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Abstracts Brochure - CERN

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

Very Small Beam Size Measurement by Reflective SR Interferometer at KEK-ATF<br />

An SR interferometer with the Herschelian<br />

reflective optics has been developed for the T. Naito, T. Mitsuhashi (KEK)<br />

measurement of several um beam size. The<br />

chromatic aberration of the optical system applied in the SR interferometer limits the resolution of SR interferometer.<br />

We used objective lens of the SR interferometer by a focusing mirror. For the convenience of observation of the<br />

interferogram, we applied Herschelian arrangement of the optics. The measured vertical beam size was less than<br />

5um and the estimated vertical emittance was 1x10-11m at the KEK-ATF damping ring.<br />

Dual Mode Beam Current Monitor<br />

A new type HEREWARD-transformer is developed.<br />

The original scheme connects<br />

pickup coil to the low impedance input of<br />

the amplifier to increase the time constant of<br />

S. Ninomiya, T. Adachi, S. Fukumoto (KEK) S.H. Hatori, T. Kurita<br />

(WERC)<br />

the transformer. The new scheme employs negative impedance circuit which realizes perfect cancellation of the coil<br />

resistance. Therefore DC component of the beam current can be observed. Since number of winding of the pick up<br />

coil is only 100-turns, therefore by using the original scheme with a fast operational amplifier, the transformer can<br />

be operated at fast CT mode. Thus the dual mode operation can be realized by single core; the first mode is the<br />

slow beam intensity monitor, and the second is a fast response transformer. This operation mode realizes an accurate<br />

observation of the beam injection process. In order to make installation easy, the core is divided into two pieces.<br />

The magnetic shield from bending field is also installed. This monitor is developed at KEK, and installed into the<br />

accelerator at the WAKASA WAN Energy Research Center.<br />

Beam Collimator System in the J-PARC 3-50BT Line<br />

For the J-PARC 50 GeV Main Ring Synchrotron<br />

(MR), the design beam emittance is 54 M.J. Shirakata, H. Oki, T. Oogoe, Y. Takeuchi, M. Yoshioka (KEK)<br />

pi mm mrad. On the other hand, the 3 GeV<br />

beam from the Rapid Cycling Booster Synchrotron (RCS) may have a large halo component upto 216 pi mm mrad.<br />

In order to absorb the halo component, a beam collimator system will be installed in the beam transport line called<br />

as the 3-50BT, which connects the RCS and the MR. From the view of the hands-on maintenance, high endurance<br />

structure is adopted. The beam collimator design including the beam optics is reported in this paper.<br />

Installation of Beam Monitor Sensors in the LINAC Section of J-PARC<br />

In the LINAC section of J-PARC, we have several<br />

type of sensors of monitor, i.e, Beam Position<br />

Monitor, Beam Profile Monitor, Beam<br />

Size Monitor, Current Monitor, Beam Phase<br />

S. Sato, H. Ao, T. Tomisawa, A. Ueno (JAEA/LINAC) H. Akikawa<br />

(JAEA) Z. Igarashi, S. Lee (KEK)<br />

Monitor, Beam Loss Monitor. Those sensors are being installed currently. The procedures, remarks during the installation,<br />

status are described in this paper. As an examle, the beam postion monitors are one of sensors which are taken<br />

177<br />

TUPCH058<br />

TUPCH059<br />

TUPCH060<br />

TUPCH061

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