• S. Hanada
  Hiroshima University, Graduate School of Science, Higashi-Hiroshima
• A. Miyamoto, S. Sasaki
  HSRC, Higashi-Hiroshima

The HiSOR-II is a storage ring planned as a successive machine of HiSOR, a present ring at Hiroshima Synchrotron Radiation Center. This accelerator has the circumference equal to or less than 50 m, and it has the emittance about 14 nm-rad and aims at the beam energy of 700 MeV. In the HiSOR-II project, we decided to adopt electromagnets with combined function. This type magnet has an advantage for constructing a small storage ring by reducing the total number of magnet, though it has a difficulty for the independent tuning of multipole field components. In addition,　we decided to share a single return yoke between a bending magnet and adjacent quadrupole magnets. In this paper, we discuss about a possible magnetic interference between a bending magnet and a quadrupole magnet. Calculation is made with magnetic field simulation cord RADIA to analyze interference effect and examine the possibility of adoption to HiSOR-II storage ring. Also, we perform the tracking simulation of the beam with the mapping data of a magnetic field provided by this three-dimensional magnetic field analysis. By the simulation, the dynamic aperture is determined.

• A. Miyamoto, K. Goto, S. Sasaki
  HSRC, Higashi-Hiroshima
• S. Hanada
  Hiroshima University, Graduate School of Science, Higashi-Hiroshima
• H. Tsutsui
  SHI, Tokyo

The HiSOR is a synchrotron radiation (SR) source of Hiroshima Synchrotron Radiation Center (HSRC), Hiroshima University, established in 1996. HiSOR is a compact racetrack-type storage ring having 21.95 m circumference, and 400-nmrad natural emittance, which is not so small compared with those of other medium~large storage rings. There are 14 beamlines on HiSOR, but the ring has only two straight sections for undulators which are obviously not compatible with modern SR facilities. Therefore, we are planning to construct a compact storage ring, 'HiSOR-II' in which undulators are dominant light sources. We refer to the electron storage ring MAX-III as the best models to design HiSOR-II lattice. This 700 MeV storage ring is designed that the circumference is equal to or less than 50 m so that it can fit in our existing site. It has several straight sections for undulators, and its natural emittance is about 14nmrad. The booster ring aiming for the top-up injection is constructed on the inside basement of HiSOR-II. This layout brings advantages in radiation shielding and prevention of magnetic field interference between two rings.

• S. Sasaki
  HSRC, Higashi-Hiroshima

More than a decade has past after the original quasi-periodic undulator (QPU) was proposed.* Until now, much work has been done to improve the QPU performance. One of the first most productive improvements was to introduce the quasi-periodicity in an electron trajectory by partially changing the field strength in a periodic undulator.** Also, a modification of creation theory of one-dimensional quasi-periodicity gave another degree of freedom to build this type of device.*** As the result, many different types of QPUs have been and will be installed in the synchrotron radiation facilities worldwide.**** In this paper, a new scheme of quasi-periodic undulator that has a different magnetic structure is proposed. This new QPU generates a slightly higher intensity radiation with higher harmonics pattern different from those of previous QPUs. This new scheme of QPU is achieved by introducing orthogonal field in each half-period in order to create additional phase delay of electron beam at certain positions predicted by the theory. We discuss about realistic magnetic configurations as well as possibilities and limitations of new-QPUs.

* Hashimoto, Sasaki, NIM A361, 611 (1995)
** Chavanne, et al, Proc EPAC98, p2213, Diviacco, et al, ibid, p2216
*** Sasaki, et al, Proc EPAC98, p2237
**** Steier, et al, Proc EPAC08, p2311

• S. Hirata
  Hiroshima University, Faculty of Science, Higashi-Hirosima
• S. Sasaki
  HSRC, Higashi-Hiroshima

Different form conventional periodic undulators, the quasi-periodic undulator (QPU) can radiate　irrational harmonics instead of rational harmonics. It suits with experiments that need highly monochromatic light after passing through the monochromator. For this reason, the QPU is used in many synchrotron radiation facilities all over the world. Recently, new type QPUs that generate radiation spectra different from those by conventional type QPU were proposed*,**. In principle, the shape of radiation spectrum from a new QPU is determined by magnetic field distribution having different quasi periodic pattern. However, calculated spectra using a realistic magnetic field are often different from those of theoretical expectation. In this paper, a detailed comparative study is conducted to examine why there are these differences, how to correct magnetic field to get predicted spectra that fit to the theory. In addition, a possibility of modifying the basis of theory is investigated. These results, new generation method of new quasi-periodicity, and magnetic field distribution to achieve the best performance are presented at the conference.

* S. Sasaki, Proceedings of PAC09, Vancouver, May, 2009.
** S. Sasaki, Proceedings of 6th Annual Meeting of Particle Accelerator Society of Japan (in Japanese).

• S. Sasaki, T. Fujita
  JASRI/SPring-8, Hyogo-ken

The signal processing electronics of the SPring-8 Storage Ring BPM were replaced during the summer shutdown of 2006, and put into operation. However, a large filling pattern dependence was observed. The cause was attributed to the nonlinear response of the diodes to large pulse signals. The diode were attached in front of the RF switches for protection from the electrostatic discharge damages on the switch IC. We took a countermeasure for the filling pattern dependence by reducing the pulse height with a band pass filter (BPF) in front of each channel. The BPF were attached and put into the operation from November 2008. The effect of the BPF was evaluated using the beam with changing the filling patterns and repeating the position measurements. The differences of the measured position data across the filling pattern change were found to be within 10μmeters, which was the same amount of the orbit drift during the filling pattern change.

• N. Yamamoto, M. Hosaka, H. Morimoto, K. Takami, Y. Takashima
  Nagoya University, Nagoya
• Y. Hori
  KEK, Ibaraki
• M. Katoh
  UVSOR, Okazaki
• S. Koda
  SAGA, Tosu
• S. Sasaki
  JASRI/SPring-8, Hyogo-ken

Central Japan Synchrotron Radiation (SR) Research Facility is under construction in the Aichi area, and the service will start from FY2012. Aichi Science & Technology Foundation is responsible for the operation and management, and Nagoya University SR Research Center is responsible to run the facility and support the users technically and scientifically. The accelerators consists of an injector linac, a booster synchrotron and an 1.2 GeV electron storage ring with the circumference of 72 m. To save construction expenses, the 50 MeV linac and the booster with the circumference of 48 m are built at inside of the storage ring. The beam current and natural emittance of the storage ring are 300 mA and 53 nmrad. The magnetic lattice consists of four triple bend cells and four straight sections 4 m long. The bending magnets at the centers of the cells are 5 T superbends and the critical energy of the SR is 4.8 keV. More than ten hard X-ray beam-line can be constructed. One variable polarization undulator will be installed in the first phase. The electron beam will be injected from the booster with the full energy and the top-up operation will be introduced as early as possible.