Developments of the RCNP cyclotron cascade

Similar documents
RCNP cyclotron facility

Design of a Sector Magnet for High Temperature Superconducting Injector Cyclotron

HTS Magnets for Accelerator Applications

HIRFL STATUS AND HIRFL-CSR PROJECT IN LANZHOU

Isospin symmetry structure of J π =1 + states in 58 Ni and 58 Cu studied by high-resolution 58 Ni( 3 He,t) and 58 Ni(p,p ) measurements

STATUS OF THE CYCLOTRON CASCADE AND FUTURE PROSPECT AT RCNP

Notes on the HIE-ISOLDE HEBT

The Research Center for Nuclear Physics Ring Cyclotron

Research Activities at the RCNP Cyclotron Facility

Beam Diagnostics and Instrumentation JUAS, Archamps Peter Forck Gesellschaft für Schwerionenforschnung (GSI)

Heavy Ion Accelerators for RIKEN RI Beam Factory and Upgrade Plans. Upgrade Injector

The heavy ion irradiation facility at KVI-CART

Operational Experience in PIAVI-ALPI Complex. E. Fagotti INFN-LNL

DEVELOPMENT OF FFAG AT KYUSYU UNIVERSITY

2. Acceleration Scheme

Present status of RIBF accelerators at RIKEN

DEVELOPMENT OF JINR FLNR HEAVY-ION ACCELERATOR COMPLEX IN THE NEXT 7 YEARS

Progress in April December 2007 Schedule in Jan. March 2008

Preliminary Simulation of Beam Extraction for the 28 GHz ECR Ion Source

An Introduction to the Ion-Optics of Magnet Spectrometers

Design and test of an Accelerator Driven Neutron Activator at the Joint Research Centre of the European Commission

Magnetic Field Design for a 2.45-GHz ECR Ion Source with Permanent Magnets

Beam Diagnostics for RIBF in RIKEN

Multi-Purpose Accelerator-Accumulator ITEP-TWAC for Nuclear Physics and Practical Applications

THE SUPER-FRS PROJECT AT GSI

Beam diagnostics: Alignment of the beam to prevent for activation. Accelerator physics: using these sensitive particle detectors.

GANIL STATUS REPORT. B. Jacquot, F. Chautard, A.Savalle, & Ganil Staff GANIL-DSM/CEA,IN2P3/CNRS, BP 55027, Caen Cedex, France.

STORAGE RINGS FOR RADIO-ISOTOPE BEAMS

Status of the EBIT in the ReA3 reaccelerator at NSCL

III. CesrTA Configuration and Optics for Ultra-Low Emittance David Rice Cornell Laboratory for Accelerator-Based Sciences and Education

Ion Beam Cocktail Development and ECR Ion Source Plasma Physics Experiments at JYFL

Status & Plans for the TRIUMF ISAC Facility

DUBNA CYCLOTRONS STATUS AND PLANS

Status of the ESR And Future Options

Development and application of the RFQs for FAIR and GSI Projects

Basic Principle of Cyclotron

arxiv: v2 [physics.acc-ph] 21 Jun 2017

STATUS REPORT ON SPIRAL1 F. Chautard October 2 nd, 2007

The Accelerator System for ReA3 the New Re-accelerated RIBs Facility at MSU

High-resolution Study of Gamow-Teller Transitions

Progress of RAON Heavy Ion Accelerator Project in Korea

THE DESIGN AND COMMISSIONING OF THE ACCELERATOR SYSTEM OF THE RARE ISOTOPE REACCELERATOR ReA3 AT MICHIGAN STATE UNIVERSITY*

NSCL and Physics and Astronomy Department, Michigan State University Joint Institute for Nuclear Astrophysics

Magnetic Separator for light RIB production

Performance of the ANL ECR Charge Breeder. with Low Mass Beams. Investigations with low mass species. Review of charge breeder design

Ion Implanter Cyclotron Apparatus System

Accelerator Physics, BAU, First Semester, (Saed Dababneh).

A PRELIMINARY ALIGNMENT PLAN FOR RIA AT MSU

Development of the UNILAC towards a Megawatt Beam Injector

The Ring Branch. Nuclear Reactions at. Mass- and Lifetime Measurements. off Exotic Nuclei. Internal Targets. Electron and p. Experiments: Scattering

LOLA: Past, present and future operation

TAMU-TRAP facility for Weak Interaction Physics. P.D. Shidling Cyclotron Institute, Texas A&M University

Nano-ECRIS project: a new ECR ion source at Toyo University to produce endohedral fullerenes

Investigation on the spiral inflector and central region of the IsoDAR test-bench cyclotron

UPGRADE AND COMMISSIONING OF THE PIAVE-ALPI ECR INJECTOR AT LNL

Direct-Current Accelerator

Report on PIAVE G. Bisoffi

The FAIR Accelerator Facility

UPGRADE OF THE HIT INJECTOR LINAC-FRONTEND

The accelerators at LNS - INFN and diagnostics aspects of the radioactive beams

VELA/CLARA as Advanced Accelerator Studies Test-bed at Daresbury Lab.

OPERATION STATUS OF HIGH INTENSITY ION BEAMS AT GANIL

Analysis of a Cyclotron Based 400 MeV/u Driver System For a Radioactive Beam Facility

Weak focusing I. mv r. Only on the reference orbit is zero

THE ACCULINNA AND ACCULINNA-2 RADIOACTIVE ION BEAM FACILITY AT DUBNA: STATUS AND PERSPECTIVES

A CYCLOTRON TEST SITE FOR NEUTRINO EXPERIMENTS

UPGRADE OF THE HIT INJECTOR LINAC-FRONTEND

University of Huddersfield Repository

Section 4 : Accelerators

II. 5. Study for NaI(Tl) and Scintillation Fiber with 80 MeV Proton Beam Toward ESPRI Experiment at NIRS-HIMAC, RIKEN-RIBF

The CIS project and the design of other low energy proton synchrotrons

IBA C400 Cyclotron Project for hadron therapy

Polarized Proton Acceleration at the J-PARC Accelerator Complex

Structural Modifications of Cyclotron to Produce New Therapeutic & Diagnostic Particles

Particle physics experiments

ANURIB Advanced National facility for Unstable and Rare Ion Beams

Refurbishment of the Electrostatic Accelerators of ithemba LABS

ARIEL at TRIUMF: science, status and opportunities

Alberto Garbayo - MEng (hons) CEng Business Development Manager

Magnetic field simulation in the central region of the VINCY Cyclotron

Accelerators for the Advanced Exotic Beam Facility

The scanning microbeam PIXE analysis facility at NIRS

RF systems for the MAX IV rings

positron source EPOS - general concept - timing system - digital lifetime measurement

Chopping High-Intensity Ion Beams at FRANZ

SC-ECR ion source for RIKEN RIBF

Ne(alpha,n) revisited

Small Isochronous Ring (SIR) project at NSCL, MSU. Eduard Pozdeyev NSCL, Michigan Sate University

Charge State Breeding for the. at TRIUMF

Minicourse on Experimental techniques at the NSCL Fragment Separators

DEVELOPMENT OF LARGE SCALE OPTIMIZATION TOOLS FOR BEAM TRACKING CODES*

The RI Beams from the Tokai Radioactive Ion Accelerator Complex (TRIAC)

1.4 The Tools of the Trade!

Department of Radiation Protection, Nuclear Science Research Institute, Japan Atomic Energy Agency

1 AT/P5-05. Institute of Applied Physics, National Academy of Sciences of Ukraine, Sumy, Ukraine

DESIGN AND CONSTRUCTION OF LOW ENERGY ELECTRON ACCELERATORS AT SINP MSU

SLS at the Paul Scherrer Institute (PSI), Villigen, Switzerland

Robert A. Meger Richard F. Fernster Martin Lampe W. M. Manheimer NOTICE

The SARAF CW 40 MeV Proton/Deuteron Accelerator

New Tandetron Accelerator Laboratory at MTA Atomki, Debrecen: Multi-Purpose and Multi-User Facility

Transcription:

CYCLOTRONS 2007 The 18th International Conference on Cyclotrons and Their Applications Developments of the RCNP cyclotron cascade K. Hatanaka,, M. Fukuda, T. Saito, T. Yorita,, H. Tamura, M. Kibayashi, H. Okamura, A. Tamii,, Y. Sakemi, K. Nagayama,, M. Uraki,, S. Morinobu Research Center for Nuclear Physics Osaka University October 3, 2007 Giardini Naxos, Messina, Italy

Outline 1.RCNP Cyclotron Facility 2.Flat Flat-top top Acceleration System (TUPPRA27) 3.18 GHz Superconducting ECR Ion Source 4.New Beam Line 5.New Control System 6.New Power Supplies 7.Summary

Cryogenic UCN Source RI beam R I Ring Cyclotron K=400 MeV since 1992 DE/E ~ 0.01% 10ucn/cc at 90neV (with 400W proton) Double Arm Spectrometer White Neutron Source AVF Cyclotron K=140 MeV since 1973 DE/E < 0.1% Energy Resolution DE/E ~ 0.005% RI production RI Upgraded recently

Neutron White Neutron energy spectrum Source

Research programs at the RCNP cyclotron facility Nuclear Physics Few nucleon system Medium modification of the interaction Spin isospin excitations Giant resonance Heavy ion physics with radioactive isotopes... Fundamental Symmetry Ultra Cold Neutron 210 Fr EDM Interdisciplinary Researches Nuclear chemistry Biological science Material science Radiation damage of semiconductor devices

Requirements for Beam Conditions of AVF Cyclotron Conditions High Intensity Mode High Resolution Mode Flat-top Acceleration Intensity a few ma hundreds na Increasing Energy spread 1 ~ 5*10-3 0.5 ~ 1*10-3 ~ 1*10-4 Emittance 10p mm mr ~ 5p mm mr < 5p mm mr Extraction Multi-turn Quasi-single-turn Pure single-turn Transmission efficiency Low High Very high Beam halo Small Small Halo-free

Principle 2. Flat-top top Acceleration System Fundamental Acceleration Sinusoidal voltage waveform Acceleration region Flat-top Acceleration Flat-top voltage waveform Voltage Time Superimposing harmonic voltage Voltage Energy spread E/E 0 = 10-3 E 0 harmonic voltage waveform Energy spread E/E 0 = 10-4 E 0 Intensity E Intensity E Energy Energy

3 rd harmonics First harmonics

Flat-top top Cavity Characteristics Harmonic frequency : 50 Harmonics : k = 5, 7, 9 80 MHz Flat-top cavity Outer tube 170 mm Length 700 mm Layout of RF system Capacitively coupled to the main resonator Dee voltage pickup New Dee electrode with a 10 mm wide and 1 m long slot

Flat-top top Voltage Waveform Dee-voltage pickup electrode Example of the pickup voltage waveform 53MeV proton (300MeV @Ring) f 1 = 15.417 MHz f 5 = 77.084 MHz 40 4 electrodes facing the Dee electorode, placed near the acceleration gap, used for regulation of RF system. Voltage (mv) 20 0-20 -40 100 200 300 400 500 Phase (RF degrees)

Improvement of 300 MeV Proton Beam Energy spread and intensity of 300 MeV proton beam - transferred to Grand-RAIDEN in achromatic mode - elastically scattered off a gold target : 197Au(p, p) at 8 deg., 1.68 mg/cm 2 thick So far April in 2004 Recent result April in 2007 AVF : Fundamental acceleration Ring : Flat-top acceleration 5 na (20 na for E=70 kev) AVF : Flat-top acceleration Ring : Flat-top acceleration 20 na (60 na for E=70 kev) 37 kev FWHM 30 kev FWHM!!

3. 18 GHz Superconducting ECR Ion Source Highly charged heavy ions A variety of heavy ions at high intensity

Superconducting Coils Sectional view of the superconducting ECR ion source Axial magnetic field distribution produced by the superconducting mirror coils Hexapole permanent magnet Aperture : 90mm Plasma chamber Inner diameter : 80mm D C U2 U1

Production of Heavy Ions Gaseous ions such as 16, 18 O, 40 Ar, 86 Kr 11 B ion by MIVOC method using o-carborane(c 2 B 10 H 12 ) Example of beam currents Provided for users

Charge State Distributions (I) 16 O 18 O 40 Ar 86 Kr

Charge State Distribution (II) Production of 11 B ion - MIVOC (Metal Ion from VOlatile Compounds) - o-carborane (C 2 B 10 H 12 ) - vapor pressure of 1-2 Torr. 11 B

4. New Beam Line Profile monitor Emittance Slit Achromatic Transport Horizontal Focal Plane Vertical Emittance monitor - Beam diagnosis : energy spread and emittance Profile Monitor - Bypass line : transportation Emittance monitor of the low energy Focal plane beam from the AVF cyclotron Slit directly to experimental halls Profile Monitor

Emittance Measurement =5p mm mrad

Energy Spread Measurement Ring Cyclotron 14 12 10 using 9th harmonics Current (na) 8 6 4 Width Energy spread 2 0 20 25 30 35 40 45 50 X (mm) Focal Plane Profile monitor Analyzing section (D=12.6m, M=1) Dispersive Transport Vertical Horizontal

5. New Control System Background of the renewal - Difficulty in maintenance of the Micro VAX system - Very slow processing speed PC-base control system - Maintaining hierarchical control system - Distributed control system using network - 3 sets of main console - InTouch software for human machine interface New local controller - PLC(Programmable Logic Controller) New control room

6. New Power Supplies Background of the renewal - More than 35 years have passed since the fabrication of the AVF cyclotron. - Most of electric parts are not available now. Trim coil power supplies - 16 power supplies - modification of max. coil currents RF power supplies for a final amplifier tube - Screen-grid - Control-grid - Filament New power supplies for 13 pairs of trim coils

7. Summary The upgrade of the RCNP AVF cyclotron has been successfully started and is continued. The beam quality and intensity of 300 MeV proton has been improved by the flat-top acceleration in the AVF cyclotron. Developments are being performed to apply the system to other beams. An 18 GHz superconducting ECR ion source has been commissioned to increase the beam intensity of highly-charged heavy ions; 7.5 MeV /u 86 Kr 23+ was delivered for experiments. A new beam line has been installed to diagnose the quality of the beam from the AVF cyclotron and helps to make it match to the acceptance of the ring cyclotron. It also makes 10-400 MeV protons and 1-100 MeV/u heavy ions available for a variety of researches in nuclear physics and fundamental physics as well as interdisciplinary studies.

Development of Flat-top top Accelerated Beam Particle Energy (MeV) AVF fundamental Harmonics Ring AVF frequency (MHz) Order Freq. (MHz) 4 He 400 87.14 10.144018 5 50.72009 7 71.008126 3 He 420 87.81 11.65007 5 58.25035 86 Kr 21+ 640 6.0129 9 54.1161 d 80 18.73 6.75 9 60.75 pol.d 200 43.6 10.11632 5 50.5816 p 200 39.32 13.375664 5 66.87832 p 250 46.7 14.496449 5 72.482245 p 300 53.3 15.416773 5 77.083865 Under development

3 rd harmonics First harmonics