JYFL ION COOLER AND BUNCHER.

Slides:



Advertisements
Similar presentations
What is the ISOLDE cooler RFQ CB - ISCOOL H. Frånberg.
Advertisements

Design and Experimental Considerations for Multi-stage Laser Driven Particle Accelerator at 1μm Driving Wavelength Y.Y. Lin( 林元堯), A.C. Chiang (蔣安忠), Y.C.
ISOLDE WS 2007 Results with ISCOOL a new Radio Frequency Quadrupole Cooler and Buncher at ISOLDE P. Delahaye, H. Frånberg, AB-OP-PSB, ISCOOL, COLLAPS,
EURISOL_DS – Task 11 Subtask 5 Neutron- and proton-induced reactions up to Fermi energy J. Äystö / V. Rubchenya JYFL, Jyväskylä (P9) / KhRI, St.Petersburg.
JYFLTRAP: Spectroscopy with multi-trap facility Facility Mass purified beams In-trap spectroscopy Future plans.
electrostatic ion beam trap
Operational aspects 2008 run ISCOOL Isolde workshop Nov 2008 Erwin Siesling.
Laser pumping of ions in a cooler-buncher The University of Manchester, UK The University of Birmingham, UK At the JYFL accelerator facility, Finland.
Intense Field Femtosecond Laser Interactions AMP TalkJune 2004 Ultrafast Laser Interactions with atoms, molecules, and ions Jarlath McKenna Supervisor:
The LaSpec project. At FAIR… Cheapest(?),Fully destripped…
Mass Spectrometry.
The CARIBU facility Guy Savard Argonne National Laboratory & University of Chicago ATLAS Users Meeting May
Photoelectron Spectroscopy Lecture 7 – instrumental details –Photon sources –Experimental resolution and sensitivity –Electron kinetic energy and resolution.
On-line tests RFQ cooler ISCOOL A quick summary P. Delahaye, H. Frånberg, I. Podadera ISCOOL, COLLAPS, ISOLDE collaboration.
Ion Beam Cocktail Development and ECR Ion Source Plasma Physics Experiments at JYFL Olli Tarvainen 11th International Conference on Heavy Ion Accelerator.
Proposed injection of polarized He3+ ions into EBIS trap with slanted electrostatic mirror* A.Pikin, A. Zelenski, A. Kponou, J. Alessi, E. Beebe, K. Prelec,
Structures and shapes from ground state properties 1.Nuclear properties from laser spectroscopy 2.Status of laser measurements of moments and radii 3.New.
Collinear laser spectroscopy of 42g,mSc
N=126 factory Guy Savard Scientific Director of ATLAS Argonne National Laboratory & University of Chicago ATLAS Users Meeting ANL, May 15-16, 2014.
Radioactive ion beam facilities How does they work ? 2012 Student Practice in JINR Fields of Research 9.oct.2012 I. Sivacekflerovlab.jinr.ru.
Zoran Andjelkovic Johannes Gutenberg Universität Mainz GSI Darmstadt Laser Spectroscopy of Highly Charged Ions and Exotic Radioactive Nuclei (Helmholtz.
Duncan J S Johnson.  Determine nuclear properties by observing HFS via collinear laser spectroscopy.  Currently in the process of studying manganese.
Mass measurements using low energy ion beams -1- C. Thibault 31 mars 2004 Motivations to measure masses Present status Experimental methods for direct.
Calculation of the beam dynamics of RIKEN AVF Cyclotron E.E. Perepelkin JINR, Dubna 4 March 2008.
Laser Laboratory (-ies) Peter Müller. 2 Search for EDM of 225 Ra Transverse cooling Oven: 225 Ra (+Ba) Zeeman Slower Optical dipole trap EDM probe Advantages:
28. November 2005 Fission product yield measurements with JYFLTRAP A novel application of a Penning trap H. Penttilä, J. Äystö, V.-V. Elomaa, T. Eronen,
International Workshop on Stopping and Manipulation of Ions, Groningen, 28 March 2006 Latest developments at the IGISOL laser ion source Iain Moore University.
RFQ cooler and buncher project for ISOLDE Present status and off-line test results Hanna Frånberg, ISOLDE.
The REXTRAP Penning Trap Pierre Delahaye, CERN/ISOLDE Friedhelm Ames, Pierre Delahaye, Fredrik Wenander and the REXISOLDE collaboration TAS workshop, LPC.
Ion Preparation in TITAN’s RFQ
Fundamental Interactions Physics & Instrumentation Conclusions Conveners: P. Mueller, J. Clark G. Savard, N. Scielzo.
 angular correlations LPC-Team : G. Ban, G. Darius, P. Delahaye, D. Durand, X. Flechard, M. Herbane, M. Labalme, E. Liénard, F. Mauger, A. Mery, O. Naviliat,
A new RFQ cooler: concept, simulations and status Trapped Radioactive Isotopes:  icro-laboratories for Fundamental Physics E. Traykov TRI  P project.
A mass-purification method for REX beams
1 Laser Background 2 Apparatus Overview 3 Ion Beam Properties A Energy Spread B Spatial Spread 4 Xe + & Xe 2+ In Laser 5 Z-Scan of Laser Focus 6 Summary.
Molecular Triplet States: Excitation, Detection, and Dynamics Wilton L. Virgo Kyle L. Bittinger Robert W. Field Collisional Excitation Transfer in the.
ECT* - The interplay between atomic and nuclear physics, Trento 2015 Laser Spectroscopy of Cd: Simple Trends in Complex Nuclei D. T. Yordanov for.
Status Report of the LISOL Laser Ion Source Yu.Kudryavtsev, T.Cocolios, M.Facina, J.Gentens, M.Huyse, O.Ivanov, D.Pauwels, M.Sawicka, P.Van den Bergh,
A systematic study of  - decay of neutron-rich Rh and Ag isotopes Sixth China Japan Joint Nuclear Physics Symposium Shanghai, May 16-20, 2006 Youbao Wang.
Nanuf03, Bucharest, Stefan Kopecky Traps for fission product ions at IGISOL Experimental Facilities Mass Measurements Status and Future Perspectives.
Laser pumping of ions in a cooler-buncher.. Introduction to laser spectroscopy Ion source (60kV)Laser PMT Gates Tuning voltage Isotope Shifts   Size.
PARALLEL PLATES. From previous work, the electric field strength can be found from the electric force on a test charge.
FLAIR meeting, GSI March Positron Ring for Antihydrogen Production A.Sidorin for LEPTA collaboration JINR, Dubna.
Trends in Heavy Ion Physics Research, Dubna, May Present and future physics possibilities at ISOLDE Karsten Riisager PH Department, CERN
Direct measurement of the 4 He( 12 C, 16 O)  cross section near stellar energy Kunihiro FUJITA K. Sagara, T. Teranishi, T. Goto, R. Iwabuchi, S. Matsuda,
Magnetic Reconnection in Plasmas; a Celestial Phenomenon in the Laboratory J Egedal, W Fox, N Katz, A Le, M Porkolab, MIT, PSFC, Cambridge, MA.
The HITRAP Project at GSI For the HITRAP collaboration: Frank Herfurth GSI Darmstadt.
Design and Development of a Trochoidal Mass Separator at the Berkeley Gas-filled Separator J.M. Gates, K.E. Gregorich, G.K. Pang, N.E. Esker and H. Nitsche.
TRI  P RFQ design, simulations and tests E. Traykov TRI  P project and facility RFQ tests and design Simulations Conclusion TRI  P Group: G.P. Berg,
TRIGA-SPEC: Developement platform for MATS and LaSpec at FAIR Double-beta transition Q-value measurements with TRIGA-TRAP NUSTAR Meeting Christian.
Beam Preparation, Task 9 Department of Physics, University of Jyväskylä.
AP Physics Summer Institute Free-Response-Questions MAGNETISM.
ESS | Non-Invasive Beam Profile Measurements| | C. Böhme Non-Invasive Beam Profile Measurement Overview of evaluated methods.
Alexander Aleksandrov Spallation Neutron Source Oak Ridge, USA
Traps for antiprotons, electrons and positrons in the 5 T and 1 T magnetic fields G. Testera & Genoa group AEGIS main magnetic field (on axis) : from Alexei.
One way to improve first class mass ISOLTRAP
Elettra Sincrotrone Trieste
& Figures Descriptions
Fragmentation and lifetime of C60q+ trapped in a cone trap
First results from IS468 and further investigation of in-trap decay of 62Mn First results from 2008 ; Problems and questions ; Further investigations ;
Siara Fabbri University of Manchester
Wakefield Accelerator
Laser assisted decay spectroscopy at the cris beam line at
Introduction to ISOLDE RFQ
Precision Measurements of Very-Short Lived Nuclei
New Observations from the Hyperfine Structure of 49,51K
Chapter 29 Problems Problems 7, 9, 12, 30, 37, 41.
Studies of Emittance & Lifetime
Low Energy Electron-Ion Collision
Improvement of a dc-to-pulse conversion efficiency of FRAC
Presentation transcript:

JYFL ION COOLER AND BUNCHER

The JYFL IGISOL facility High Voltage Cyclotron beam Ion guide Separator magnet Beam switchyard Ion Beam Cooler 90 bend High Voltage Penning Trap 1 2 m

Cooler layout Ion beam cooler Central beam line Cooler beam line Beam switchyard

89Y

Energy spread Collinear laser spectroscopy setup Off-line Barium beam dEFWHM < 4 eV 20 MHz doppler broadening Beam intensity cut off vs. bias voltage. Intensive beams (129Xe, few nA) dEFWHM = 1.5 eV On-line beams 105 ions/s dEFWHM = 0.7 eV Off-line 129Xe+

Delay time IGISOL delay time ~ms Without axial field: diffusion, space charge Depends on: - Einj - dEinj - pHe Without axial field up to hundreds of ms Shorter by axial electric field (down to ms region) Longer  beam bunching

ii iii iv i

Transmission - 29 MeV proton induced fission of 238U - Normal ion guide pressure 250 mbar - Skimmer voltage varied - A = 112 IGISOL beam (mostly 112Rh) - Beta count rate in two Si-detector setups, before and after the cooler - Transmission > 60 %

Bunching - Separator beam on t = 0 - 1000 ms Z +2 V +1 V +0.5 V -1V +70 V (collect) 0 V (release) Potential along z - axis - Separator beam on t = 0 - 1000 ms - Cooler end plate voltage down t = 3300-4000 ms

Delayed Ion-photon coincidence method LCR LASER IONS Delayed Ion-photon coincidence method Bunched beam method Photons gated on the ion bunch Counts Singles photons Photons gated on the ion bunch Ion Beam Energy Tuning (eV)

Bunch width - Mass and Space charge effects 174Hf ttrap = 0.5 s Gate1 = 15 ms Gate1 = 30 ms Gate1 = 75 ms Hf 15(1) ms Ti 10(1) ms (with <10 000 ions/bunch)

Ion survival in the Buncher

On-line photon efficiency in collinear laser spectroscopy (ion survival) Without the buncher - Metastable population - IGISOL pressure P. Campbell et al. Hypf. Int. 127 (2000) With the buncher - Off-line efficiencies hold metastables reduced - No IGISOL pressure effects (below fig. pIG=450 mbar)