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Lattice design for high intensity proton storage ring

Abstract

Japan Atomic Energy Research Institute, JAERI, has been proposing the Neutron Science Project (NSP) which is composed of research facilities based on a proton linac and a proton storage ring with an energy of 1.5 GeV. In the proton storage ring, the pulsed beam from the linac is accumulated, and high intensity pulsed beam is produced for the neutron scattering experiment. The goal of the proton storage ring is to provide a short pulsed proton beam of less than 1 {mu}s with an average beam power of 5 MW with two rings. The study of the proton storage ring whose beam power is 2.5 MW has been performed. To achieve a beam power of 2.5 MW with an energy of 1.5 GeV, it is necessary to accumulate 2.08x10{sup 14} protons. When the beam injection is completed, accumulated protons are extracted from the ring during 1 turn. Lattice design for high intensity proton storage ring has been performed. Two kinds of a lattice are examined as a lattice of the proton storage ring for neutron science project. One is FODO lattice and the other is Triple Bend Achromatic (TBA) lattice. Each lattice has zero dispersion regions and long straight sections. The  More>>
Authors:
Kinsho, Michikazu; Noda, Fumiaki; [1]  Ishi, Yoshihiro; Nakayama, Koichi
  1. Japan Atomic Energy Research Inst., Tokai, Ibaraki (Japan). Tokai Research Establishment
Publication Date:
May 01, 1999
Product Type:
Technical Report
Report Number:
JAERI-Research-99-037
Reference Number:
SCA: 430400; PA: JPN-99:050394; EDB-99:081124; SN: 99002124424
Resource Relation:
Other Information: PBD: May 1999
Subject:
43 PARTICLE ACCELERATORS; NEUTRON SOURCES; PLANNING; DESIGN; PROTON BEAMS; SPALLATION; STORAGE RINGS; BEAM OPTICS; MAGNETIC FIELD CONFIGURATIONS; BEAM BENDING MAGNETS; BEAM FOCUSING MAGNETS; 430400
OSTI ID:
10147655
Research Organizations:
Japan Atomic Energy Research Inst., Tokyo (Japan)
Country of Origin:
Japan
Language:
Japanese
Other Identifying Numbers:
Other: ON: DE99760447; TRN: JP9950394
Availability:
OSTI; NTIS (US Sales Only)
Submitting Site:
JPN
Size:
83 p.
Announcement Date:
Sep 10, 1999

Citation Formats

Kinsho, Michikazu, Noda, Fumiaki, Ishi, Yoshihiro, and Nakayama, Koichi. Lattice design for high intensity proton storage ring. Japan: N. p., 1999. Web.
Kinsho, Michikazu, Noda, Fumiaki, Ishi, Yoshihiro, & Nakayama, Koichi. Lattice design for high intensity proton storage ring. Japan.
Kinsho, Michikazu, Noda, Fumiaki, Ishi, Yoshihiro, and Nakayama, Koichi. 1999. "Lattice design for high intensity proton storage ring." Japan.
@misc{etde_10147655,
title = {Lattice design for high intensity proton storage ring}
author = {Kinsho, Michikazu, Noda, Fumiaki, Ishi, Yoshihiro, and Nakayama, Koichi}
abstractNote = {Japan Atomic Energy Research Institute, JAERI, has been proposing the Neutron Science Project (NSP) which is composed of research facilities based on a proton linac and a proton storage ring with an energy of 1.5 GeV. In the proton storage ring, the pulsed beam from the linac is accumulated, and high intensity pulsed beam is produced for the neutron scattering experiment. The goal of the proton storage ring is to provide a short pulsed proton beam of less than 1 {mu}s with an average beam power of 5 MW with two rings. The study of the proton storage ring whose beam power is 2.5 MW has been performed. To achieve a beam power of 2.5 MW with an energy of 1.5 GeV, it is necessary to accumulate 2.08x10{sup 14} protons. When the beam injection is completed, accumulated protons are extracted from the ring during 1 turn. Lattice design for high intensity proton storage ring has been performed. Two kinds of a lattice are examined as a lattice of the proton storage ring for neutron science project. One is FODO lattice and the other is Triple Bend Achromatic (TBA) lattice. Each lattice has zero dispersion regions and long straight sections. The betatron variation around the ring of the FODO lattice is smooth. Such a property will minimize the possible envelope oscillation for beams with large space charge tune shift. There are long straight sections in the TBA lattice. Such a property will give enough space for injection, rf cavity, and extraction. The consideration of beam dynamics, instabilities, injection scheme, and extraction scheme for each lattice is important to decide which is better lattice for the proton storage ring. This is the main subject for our study of the ring. This paper describes preliminary results of the lattice design for the proton storage ring. (author)}
place = {Japan}
year = {1999}
month = {May}
}