Injector and Collider Rings of Superkekb B Factory
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Development of an Electron Gun for the Kek Positron Generator
Particle Accelerators, 1990, Vol. 27, pp. 145-149 © 1990 Gordon and Breach, Science Publishers, Inc. Reprints available directly from the publisher Printed in the United States of America Photocopying permitted by license only DEVELOPMENT OF AN ELECTRON GUN FOR THE KEK POSITRON GENERATOR HIDEKI IWATA, YUJIRO OOAWA*, SATOSIll OHSAWA*, HITOSHI KOBAYASHI*, MITUHIRO YOKOTA*, SHIGEKI FUKUDA* and AKIRA ASAMI* Ishikawajima-harima Heavy Industries Co., Ltd. * National Laboratory for High Energy Physics(KEK) 1-1 Oho, Tsukuba-shi, Ibaraki-ken, 305 Japan Abstract In the KEK Positron Generator, a semi-long pulsed beam (-40ns) has turned out to be suitable for effective positron injection into the PF storage ring. However, to use the semi-long pulsed beam, there was a problem concerning the cathode lifetime of the gun. Thus, a new gun has been developed with a dispenser cathode, Y-796(EIMAC); the characteristics of this gun have been investigated. This new gun has been used since October 1988 and has continued to produce constant current of about 12 A without having to exchange its cathode. Thus, the cathode lifetime has been remarkably improved. INTRODUCTION Positrons had so far been utilized only in the e+-e- colliding experiments of TRISTAN, which began in November 1986. Since 1988, however, it had started to use positrons also in the Photon Factory storage ring. It had been confinned that a positron beam with a width of -40 ns was suitable for the PF ring to reduce the injection time. t ,2,3 However, to use this semi-long pulsed beam, there was a problem regarding the cathode lifetime of the old gun, the cathode of which was an oxide-coated type.4 Therefore, a new gun with a dispenser cathode, Y-796(EIMAC), has been developed to achieve a long lifetime of the cathode and to obtain a larger anode current. -
Participants
PARTICIPANTS Abbott, Richard [email protected] California Institute of Technology Aldach, Jackie [email protected] Stanford Linear Accelerator Center Allen, Christopher [email protected] Los Alamos National Laboratory Allison, Stephanie [email protected] Stanford Linear Accelerator Center Allison, Trent [email protected] Thomas Jefferson National Accelerator Facility Anicic, Damir [email protected] Paul Scherrer Institut PSI Armstrong, Dennis [email protected] Isaac Newton Group Bacher, Reinhard [email protected] DESY Backman, Raymond H. [email protected] Mega Industries, L.L.C. Baek, Sulhee [email protected] Samsung Advanced Institute of Technology Baer, Ralph C. [email protected] GSI Darmstadt Bartlett, J. Frederick [email protected] Fermi National Accelerator Laboratory Bec, Matthieu [email protected] Gemini Observatory Bernstein, Dorel [email protected] Stanford Linear Accelerator Center Bevins, Brian [email protected] Thomas Jefferson National Accelerator Facility Bickley, Matthew [email protected] Thomas Jefferson National Accelerator Facility Biocca, Alan [email protected] Lawrence Berkeley National Laboratory Birke, Thomas [email protected] Los Alamos National Laboratory PARTICIPANTS 8th International Conference on Accelerator & Large Experimental Physics Control Systems Bjorklund, Eric [email protected] Spallation Neutron Source Blumer, Thomas [email protected] Paul Scherrer Institut PSI Bolkhovityanov, Dmitry [email protected] Budker Institute of Nuclear Physics Bolshakov, Timofei [email protected] Fermi National Accelerator Laboratory Bookwalter, Valerie [email protected] Thomas Jefferson National Accelerator Facility Boriskin, Victor [email protected] Kharkov Institute Physics & Technology Bork, Rolf [email protected] California Institute of Technology Brazier, John [email protected] Brazier Systems & Consultants Ltd. -
Superkekb VACUUM SYSTEM K
SuperKEKB VACUUM SYSTEM K. Shibata#, KEK, Tsukuba, Japan Abstract size in the horizontal and vertical directions at the IP, I is SuperKEKB, which is an upgrade of the KEKB B- the beam current, y is the vertical beam-beam * factory (KEKB), is a next-generation high-luminosity parameter, y is the vertical beta function at the IP, RL electron-positron collider. Its design luminosity is 8.0× and Ry are the reduction factors for the luminosity and 1035 cm-2s-1, which is about 40 times than the KEKB’s vertical beam-beam tune-shift parameter, respectively, record. To achieve this challenging goal, bunches of both owing to the crossing angle and the hourglass effect. The beams are squeezed extremely to the nanometer scale and subscripts + and – indicate a positron or electron, the beam currents are doubled. To realize this, many respectively. At the SuperKEKB, crossing the beams by upgrades must be performed including the replacement of using the “nanobeam scheme” [3] makes it possible to * th beam pipes mainly in the positron ring (LER). The beam squeeze y to about 1/20 of KEKB’s size. In the pipes in the LER arc section are being replaced with new nanobeam scheme, bunches of both beams are squeezed aluminium-alloy pipes with antechambers to cope with extremely to the nanometer scale (0.3 mm across and 100 the electron cloud issue and heating problem. nm high) and intersect only in the highly focused region Additionally, several types of countermeasures will be of each bunch at a large crossing angle (4.8 degrees). -
The Large Hadron Collider Lyndon Evans CERN – European Organization for Nuclear Research, Geneva, Switzerland
34th SLAC Summer Institute On Particle Physics (SSI 2006), July 17-28, 2006 The Large Hadron Collider Lyndon Evans CERN – European Organization for Nuclear Research, Geneva, Switzerland 1. INTRODUCTION The Large Hadron Collider (LHC) at CERN is now in its final installation and commissioning phase. It is a two-ring superconducting proton-proton collider housed in the 27 km tunnel previously constructed for the Large Electron Positron collider (LEP). It is designed to provide proton-proton collisions with unprecedented luminosity (1034cm-2.s-1) and a centre-of-mass energy of 14 TeV for the study of rare events such as the production of the Higgs particle if it exists. In order to reach the required energy in the existing tunnel, the dipoles must operate at 1.9 K in superfluid helium. In addition to p-p operation, the LHC will be able to collide heavy nuclei (Pb-Pb) with a centre-of-mass energy of 1150 TeV (2.76 TeV/u and 7 TeV per charge). By modifying the existing obsolete antiproton ring (LEAR) into an ion accumulator (LEIR) in which electron cooling is applied, the luminosity can reach 1027cm-2.s-1. The LHC presents many innovative features and a number of challenges which push the art of safely manipulating intense proton beams to extreme limits. The beams are injected into the LHC from the existing Super Proton Synchrotron (SPS) at an energy of 450 GeV. After the two rings are filled, the machine is ramped to its nominal energy of 7 TeV over about 28 minutes. In order to reach this energy, the dipole field must reach the unprecedented level for accelerator magnets of 8.3 T. -
FROM KEK-PS to J-PARC Yoshishige Yamazaki, J-PARC, KEK & JAEA, Japan
FROM KEK-PS TO J-PARC Yoshishige Yamazaki, J-PARC, KEK & JAEA, Japan Abstract target are located in series. Every 3 s or so, depending The user experiments at J-PARC have just started. upon the usage of the main ring (MR), the beam is JPARC, which stands for Japan Proton Accelerator extracted from the RCS to be injected to the MR. Here, it Research Complex, comprises a 400-MeV linac (at is ramped up to 30 GeV at present and slowly extracted to present: 180 MeV, being upgraded), a 3-GeV rapid- Hadron Experimental Hall, where the kaon-production cycling synchrotron (RCS), and a 50-GeV main ring target is located. The experiments using the kaons are (MR) synchrotron, which is now in operation at 30 GeV. conducted there. Sometimes, it is fast extracted to The RCS will provide the muon-production target and the produce the neutrinos, which are sent to the Super spallation-neutron-production target with a beam power Kamiokande detector, which is located 295-km west of of 1 MW (at present: 120 kW) at a repetition rate of 25 the J-PARC site. In the future, we are conceiving the Hz. The muons and neutrons thus generated will be used possibility of constructing a test facility for an in materials science, life science, and others, including accelerator-driven nuclear waste transmutation system, industrial applications. The beams that are fast extracted which was shifted to Phase II. We are trying every effort from the MR generate neutrinos to be sent to the Super to get funding for this facility. -
Design Study of a Superconducting Insertion Quadrupole Magnet for the Large Hadron Collider
EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH European Laboratory for Particle Physics Large Hadron Collider Project LHC Project Report 75 DESIGN STUDY OF A SUPERCONDUCTING INSERTION QUADRUPOLE MAGNET FOR THE LARGE HADRON COLLIDER G. Kirby, R. Ostojic, and T. M. Taylor A. Yamamoto*, K. Tsuchiya*, N. Higashi*, T. Nakamoto*, T. Ogitsu*, N. Ohuchi*, T. Shintomi*, and A. Terashima* Abstract The conceptual design study of a high gradient superconducting insertion quadrupole magnet has been carried out in collaboration between KEK and CERN for the Large Hadron Collider (LHC) to be built at CERN. A model magnet design has been optimized to provide a nominal design field gradient of 240 T/m with a bore aperture of 70 mm and an operational field gradient of 225 T/m at 1.9 K under radiation environment with a beam energy deposit of several watts per meter in the superconducting coils. The design and its optimization process are discussed. LHC Division *National Laboratory for High Energy Physics (KEK), Tsukuba, Ibaraki, 305, Japan ASC Pittsburg ‘96 Administrative Secretariat LHC Division CERN CH - 1211 Geneva 23 Switzerland Geneva, 12 November 1996 Design Study of a Superconducting Insertion Quadrupole Magnet for The Large Hadron Collider A. Yamamoto, K. Tsuchiya, N. Higashi, T. Nakamoto T. Ogitsu, N. Ohuchi, T. Shintomi, and A. Terashima National Laboratory [or High Energy Physics (KEK), Tsukuba, Ibaraki, 305, Japan G. Kirby*, R. Ostojic, and T. M. Taylor European Laboratory for Particle Physics (CERN), 23 Geneva, CH-1211, Switzerland Abstract---The conceptual design study of a 111. MODEL MAGNET DESIGN high gradient superconducting insertion quadrupole magnet has been carried out i n A. -
Commissioning of the KEKB B-Factoryinvited
Proceedings of the 1999 Particle Accelerator Conference, New York, 1999 COMMISSIONING OF THE KEKB B–FACTORY K. Akai, N. Akasaka, A. Enomoto, J. Flanagan, H. Fukuma, Y. Funakoshi, K. Furukawa, J. Haba, S. Hiramatsu, K. Hosoyama, N. Huang∗, T. Ieiri, N. Iida, T. Kamitani, S. Kato, M. Kikuchi, E. Kikutani, H. Koiso, S.–I. Kurokawa, M. Masuzawa, S. Michizono, T. Mimashi, T. Nakamura, Y. Ogawa, K. Ohmi, Y. Ohnishi, S. Ohsawa, N. Ohuchi, K. Oide,D.Pestrikov†,K.Satoh, M. Suetake, Y. Suetsugu, T. Suwada, M. Tawada, M. Tejima, M. Tobiyama, N. Yamamoto, M. Yoshida, S. Yoshimoto, M. Yoshioka, KEK, Oho, Tsukuba, Ibaraki 305-0801, Japan, T. Browder, Univ. of Hawaii, 2505 Correa Road, Honolulu, HI 96822, U.S.A. Abstract The commissioning of the KEKB B–Factory storage rings started on Dec. 1, 1998. The two rings both achieved a stored current of over 0.5 A after operating for four months. The two beams were successfully collided several times. The commissioning stopped on Apr. 19, taking a 5-week break to install the Belle detector. 1 BRIEF HISTORY OF THE COMMISSIONING The KEKB B–Factory[1] consists of two storage rings, the LER (3.5 GeV, e+) and the HER (8 GeV, e−), and the in- jector Linac/beam-transport (BT) system. The Linac was upgraded from the injector for TRISTAN, and was com- missioned starting in June 1997, including part of the BT line. The injector complex was ready before the start of commissioning of the rings.[2] Figure 1 shows the growth of the stored currents in the two rings through the period of commissioning. -
Development of Pulsed Neutron Sources パルス中性子源の開発
23/12/2020 Development of Pulsed Neutron Sources パルス中性子源の開発 Yoshiaki Kiyanagi 鬼柳善明 Nagoya University 名古屋大学工学研究科 1 History of Pulsed Neutron Sources (Change of plans from 1990) ESS SNS J-PARC (2022?) (2006) (2008) (1982) (1985) IPNS(1981) KENS(1980) 136MeV 1971 1959 300MeV 45MeV Hokkaido 1973 45MeV 2 Accelerator-driven Neutron Sources before KENS established in 1980 (Electron Acc.) (Except for nuclear data measurements) Hokkaido University The Gaerttner Linear Accelerator Center at Rensselaer Polytechnic Institute (RPI) Harwell Linac Linac at Laboratory of Nuclear Science at (opposite present ISIS) Tohoku University (LNS) (Present: Research Center for Electron Photon Science) 3 National Laboratory for High Energy Physics: KEK (Now, High Energy Accelerator Research Organization) Booster Synchrotron Utilization Facility KENS:KEK Neutron Source (KEK中性子源) Green area Proton therapy Muon https://www2.kek.jp/openhouse/1996/image/BSF/BSF7.gif 4 Coupling of Target-Moderator- Reflector research Late Prof. Watanabe performed experiments using a RI neutron source. スパレーション・パルス中性子源KENSとそれによる中性子散乱 渡邊昇、佐々木寛、石川義和 日本原子力学会誌 Vol. 23, No. 6 (1981) 389-398 5 Development of a Methane Cold Moderator at Hokkaido University Cylindrical shape Neutron Energy Spectra Spectra Energy Neutron moderator with a re-entrant hole Neutron Energy (eV) K. Inoue, N. Otomo, H. Iwasa and Y. Kiyanagi, J. Nuclear Science and Technology, Vol.11, No.5, pp.228-229, (1974) 6 KENS Neutron source Cold source Co-existence Thermal source The first cold neutron source set at a dedicated neutron scattering experimental facility. (There was an opinion a cold source was not necessary for neutron sources based on accelerators) A wise decision by Professors Watanabe and Ishikawa 渡邊昇, 石川義和: 物理学会誌, 39, 826 (1984). -
Tevatron Accelerator Physics and Operation Highlights A
FERMILAB-CONF-11-129-APC TEVATRON ACCELERATOR PHYSICS AND OPERATION HIGHLIGHTS A. Valishev for the Tevatron group, FNAL, Batavia, IL 60510, U.S.A. Abstract Table 1: Integrated luminosity performance by fiscal year. The performance of the Tevatron collider demonstrated FY07 FY08 FY09 FY10 continuous growth over the course of Run II, with the peak luminosity reaching 4×1032 cm-2 s-1, and the weekly Total integral (fb-1) 1.3 1.8 1.9 2.47 -1 integration rate exceeding 70 pb . This report presents a review of the most important advances that contributed to Until the middle of calendar year 2009, the luminosity this performance improvement, including beam dynamics growth was dominated by improvements of the antiproton modeling, precision optics measurements and stability production rate [2], which remains stable since. control, implementation of collimation during low-beta Performance improvements over the last two years squeeze. Algorithms employed for optimization of the became possible because of implementation of a few luminosity integration are presented and the lessons operational changes, described in the following section. learned from high-luminosity operation are discussed. Studies of novel accelerator physics concepts at the Tevatron are described, such as the collimation techniques using crystal collimator and hollow electron beam, and compensation of beam-beam effects. COLLIDER RUN II PERFORMANCE Tevatron collider Run II with proton-antiproton collisions at the center of mass energy of 1.96 TeV started in March 2001. Since then, 10.5 fb-1 of integrated luminosity has been delivered to CDF and D0 experiments (Fig. 1). All major technical upgrades of the accelerator complex were completed by 2007 [1]. -
Present Status of Kekb Project
PRESENT STATUS OF KEKB PROJECT Shin-ichi Kurokawa KEK, High Energy Accelerator Research Organization 1-1 Oho, Tsukuba-shi, Ibaraki-ken, 305-0801, Japan Abstract GeV electron and a 5.3-GeV positron collide and produce a pair of B meson and anti-B meson at rest at the Υ(4S) The KEK B-Factory, KEKB, is an asymmetric-energy, resonance. In the laboratory frame where an 8-GeV two-ring, electron-positron collider for B physics. Eight- electron and a 3.5-GeV positron collide, the B and anti-B GeV electrons stored in a high-energy ring (HER) and mesons move along the direction of the incoming 3.5- GeV positrons in a low-energy ring (LER) collide at electron, travel over a few hundred µm, and decay at an interaction point (IP), which BELLE detector different positions. By detecting the decay products, we surrounds. In order to facilitate detection of CP-violation can identify the B and anti-B mesons. This identification effect at the bottom-quark sector, the machine is designed is essential for studying CP-violation, which is a subtle to reach a luminosity of 1034cm-2s-1. Even with a high difference in behavior between particles and anti- beam-beam tuneshift of 0.052 and a small βy* of 1 cm at particles. IP, necessary currents in the rings amount to 1.1 A at HER and 2.6 A at LER. KEKB adopts new schemes to reach TSUKUBA IP the goal, such as ±11 mrad finite-angle collision at IP, non-interleaved-sextupole chromaticity correction to have HER LER HER large dynamic apertures, higher-order-mode-free normal LER conducting cavity called ARES and single-cell, single- mode, superconducting cavities to prevent coupled-bunch instabilities and combat heavy beam-loading, among others. -
MIT at the Large Hadron Collider—Illuminating the High-Energy Frontier
Mit at the large hadron collider—Illuminating the high-energy frontier 40 ) roland | klute mit physics annual 2010 gunther roland and Markus Klute ver the last few decades, teams of physicists and engineers O all over the globe have worked on the components for one of the most complex machines ever built: the Large Hadron Collider (LHC) at the CERN laboratory in Geneva, Switzerland. Collaborations of thousands of scientists have assembled the giant particle detectors used to examine collisions of protons and nuclei at energies never before achieved in a labo- ratory. After initial tests proved successful in late 2009, the LHC physics program was launched in March 2010. Now the race is on to fulfill the LHC’s paradoxical mission: to complete the Stan- dard Model of particle physics by detecting its last missing piece, the Higgs boson, and to discover the building blocks of a more complete theory of nature to finally replace the Standard Model. The MIT team working on the Compact Muon Solenoid (CMS) experiment at the LHC stands at the forefront of this new era of particle and nuclear physics. The High Energy Frontier Our current understanding of the fundamental interactions of nature is encap- sulated in the Standard Model of particle physics. In this theory, the multitude of subatomic particles is explained in terms of just two kinds of basic building blocks: quarks, which form protons and neutrons, and leptons, including the electron and its heavier cousins. From the three basic interactions described by the Standard Model—the strong, electroweak and gravitational forces—arise much of our understanding of the world around us, from the formation of matter in the early universe, to the energy production in the Sun, and the stability of atoms and mit physics annual 2010 roland | klute ( 41 figure 1 A photograph of the interior, central molecules. -
First New Particle-‐Smasher Since the LHC Comes
www.coepp.org.au Media release for immediate release Thursday 3 March 2016 First new particle-smasher since the LHC comes online A new particle collider, SuperKEKB, located at the KEK laboratory in Tsukuba, Japan has achieved “First Turns” and is now in the test operation stage. This is the newest “particle-smasher” to go online since the LHC at CERN in Geneva. SuperKEKB will be the world’s highest-luminosity collider and, in association with the Belle II experiment, it will collide electrons with their antiparticles – positrons – in the search for new physics. Designed and built at KEK by a team of Japanese accelerator physicists, SuperKEKB, along with the Belle II detector at the interaction point, will search for new physics beyond the Standard Model by measuring rare decays of elementary particles such as beauty quarks, charm quarks and tau leptons. In contrast to the LHC, which is the world's highest energy machine, SuperKEKB/Belle II is designed to have the world’s highest luminosity or rate of collisions (40 times higher than its predecessor KEKB). This will make SuperKEKB the world’s “highest luminosity” machine and the leading accelerator on the “luminosity frontier”. Key milestones: • 10 February, 2016: SuperKEKB succeeded in circulating and storing a positron beam moving close to the speed of light around the 3.0 kilometre circumference of its main ring. • 26 February, 2016: SuperKEKB electron-positron collider succeeded in circulating and storing a seven billion electron-volt energy (7 GeV) electron beam around its ring of magnets in the opposite direction. The achievement of these “first turns” – i.e.