Aims: Measure B(E2) value (systematics) for 0+ →2+1 and 2+1 →2+2 from the valence maximum (17066Dy104) to the triaxial ‘favoured number at N=116’ Specific.

Slides:

Advertisements

Similar presentations

Precision Determinations of the Transition Quadrupole Moments Approaching the N  N Valence Maximum: Lifetimes of Yrast States in 166,168 Dy An

Advertisements

LYCCA: Lund - York - Cologne - CAlorimeter Status report L U N D U N I V E R S I T YU N I V E R S I T Y Nuclear Structure Group.

LOI for the AGATA-PRESPEC campaign, GSI Spectroscopy and B(E2) measurements in neutron rich Mo nuclei: Search for shape transitions near the astrophysical.

Shell model studies along the N~126 line Zsolt Podolyák.

From Magic 208 Pb to the 170 Dy Mid-Shell Paddy Regan WNSL, Yale University, New Haven, CT and Dept. of Physics, University of Surrey, UK

NPSC-2003Gabriela Popa Microscopic interpretation of the excited K  = 0 +, 2 + bands of deformed nuclei Gabriela Popa Rochester Institute of Technology.

Relativistic Coulomb excitation of nuclei near 100 Sn C.Fahlander, J. Eckman, M. Mineva, D. Rudolph, Dept. Phys., Lund University, Sweden M.G., A.Banu,

Rare ISotope INvestigation at GSI Status of the relativistic beam campaign Introduction Fast beam physics program Experimental methods Status and perspectives.

Examples: Nuclear Decay. Examples Al -> 4 2 He + ________.

The Nature of Molecules

Joint IAEA-ICTP Workshop on Nuclear Reaction Data for Advanced Reactor Technologies Student’s presentation Calculation of correction factors for neutron.

Periodic Table – Filling Order

Workshop on Physics on Nuclei at Extremes, Tokyo Institute of Technology, Institute for Nuclear Research and Nuclear Energy Bulgarian Academy.

Status and needs of activation data for fusion Robin Forrest 1 and Jura Kopecky 2 1 Euratom/UKAEA Fusion Association Culham Science Centre, UK 2 JUKO Research,

N. Saito The RISING stopped beam physics meeting Technical status of RISING at GSI N. Saito - GSI for the RISING collaboration Introduction Detector performance.

Reiner Krücken - Yale University Reiner Krücken Wright Nuclear Structure Laboratory Yale University Why do we measure lifetimes ? The recoil-distance method.

Fast Timing with Diamond Detectors Lianne Scruton.

Coulomb excitation of 127,128 Cd R. Krücken 1, M. Gorska 2, P. Boutachkov 2, A. Dewald 5, R. Gernhäuser 1, A. Jungclaus 4, Th. Kröll 3, D. Mücher 1, F.

Periodic Table Of Elements

High-spin structures in the 159 Lu nucleus Jilin University, China Institute of Atomic Energy 李聪博 The 13th National Nuclear Structure Conference of China.

THE NATIONAL CONTEXT FOR THE CURRICULUM Carrie Ansell and Maureen Lewis From: Learning to Teach in the Primary School 2nd edition, Routledge © 2010 UNIT.

Nuclear Structure studies using fast radioactive beams J. Gerl SNP2008 July Ohio University, Athens Ohio USA –The RISING experiment –Relativistic.

abrasion ablation  σ f [cm 2 ] for projectile fragmentation + fission  luminosity [atoms cm -2 s -1 ]  70% transmission SIS – FRS  ε trans transmission.

Experimental studies of spatial distribution of neutron production around thick lead target irradiated by 0.9 GeV protons Antonín Krása&Vladimír Wagner.

B-1 Fragmentation – 0 Introduction Generalities Isotopic distributions Neck emission Participant-spectator model Fragment separators LISE of GANIL FRS.

Lund Lund York Cologne Calorimeter present status test results with Thanks to Andreas Wendt !!

Rare Isotope Spectroscopic INvestigation at GSI. abrasion ablation  σ f [cm 2 ] for projectile fragmentation + fission  luminosity [atoms cm -2 s -1.

E. Sahin, G. de Angelis Breaking of the Isospin Symmetry and CED in the A  70 mass region: the T z =-1 70 Kr.

CULTURAL FOOTPRINT PT09 – Cultural Diversity and Cultural Exchange PORTUGAL Arts Council Portugal (DGArtes) Overview of the programmes in PA17, EEA Grants.

FAIR (Facility for Antiproton and Ion Research) (Darmstadt, Germany) low-energy cave MeV/u fragmentation/fission ~1GeV/u fragment separator 350m.

Nuclear Spectrcosopy in Exotic Nuclei Paddy Regan Dept,. Of Physics University of Surrey, Guildford, UK

Moumita Maiti, Kaustab Ghosh, T.M. Mendonça, Thierry Stora, Susanta Lahiri Primary result on RaBIT irradiations of LBE targets at CERN-ISOLDE.

Neutron Capture Cross Sections from 1 MeV to 2 MeV by Activation Measurements Korea Institutes of Geoscience and Mineral Resource G.D.Kim, T.K.Yang, Y.S.Kim,

BLIP Operations – 162 days of operation o Safety o Forklift needs a new tire o Production o Sr-82 targets out of beam as of 14 Jun o New Sr-82 targets.

César Domingo Pardo GSI Helmholtzzentrum für Schwerionenforschung GmbH Status of and Expected Performance AGATA ISTANBUL WORKSHOP

Bentley et al - Istanbul May 7th Letter of Intent: Letter of Intent: Isospin Symmetry and Transition Rates in Isobaric Multiplets M.A.Bentley,

R.Burcu Cakirli*, L. Amon, G. Audi, D. Beck, K. Blaum, Ch. Böhm, Ch. Borgmann, M. Breitenfeldt, R.F. Casten, S. George, F. Herfurth, A. Herlert, M. Kowalska,

E0 DECAY OF THE LEVELS IN 156 DY AND 160 ER G. Lo Bianco, S. Nardelli, S. Das Gupta, D.L. Balabanski, N. Blasi, K. Gladnishki, A. Saltarelli, L.

Summary of LOIs to INTC (24 June 2010). Call for Letters of Intent (deadline May 21) 34 Letters submitted 284 Participants from 76 Laboratories in 22.

ISIS OPTIMVS NEVTRONVM SPALLATIONENSIVM FONS MVNDI ISIS Developments David Findlay Accelerator Division ISIS Department Rutherford Appleton Laboratory.

Validation of GEANT4 versus EGSnrc Yann PERROT LPC, CNRS/IN2P3

Daniel Bloor & The AGATA Collaboration IoP NPPD Conference, University of Glasgow, 05/04/11. Development of a simulation package for fragmentation reactions.

Coulomb excitation of the two proton-hole nucleus 206 Hg CERN-ISOLDE, Geneva, Switzerland (M. Kowalska, E. Rapisarda, T. Stora, F.J.C. Wenander) GSI, Darmstadt,

Nuclear Physics LOS ALAMOS NATIONAL LABORATORY 1 Line B preparations Hardware issues Install Fast Kicker (up to 200  C/sec). Reinstall Line B transport.

Electron Configuration

1 H 2 He 3 Li 4 Be 5 B 6 C 7 N 8 O 9 F 10 Ne 11 Na 12 Mg 13 Al 14 Si

Chemeketa Community College

Periodensystem Biomaterials Research - Manfred Maitz H He Li Be B C N

Emission of Energy by Atoms and Electron Configurations

Trends of the Periodic Table

WHAT THE HECK DO I NEED TO BE ABLE TO DO?

Periodic Table of the Elements

ТАБЛИЦА Б. Е. ЛИПОВА «STRUCTURE OF ATOMIC NUCLEUS”

Isospin Symmetry test on the semimagic 44Cr

Starter – Name 10 “High End” British made products

Russian Research Center “ Kurchatov Institute”

!'!!. = pt >pt > \ ___,..___,..

Rare Isotope Spectroscopic INvestigation at GSI

Electron Configurations

ISIS OPTIMVS NEVTRONVM SPALLATIONENSIVM FONS MVNDI

DETECTION LIMITS < 1 ppt ng/L 1-10 ppt ng/L ppt ng/L

Liverpool Tutoring for Primary School. If you're searching for a K to 12 maths or English tutor in Liverpool, check out au.

Simulations of the AGATA Response to Relativistic Heavy Ions Beams

LAHET code simulations in comparison with bare Pb spallation target experiment Daniela Henzlova.

Rare Isotope Spectroscopic INvestigation at GSI

Electron Configurations and the Periodic Table

108Sn studied with intermediate-energy Coulomb excitation

Rare Isotope Spectroscopic INvestigation at GSI

7 pt 7 pt 7 pt 7 pt 7 pt 14 pt 14 pt 14 pt 14 pt 14 pt 21 pt 21 pt

Presentation transcript:

Aims: Measure B(E2) value (systematics) for 0+ →2+1 and 2+1 →2+2 from the valence maximum (17066Dy104) to the triaxial ‘favoured number at N=116’ Specific cases: B(E2:0+ →2+) 164,166,168,170Dy (Eg ~ 80 keV) B(E2:0+ →2+) 176,178,180Yb (Eg ~80 keV) B(E2: 0+ →2+1) 186,188,190,192W (Eg =100,144,207,218 keV) B(E2: 0+ →2+1) 192,194,196Os (Eg =206, 219, 300 keV)

The current ‘state of the art’

Fast RISING with CATE (to be replaced with AGATA D + LYCCA) 152Sm primary beam (750 MeV/A) Coulex on a 0.4 g/cm2 197Au target:

Dy using a 176Yb primary beam Yb using a 186W primary beam W using a 197Au or 198Pt beam Os using a 197Au or 198Pt beam