Nanuf03, Bucharest, 7.-12. 9. 2003Stefan Kopecky Traps for fission product ions at IGISOL Experimental Facilities Mass Measurements Status and Future Perspectives.

Slides:

Advertisements

Similar presentations

ISAC Physics Working Group Convenors Malcolm Butler and Barry Davids.

Advertisements

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

SYNTHESIS OF SUPER HEAVY ELEMENTS

Daisuke Kameda BigRIPS team, RIKEN Nishina Center

Penning-Trap Mass Spectrometry for Neutrino Physics

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.

Testing isospin-symmetry breaking and mapping the proton drip-line with Lanzhou facilities Yang Sun Shanghai Jiao Tong University, China SIAP, Jan.10,

JYFLTRAP: Spectroscopy with multi-trap facility Facility Mass purified beams In-trap spectroscopy Future plans.

High precision study of the  decay of 42 Ti  V ud matrix element and nuclear physics  Experimental and theoretical precisions  New cases: goals and.

Operational aspects 2008 run ISCOOL Isolde workshop Nov 2008 Erwin Siesling.

The ion trap facility SHIPTRAP at GSI Status and Perspectives Michael Block for the SHIPTRAP collaboration.

Laser pumping of ions in a cooler-buncher The University of Manchester, UK The University of Birmingham, UK At the JYFL accelerator facility, Finland.

55. Jahrestagung der ÖPG, September 2005 Pionischer Wasserstoff: Präzisionsmessungen zur starken Wechselwirkung J. Marton Stefan Meyer Institut der ÖAW.

The LaSpec project. At FAIR… Cheapest(?),Fully destripped…

Coulomb excitation and  -decay studies at (REX-)ISOLDE around Z = 28 J. Van de Walle – KVI - Groningen 1. ISOLDE and REX-ISOLDE ; 2. Results around Z=28.

DESIR  SPIRAL2 organization & scientific program layout of the facility status and perspectives LUMIERE  Laser DESIR: the LUMIERE.

The CARIBU facility Guy Savard Argonne National Laboratory & University of Chicago ATLAS Users Meeting May

ISCC 24 May 2004L.M. Fraile L.M. Fraile, CERN PH/IS ISOLDE scientific coordinator’s report ISOLDE Collaboration Committee 24 th May 2004 ISOLDE scientific.

The polar experience: IGISOL proposal I77, study of the beta decay of 102,104,105 Tc by means of the total absorption technique A. Algora IFIC-Univ. Valencia.

Lecture 2:Research frontiers 1 9/9/ FYPC Most recent long range planning reports: FYPC (Canada), NSAC (USA) Collision products at RHIC.

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

Decay Spectroscopy Working Group Nuclear Structure Theory Morten Hjorth-Jensen – Shell Structure and Interactions Ivan Borzov – Theory of  Decay Applications.

N=126 factory Guy Savard Scientific Director of ATLAS Argonne National Laboratory & University of Chicago ATLAS Users Meeting ANL, May 15-16, 2014.

TITAN Mass Measurement of 11 Li (and other halo nuclei) Ryan Ringle, TRIUMF.

Preparation of an isomerically pure beam and future experiments Outline TAS Workshop, Caen, March 30-31, 2004 Klaus Blaum for the ISOLTRAP Collaboration.

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.

Mass measurements using low energy ion beams -1- C. Thibault 31 mars 2004 Motivations to measure masses Present status Experimental methods for direct.

Исследование запаздывающего деления и сосуществования форм в ядрах таллия, астата и золота (ИРИС, ПИЯФ — ISOLDE, CERN) A. E. Барзах, Ю. M. Волков, В. С.

Simple Atom, Extreme Nucleus: Laser Trapping and Probing of He-8 Zheng-Tian Lu Argonne National Laboratory University of Chicago Funding: DOE, Office of.

Status of the ion traps at ATLAS Jason Clark ATLAS users workshop August 8, 2009.

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,

 -capture measurements with the Recoil-Separator ERNA Frank Strieder Institut für Physik mit Ionenstrahlen Ruhr-Universität Bochum HRIBF Workshop – Nuclear.

Contribution of Penning trap mass spectrometry to neutrino physics Szilárd Nagy MPI-K Heidelberg, Germany New Instruments for Neutrino Relics and Mass,

1 stephan ettenauer for the TITAN collaboration Experimental Program on Halo Nuclei with non-accelerated Beams at TRIUMF Weakly Bound Systems in Atomic.

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

Masses of tripline nuclei Frank Herfurth, ISOLDE/CERN.

Fundamental Interactions Physics & Instrumentation Conclusions Conveners: P. Mueller, J. Clark G. Savard, N. Scielzo.

LLNL-PRES This work was performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under contract DE-AC52-07NA27344.

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

The FAIR* Project *Facility for Antiproton and Ion Research Outline:  FAIR layout  Research programs Peter Senger, GSI USTC Hefei Nov. 21, 2006 and CCNU.

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.

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:

W. Nazarewicz. Limit of stability for heavy nuclei Meitner & Frisch (1939): Nucleus is like liquid drop For Z>100: repulsive Coulomb force stronger than.

Outline Sebastian George Tokyo 2007 High-Precision Mass Spectrometry

1 CNS summer school 2002 The RI-Beam Factory and Recent Development in Superheavy Elements Search at RIKEN ◆ Brief introduction to the RI Beam Factory.

Variational approach to isospin symmetry breaking in medium mass nuclei A. PETROVICI Institute for Physics and Nuclear Engineering, Bucharest, Romania.

Precision mass measurements of n-rich nuclei between N=50 and 82. Short overview on the experimental approach Penning trap mass measurements on n-rich.

ISOLDE Physics Report Magdalena Kowalska. Injector schedule since last meeting 2 September: confirmation of 2 more weeks with protons – until December.

February 12-15,2003 PROCON 2003, Legnaro-Padova, Italy Jean Charles THOMAS University of Leuven / IKS, Belgium University of Bordeaux I / CENBG, France.

The HITRAP Project at GSI For the HITRAP collaboration: Frank Herfurth GSI Darmstadt.

G. Bollen, INTC-NUPAC Meeting, CERN, Geneva, October 2005 Overview and Motivation Mass Measurements at ISOLDE … … and elsewhere Conclusions Mass Measurements.

Alexander Herlert High-precision mass measurements for reliable nuclear-astrophysics calculations CERN, PH-IS NIC-IX, CERN, Geneva, June 29, 2006.

Technical solutions for N=Z Physics David Jenkins.

TRIGA-SPEC: Developement platform for MATS and LaSpec at FAIR Double-beta transition Q-value measurements with TRIGA-TRAP NUSTAR Meeting Christian.

How can one produce rare isotopes? Question Slid 3 Hendrik Schatz NNPSS 2012, Slide 3 Rare Isotope Production Techniques: Uniqueness of FRIB Target spallation.

Michael Dworschak, GSI for the SHIPTRAP collaboration

FIDIPRO-JSPS Workshop, Keurusselkä , AriJokinen, JYFL Nuclear structure probed by precision atomic mass measurements in a Penning trap Ari.

Max-Planck-Institut für Kernphysik, Heidelberg Zhuang GE RIKEN, Wako, Japan Mass measurements of short-lived nuclides at storage rings in Asia and its.

The DESIR facility at SPIRAL2

PIPERADE: A Penning trap isobar separator for SPIRAL2/DESIR

One way to improve first class mass ISOLTRAP

The role of isospin symmetry in medium-mass N ~ Z nuclei

JYFL ION COOLER AND BUNCHER.

Emmanuel Clément IN2P3/GANIL – Caen France

Presentation transcript:

Nanuf03, Bucharest, Stefan Kopecky Traps for fission product ions at IGISOL Experimental Facilities Mass Measurements Status and Future Perspectives Experimental Facilities Mass Measurements Status and Future Perspectives

Nanuf03, Bucharest, Stefan Kopecky IGISOL Fission Yields

Nanuf03, Bucharest, Stefan Kopecky IGISOL (Ion Guide Isotope Separation Online) Short delay Times Chemical Insensitive Large Energy Spread (100 eV) Continuous Beam

Nanuf03, Bucharest, Stefan Kopecky RFQ-Trap Layout

Nanuf03, Bucharest, Stefan Kopecky RFQ-cooler

Nanuf03, Bucharest, Stefan Kopecky Radial confinement +Vcos  t -Vcos  t

Nanuf03, Bucharest, Stefan Kopecky Axial confinement Transmission 50 % Bunch width 2-3  s Energy spread <1 eV

Nanuf03, Bucharest, Stefan Kopecky Collinear Laser-Spectroscopy increased by a factor of 10 reduced by a factor of 20 =R ph  T gate /T acc =  F overlap  F doppler   geom   PM  F atom

Nanuf03, Bucharest, Stefan Kopecky Magnet 7T superconducting Magnet Magnex Scientific Ltd 160mm warm bore 2 homogenous regions 1cm and 10 -7

Nanuf03, Bucharest, Stefan Kopecky Purification Trap Electrode Structure

Nanuf03, Bucharest, Stefan Kopecky Radial Motion without buffer gaswith buffer gas Magnetron motion  - Cyclotron motion  +  - +  + =  C = qB/m Cyclotron radius decreases Magnetron radius increases

Nanuf03, Bucharest, Stefan Kopecky Dipol –Excitation with  - HP33120A

Nanuf03, Bucharest, Stefan Kopecky Quadrupol –Excitation with  C 126 Xe HP33120A

Nanuf03, Bucharest, Stefan Kopecky Fast-scheme Total cycle time 120ms p = 9.9 e-2 mbar Cooling time 55 ms  - 5ms / 300mV  C 55ms / 350mV FWHM = 35Hz R = m/  m = Xe

Nanuf03, Bucharest, Stefan Kopecky Best Mass resolution 58 Cu 58 Ni FWHM=13,6Hz R= Mass Excess Our result: /- 30keV AME95: /- 2.5keV FWHM=13,8Hz R=134100

Nanuf03, Bucharest, Stefan Kopecky Purification Trap Transmission between % – spark ion source, stable Xe, Faraday-cup –  -activity, Fission products A=112 ( Rh-112), Si-detector Capturing efficiency of trap 60% Total Efficiency 20%  Front end for Precision Trap  Isobaric pure beams for Decay Spectroscopy  Mass Measurements

Nanuf03, Bucharest, Stefan Kopecky p-induced fission, A=112 Ru-112 T 1/2 =1.75s Rh-112 T 1/2 =2.1s Q  =3.670MeV Pd-112 T 1/2 =21.03h Q  =6.8 MeV

Nanuf03, Bucharest, Stefan Kopecky Beam Purification

Nanuf03, Bucharest, Stefan Kopecky Tof-methode

Nanuf03, Bucharest, Stefan Kopecky Tof-resonance

Nanuf03, Bucharest, Stefan Kopecky Fundamental interactions and symmetries (< 1 keV) –Q-values of nuclear  decay CVC theory and unitarity of CKM matrix Search for scalar and tensor currents Charge symmetry in nuclei (1 keV) –Isospin multiplets and Coulomb energy differences Nuclear structure ( keV) –Global correlations (100 keV) –Local correlations (10 keV) Local deformation, coexistence, mixing and pairing –Drip-line phenomena and halos (10 keV) Nuclear astrophysics (>10 keV) What level of accuracies are needed?

Nanuf03, Bucharest, Stefan Kopecky Structure of neutron-rich Zr-isotopes ” Ground state changes from spherical to deformed via coexistence” See, G. Lhersonneau et al.,Phys. Rev. C49(1994)1379 & refs. No reliable direct mass measurements existed so far!

Nanuf03, Bucharest, Stefan Kopecky 104 Zr Total cycle time 450ms p = 3 e-2 mbar Cooling time 330 ms  - 15ms / 160mV  C 90ms / 190mV FWHM = 18 Hz R = Zr-measurement

Nanuf03, Bucharest, Stefan Kopecky preliminary Zr results

Nanuf03, Bucharest, Stefan Kopecky preliminary Zr results

Nanuf03, Bucharest, Stefan Kopecky Nuclear Mean Field Calculation Stoitsov M.V, Dobaczewski J. and Nazarewicz W., to be published

Nanuf03, Bucharest, Stefan Kopecky Z=40, A=100 -region Mo Nb Zr Y Sr

Nanuf03, Bucharest, Stefan Kopecky Summary RFQ-Cooler Reduce in energy spread of ion beam (<1eV) Bunching of beam (  s)  Improved condition for Collinear Laser Spectroscopy  Front end for Purification Trap Purification Trap Isobaric Pure beams ( R = ) Cycle Times ( 120ms - 450ms)  Front End for Precision Trap  Decay Spectroscopy of Exotic Nuclei  Mass Measurement for Nuclear Structure Effects Precision Trap  High Precision Mass Measurements