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

Slides:



Advertisements
Similar presentations
ISAC Physics Working Group Convenors Malcolm Butler and Barry Davids.
Advertisements

SYNTHESIS OF SUPER HEAVY ELEMENTS
ATLAS Users Workshop August CARIBU: early science program Guy Savard Argonne National Laboratory and University of Chicago.
Initial Science Case For GRETINA at ATLAS M.P. Carpenter Physics Division, Argonne National Laboratory ANL Gretina Workshop March 1, 2013.
The fission of a heavy fissile nucleus ( A, Z ) is the splitting of this nucleus into 2 fragments, called primary fragments A’ 1 and A’ 2. They are excited.
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.
Γ spectroscopy of neutron-rich 95,96 Rb nuclei by the incomplete fusion reaction of 94 Kr on 7 Li Simone Bottoni University of Milan Mini Workshop 1°-
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.
Mass measurements on neutron-rich nuclei with the CPT mass CARIBU Kumar S. Sharma Department of Physics and Astronomy Winnipeg MB.
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.
ROGER CABALLERO FOLCH, Barcelona, 9 th November 2011.
Multinucleon Transfer Reactions – a New Way to Exotic Nuclei? Sophie Heinz GSI Helmholtzzentrum and Justus-Liebig Universität Gießen Trento, May ,
Estimation of production rates and secondary beam intensities Martin Veselský, Janka Strišovská, Jozef Klimo Institute of Physics, Slovak Academy of Sciences,
218 Po ‘ 218 Po =Radium A’ ‘ 218 At =Radium B’ C D E 210 Po =Radium ‘F’ Radon =‘Emanation’ ‘Radium’ C’ C’’ The Natural Decay Chain for 238 U Aside: information.
The CARIBU facility Guy Savard Argonne National Laboratory & University of Chicago ATLAS Users Meeting May
Spectroscopy and lifetime measurements at ReA12 Hiro IWASAKI (NSCL/MSU) 7/12/2014Recoil Separator for ReA12 workshop1.
© 2003 By Default! A Free sample background from Slide 1 JINR SCIENTIFIC COUNCIL 106 nd Session, 24 September 2009, Dubna.
ATLAS/CARIBU Status Guy Savard Scientific Director of ATLAS Argonne National Laboratory & University of Chicago Workshop on Future GRETINA Science Campaigns.
AGFA – the Argonne Gas-Filled Analyzer Presentation at the 2014 ATLAS User’s Meeting May 15-16, 2014 Birger B. Back.
Nuclear Astrophysics Working Group Discussion. Schedule 6:00 – 6:15Philippe Collon (p-process: AMS) 6:15 – 6:30 Alan Chen (Classical novae/X-ray bursts)
Isospin impurity of the Isobaric Analogue State of super-allowed beta decay experimental technique isospin impurity determination Bertram Blank, CEN Bordeaux-Gradignan.
Noyaux CERN- ISOLDE Yorick Blumenfeld.
Decay Spectroscopy Working Group Nuclear Structure Theory Morten Hjorth-Jensen – Shell Structure and Interactions Ivan Borzov – Theory of  Decay Applications.
Peter G. Thirolf, LMU München The ‘Fission–Fusion‘ Reaction Mechanism: Using dense laser-driven ion beams for nuclear astrophysics for nuclear astrophysics.
Dietrich Habs ELI Photonuclear Bucharest, Feb 2, D. Habs LMU München Fakultät f. Physik Max-Planck-Institut f. Quantenoptik A Laser-Accelerated.
Lawrence Livermore National Laboratory Nicholas Scielzo Lawrence Fellow Physics Division, Physical Sciences LLNL-PRES Lawrence Livermore National.
Mass measurements using low energy ion beams -1- C. Thibault 31 mars 2004 Motivations to measure masses Present status Experimental methods for direct.
Nuclear structure around 100 Sn Darek Seweryniak, ANL.
Nuclear structure around 68 Ni J. Van de Walle, N. Kalantar et al. KVI Groningen Nuclear structure around 68 Ni J. Van de Walle, N. Kalantar et al. KVI.
Status of the ion traps at ATLAS Jason Clark ATLAS users workshop August 8, 2009.
Physics Cases Summary Matt Amthor Bucknell University ReA12 Recoil Separator Workshop – July 12, 2014.
106 th Session of the JINR Scientific Council September 24-25, 2009, Dubna Perspectives of JINR – ORNL Collaboration in the Studies of Superheavy Elements.
-NUCLEUS INTERACTIONS OPEN QUESTIONS and FUTURE PROJECTS Cristina VOLPE Institut de Physique Nucléaire Orsay, France.
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,
Status of the Subtask 6 Heavy ion reactions in the Fermi-energy domain M. Veselsky, IoP SASc Bratislava Main.
Yu. Oganessian FLNR (JINR) PAC–meeting, June 22, 2009, Dubna Experimental activities and main results of the researches at FLNR (JINR) Theme: Synthesis.
Lawrence Livermore National Laboratory Nicholas Scielzo Lawrence Fellow Physics Division, Physical Sciences LLNL-PRES Lawrence Livermore National.
1 Beta Counting System Li XiangQing, Jiang DongXing, Hua Hui, Wang EnHong Peking University
Fundamental Interactions Physics & Instrumentation Conclusions Conveners: P. Mueller, J. Clark G. Savard, N. Scielzo.
Binding energies of neutron-rich isotopes as measured with the CPT at CARIBU Jason Clark CIPANP 2015 May 19-24, 2015.
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.
Reiner Krücken Welcome to Kloster Banz. Reiner Krücken The Munich Accelerator for Fission Fragments at the FRM II in Garching Facility Overview Status.
Probed with radioactive beams at REX-ISOLDE Janne Pakarinen – on behalf of the IS494 collaboration – University of Jyväskylä ARIS 2014 Tokyo, Japan Shapes.
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,
Nanuf03, Bucharest, Stefan Kopecky Traps for fission product ions at IGISOL Experimental Facilities Mass Measurements Status and Future Perspectives.
1 Hypernuclear  -ray spectroscopy via the (K -,  0 ) reaction K. Shirotori Tohoku Univ.
1 Programme Advisory Committee for Nuclear Physics 29 th meeting, January 2009 Programme Advisory Committee for Nuclear Physics 29 th meeting,
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.
Sub-task 4: Spallation and fragmentation reactions M. Valentina Ricciardi (GSI) in place of José Benlliure (USC) Sub-task leader: Universidad de Santiago.
High-precision mass measurements below 48 Ca and in the rare-earth region to investigate the proton-neutron interaction Proposal to the ISOLDE and NToF.
Observation of new neutron-deficient multinucleon transfer reactions
The HITRAP Project at GSI For the HITRAP collaboration: Frank Herfurth GSI Darmstadt.
Closing remarks Key qestions: Location of SHE shell and SHE nuclear structure Atomic properties and relativistic effects Breakdown of Mendelejev systematic.
Welcome to the CHARMS See – Tea Saturday, March 05, 2016 Comparison of ISOLDE yields with calculated in- target production rates Strahinja Lukić,
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.
© 2003 By Default! A Free sample background from Slide 1 JINR SCIENTIFIC COUNCIL 102 nd Session, September 2007, Dubna.
March, 2006SERC Course1  Z>92 (Heaviest Element in Nature) and upto Z= achieved by n irradiation or p,  and d bombardment in Cyclotron ( )
Physics at the extremes with large gamma-ray arrays Lecture 3 Robert V. F. Janssens The 14 th CNS International Summer School CNSSS15 Tokyo, August 26.
Summary: Physics Opportunities for ISOLDE and n_TOF Peter Butler.
Present status of production target and Room design Takashi Hashimoto, IBS/RISP 2015, February.
Decay scheme studies using radiochemical methods R. Tripathi, P. K. Pujari Radiochemistry Division A. K. Mohanty Nuclear Physics Division Bhabha Atomic.
How can one produce rare isotopes? Question Slid 3 Hendrik Schatz NNPSS 2012, Slide 3 Rare Isotope Production Techniques: Uniqueness of FRIB Target spallation.
2 nd SPES Workshop Probing the Island of Stability with SPES beams.
SMI-06 Workshop, Groningen,
JYFL ION COOLER AND BUNCHER.
Recent Highlights and Future Plans at VAMOS
New Transuranium Isotopes in Multinucleon Transfer Reactions
Production Cross-Sections of Radionuclides in Proton- and Heavy Ion-Induced Reactions Strahinja Lukić.
Fission on the Neutron-Rich Side of the Valley of Stability
Presentation transcript:

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

2 ATLAS Users Meeting Guy Savard, Argonne National Laboratory May 15-16, Pb 238 U Accessing new regions: deep-inelastic reactions to reach the far north-east of the nuclear chart The Science:  nuclear shell structure at the extremes  r-process: second abundance peak, fission recycling and termination  fission barriers of neutron-rich nuclei and symmetry energy  connection of hot-fusion SHE island and mainland  Unusual GT vs 1st forbidden beta decay ratios 2

3 ATLAS Users Meeting Guy Savard, Argonne National Laboratory May 15-16, U 1 GeV/u 238 U + 1 H Armbruster et al.  difficult to reach via fragmentation  cannot be reached via fusion  unique physics, critical to the r-process, which is wide open for a facility able to reach there, even in the FRIB era 3

4 ATLAS Users Meeting Guy Savard, Argonne National Laboratory May 15-16, 2014 Producing neutron-rich N=126 nuclei  Production using deep-inelastic reaction: e.g.: 136 Xe at 9 MeV/u and 5 p  A on a 10 mg/cm Pt rotating target Calculated using GRAZING ( All of these isotopes, except for 204 Pt, are unknown … no mass, lifetime or decay properties known Extracted beam: ~ 15% of production 4

5 ATLAS Users Meeting Guy Savard, Argonne National Laboratory May 15-16, 2014 Collecting the N=126 recoils  Deep inelastic reactions used in the past to produced n-rich isotopes, the products identified in complex setups (Mayer 1985, Corradi 1999, …), but no system has so far been able to collect them efficiently.  But the cross-section are high and with high primary beam intensity and efficient collection efficiency sizable yield in unexplored n-rich regions are reachable  Proposed collection system capitalizes on High primary beam intensity High -intensity gas catcher technology  Feed low-energy systems: mass measurements, decay spectroscopy, … 136 Xe extracted recoils beam dump rotating 198 Pt target to selection stage target-like recoils 5

G. Savard May ATLAS Operation’s Review 6 The CPT-II apparatus and low-energy stations for deep-inelastic reaction products  Designed to push back space charge limit –RFQ ion guide now operating in DC mode to avoid space charge build up –Rough mass separation by in- flight mass separator before isobar separator –Rest of system essentially the same  Can operate at up to 5-50 p  A while still providing required selection before precision Penning trap  Deep inelastic reactions down to ~0.01  b … around 198 Hf on N=126 line Mass separator (  M/M ~ 1/1000) Decay Station

7 ATLAS Users Meeting Guy Savard, Argonne National Laboratory May 15-16, 2014 Status  Main components are being constructed  Production system will be installed in experimental area III in early 2015  CPT moved to this area later in 2015 to start mass measurement program in this region  Low-energy beamline to deliver these beams to various experiments to be stationed temporarily in area III to follow