the horizontal dynamic aperture at the center of<br />

a straight section is -3.7 mm and +3.4 mm and that it can be increased to -6.6 mm and +10.0 mm by changing the<br />

sextupole strength for chromaticity correction while keeping zero chromaticity. In this paper, we describe the design<br />

and the dynamic aperture of the extremely low emittance storage ring at SPring-8.<br />

Status of the Photon Factory Storage Ring after the Straight-sections Upgrade<br />

At the 2.5-GeV ring of the Photon Factory<br />

(PF), a large reconstruction of the lattice<br />

around the straight sections* has been<br />

accomplished in 2005. As a result, four<br />

short straight sections of 1.5 m have been<br />

newly created, and the lengths of the existing<br />

straight sections have been much improved.<br />

For example, the length of the<br />

T. Honda, S. Asaoka, W.X. Cheng, K. Haga, K. Harada, Y. Hori,<br />

M. Izawa, T. Kasuga, Y. Kobayashi, H. Maezawa, A. Mishina, T.<br />

Mitsuhashi, T. Miyajima, H. Miyauchi, S. Nagahashi, T. Nogami,<br />

T. Obina, C.O. Pak, S. Sakanaka, Y. Sato, T. Shioya, M. Tadano,<br />

T. Takahashi, Y. Tanimoto, K. Tsuchiya, T. Uchiyama, A. Ueda, K.<br />

Umemori, S. Yamamoto (KEK)<br />

longest straight section has been extended to 9 m from 5 m. The optics has been optimized for installing shortperiod<br />

narrow-gap (in-vacuum) undulators at the new straight sections. The reconstruction work on the ring was<br />

held from March to September 2005. In the range over two-thirds of the storage ring, all the quadrupole magnets and<br />

all the beam ducts have been renewed and rearranged. Commissioning of the storage ring was started from the end<br />

of September 2005 and continued for one month. The operation for the user experiment was resumed from the end<br />

of October on schedule. Though we made no in-situ baking after the installation for the beam ducts, the vacuum<br />

scrubbing by the synchrotron radiation is running very well. The product of the beam lifetime and the beam current<br />

exceeded 700 A min for the operation current 450 mA at the end of December 2005.<br />

*S. Asaoka et al. "New Upgrade Project for the Photon Factory Storage Ring", AIP Conf. Proc. 705, p161 (2004).<br />

Beam Position and Angular Monitor for Undulator by Using SR Monitor Technique<br />

We presented a beam position monitor by<br />

using SR monitor technique in the last PAC05. T. Mitsuhashi, M. Tadano (KEK)<br />

In this monitor, a visible SR in far tail of the<br />

undulator spectrum is extracted by a water-cooled beryllium mirror. We applied a focusing system to observe a beam<br />

position in the undulator through an optical image of beam. We continue further study of this monitor, and this time,<br />

we add the afocal system like a Kepler type telescope to measure the angular deviation of the beam. This system<br />

converts the angular deviation of optical axis of input ray into position deviation, and we can measure an angular<br />

deviation of the beam through its position deviation on the CCD. The results show us this method is applicable to<br />

457<br />

THPLS035<br />

THPLS036<br />

THPLS037

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