JYFL Accelerator Laboratory
|
|
- Caroline Benson
- 5 years ago
- Views:
Transcription
1 JYFL Accelerator Laboratory Four accelerators serving international users for basic research, applications and commerical services: K130 heavy ion cyclotron (+ three ECR ion sources and light ion source) (1992) 1.7 MV Pelletron for ion beam analysis and modification of materials (2007) MCC30 light ion cyclotron (2012) Electron LINAC (2015) Contact information:
2 r e u na vi v a 2 0 dip li o n m u a n k a a se te t t una r e n v u a iv a K1 30 yo ke n m uk a n a s e t et tu na Accelerator laboratory Pelletron Commercial applications Medical Reactions ECR MARA RITU *RADEF -Space -Microfilters -CLinac BB2 QB7 K=130 MeV Medical K=30 MeV IGISOL m *RADiation Effects Facility
3 K130 Accelerated elements: p Xe E = Q 2 /A 130 MeV Ion sources: 6.4 GHz ECRIS 14 GHz ECRIS Multicusp (H -, D - ) Upgrade: 18 GHz ECR
4 Operation of K : 6135 h 2016: 5650
5 K130 beam database
6 New 18 GHz ECRIS (HIISI) Motivation: 1. Nuclear physics experiments, especially studies of superheavy elements, would benefit from higher intensities at medium charge states, such as Ar 8+ and Xe 26+ (energy > 5 MeV/u). 2. European space industry and radiation effects community need higher-energy, higher-intensity beams in the future. The ion beam cocktail energy should be increased from present 9.3 MeV/u to about 15 MeV/u. deeper penetration in silicon irradiations in air with possibility to tilt Infrastructure funding (Academy of Finland) + ESA financial support.
7 RADEF, Jyväskylä, Finland New 18 GHz Ion Source HIISI and 16.2 MeV/u heavy ion cocktail Present: The 9.3 MeV/u cocktail used at JYFL. Species marked with have m/q 3.3 and all others m/q 3.7 Autumn 2017: The 12.5 MeV/u, m/q = 3.2 cocktail proposed to be used at JYFL with 24 segment magnets. Spring 2018: The 16.2 MeV/u, m/q = 2.8 cocktail proposed to be used at JYFL with 36 segment magnets In addition, 10 MeV/u 179 Au 54+, LET 94 MeV cm 2 /mg at Bragg peak (@50µm), Full Range 98 µm (SRIM2013)
8 New 18 GHz ECRIS (HIISI) 5000 Argon intensities 500 Quick test: Xe ma Xe ma Intensity [µa] 50 JYFL 14 GHz ECRIS at 1 kw HIISI ( GHz) at 2.3 kw GTS (18+14 GHz) at 2.6 kw VENUS ( GHz) at 4-9 kw Charge state
9 RADEF, Jyväskylä, Finland Proton beams from 0.5 to 52 MeV - Proton beams from 8 to 52 MeV in air - Energy changes with Al-degraders or from cyclotron - Fluxes from 1E3 to 3e8 protons/cm 2 /s - Low energy protons from 0.5 to 8 MeV in vacuum - Energy change using degrader foil and 90 degree dipole magnet - Good energy resolution of the beam (~30 kev FWHM) - Max fluxes depending on energy: 0.5 MeV ~5e5 protons/cm 2 /s 1.0 MeV ~8e6 protons/cm 2 /s 2.0 MeV ~8e7 protons/cm 2 /s
10 RADEF, Jyväskylä, Finland High energy electron accelerator, LINAC - Model: VARIAN clinac 2100 cd - Electron and photon beams - Electron energies: 6, 9, 12, 16 and 20 MeV - Dose rates at maximum in water: 100, 200, 300, 400, 500, 600 and 1000 rad/min - Photons: 6 and 15 MV Bremsstrahlung radiation - Dose rates at maximum in water: 100, 200, 300, 400, 500 and 600 rad/min - Maximum beam size in isocentric point 30x30 cm 2 - Heavily pulsed beam: 1/1000
11 JYFL-PAC Proposal submission: Two deadlines per year: 15 March and 15 September PAC roughly 4 weeks later Decision based on written proposal, no presentations. One dedicated refereee / proposal Voting + discussion PAC members are encouraged to contact spokespersons before the PAC meeting Proposal lifetime 2 years Commercial use not dealt in the PAC (20-25% of all beam time at K130) Program Advisory Committee: Michael Bender, Bordeax, France Jon Billowes, Manchester, UK Bertram Blank, Bordeaux, France (chair) Bo Cederwall, Stockholm, Sweden Fadi Ibrahim, Orsay, France Silvia Lenzi, Padova, Italy + Mikael Sandzelius, Scientific Secretary + Paul Greenlees, JYFL + Ari Jokinen, JYFL Last PAC October 2017
12 PAC on statistics Requested days 2833 Given days 2026 Success rate 71,5% No of proposals 389 Average number of proposals 17 Average number of pending days 383 (today 372 days) The next PAC (Proposal deadline ) 16 proposals: 4 IGISOL 2 reaction studies 1 applied 9 Ritu/gamma/Mara All in all 169 days requested
13 Supported experiments: Code Title of the experiment I195 Laser spectroscopy of scandium isotopes across N=28 I208 The spin, parity and mass of 102 Y and 102m Y I209 I210 I211 The 82 Br/ 82 Se mass difference and solar neutrinos (Project: A=82) New high sensitivity laser spectroscopy at IGISOL-4 Laser spectroscopy of tantalum using optical pumping in an ion cooler-buncher I212 Trap-assisted beta-decay spectroscopy of the very neutron-rich elements around mass A=88 I220 I221 I223 J22 J24 JR134 JR139 JR143 Mass measurements in the vicinity of 78 Ni to constraint core-collapse supernovae models and to study the N=50 and Z=78 shell closures evolution towards the neutron dripline Quantum-state Selective Decay Spectroscopy: Evolution of the 11/2- neutron-hole state along odd-a Cd isotopes (N=77-81) Beta decay spectroscopy of very neutron-deficient nuclei around mass A=110 using JYFLTRAP Towards a more precise measurement of the Q(2+) in 12 C: testing state-of-the-art ab initio theories Lifetime measurements of low-lying states in midshell Te isotopes Resubmission of the experiment JR120: In-beam γ-ray spectroscopy of 184 Pb addendum to proposal JR13 Lifetime measurements of excited states in 163 W89 and 164 W90 Recoil-Decay Tagged RDDS study of extremely neutron deficient Ir-Pt-Au nuclei and Spectroscopy of 171,172 Au First 18 months: 22 exp. supported 84 users supported 9014 hrs beam on target 4632 supported hours (51,4 %) T&S support 77 k (estimated 80 k ) JR144 JR145 JR147 JR148 NRO127 Is 188 Po Prolate Deformed? Onset of deformation in light Ra isotopes Ra Where is the i13/2 orbital in 159 Hf and 155 Yb? Manifestation of triaxiality in 135,136 Nd: chirality and wobbling motion Study of the ternary decay channel induced by shell effects via the reactions 34 S+ 208 Pb and 37 Cl+ 205 Tl S13 S19 S20 Study of high-k states in 254 No using the SAGE spectrometer Spectroscopy of the odd-proton nucleus 249 Md Search for Isomeric States in 250 Fm
14 34 S Bi
15 UNIVERSITY OF JYVÄSKYLÄ Renewal in Nuclear Spectroscopy MARA and JUROGAM3 Opens a new region of nuclear chart for study Probe different aspects of nucleon-nucleon interaction Flexibility in switching experimental set-up
16 UNIVERSITY OF JYVÄSKYLÄ New frontiers in mass measurements with FIRI-funded instruments MR-TOF AT JYFLTRAP (TEAM 1) AND MARA-LEB (TEAMS 1-3) Fast method shorter-lived nuclei! MASSES Wolf et al., Int. J. Mass. Spectrom. 349 (2013) 123 PURIFICATION PI-ICR MASS MEASUREMENT TECHNIQUE AT JYFLTRAP (TEAM 1) = To be commissioned at JYFLTRAP in 2017 = + = 2 40 times better resolution Shorter excitation times Requires fewer ions Eliseev et al., Phys. Rev. Lett. 110 (2013)
17 JYVÄSKYLÄN YLIOPISTO Phase dependent cleaning Isomerically clean beams available with unprecedented resolving power Shown: maximal 180 degree separation Scale this: For A/q = 100, 50 kev isomer 45 deg phase difference Need 200 ms 250 ms 2 10 Ultimately: few 10 kev separation possible g.s. of 127 Cd delivered to TASISPEC
18 Proof of principle in JYFL ) Laser polarization 2) First D measurement LPCTrap setup Ion cooler and buncher Penning trap MR ToF MS beam Pulse down electrodes LPCTrap IGISOL 4 : I. D. Moore et al., Nucl. Instrum. Meth. B, 317(2013)208 10/10/2017 INPC 2016, Adelaide
19 UNIVERSITY OF JYVÄSKYLÄ Archiving percentages in 2015 and ,00% 70,00% 60,00% EU goal in % 50,00% 40,00% 30,00% 20,00% 10,00% 0,00% JYX open access repository Jyväskylä University Digital Archive
20
21
22 Thank you for your attention!
Overview of JYFL TA Activities in ENSAR2
Overview of JYFL TA Activities in ENSAR2 Ari Jokinen ENSAR2 TOWN MEETING April 2018 JYU. Since 1863. 17.4.2018 1 r e u na vi v a 2 0 dip li o n m u a n k a a se te t t una r e n v u a iv a K1 30 yo ke
More informationLaser Spectroscopy on Bunched Radioactive Ion Beams
Laser Spectroscopy on Bunched Radioactive Ion Beams Jon Billowes University of Manchester Balkan School on Nuclear Physics, Bodrum 2004 Lecture 1. 1.1 Nuclear moments 1.2 Hyperfine interaction in free
More informationStatus & Future for In-Beam Spectrometers for Tagging at JYFL
Status & Future for In-Beam Spectrometers for Tagging at JYFL Department of Physics, Finland Task 1 - Improvement of RDT method (Jyväskylä) Extend the method from α-decay tagging to β-γ tagging, for the
More informationFrom simulations to an operating cyclotron The story of the K130 cyclotron
From simulations to an operating cyclotron The story of the K130 cyclotron Pauli Heikkinen University of Jyväskylä Finland Uppsala 23 25 May, 2018 Pre-historical time MC20 from SCX (1974-1991) Proposal
More informationRITU and the GREAT Spectrometer
RITU and the GREAT Spectrometer Cath Scholey Department of Physics University of Jyväskylä 19 th March 2006 3rd TASCA Detector Group Meeting, GSI Darmstadt C. Scholey (JYFL, Finland) RITU and the GREAT
More informationMEASUREMENTS FOR THE R PROCESS AT IGISOL. Anu Kankainen University of Jyväskylä
MEASUREMENTS FOR THE R PROCESS AT IGISOL Anu Kankainen University of Jyväskylä Ion-Guide Isotope Separator On-Line (IGISOL) MCC-30 K-130 Offline ion source Mass number A Light ion ion guide RFQ Cooler
More informationPursuing mass resolving power of 10 6 : Commissioning of IGISOL 4
Pursuing mass resolving power of 10 6 : Commissioning of IGISOL 4 H. Penttilä JYFL University of Jyväskylä Finland & IGISOL group Special thanks to I.D. Moore and D.Gorelov JYFL JYFL = Jyväskylän Yliopiston
More informationLaser spectroscopy and resonant laser ionization atomic tools to probe the nuclear landscape. Iain Moore University of Jyväskylä, Finland
Laser spectroscopy and resonant laser ionization atomic tools to probe the nuclear landscape Iain Moore University of Jyväskylä, Finland Nordic Conference on Nuclear Physics 2011 Outline Introduction to
More informationFISSION YIELD MEASUREMENTS WITH JYFLTRAP
FISSION YIELD MEASUREMENTS WITH JYFLTRAP Heikki Penttilä The IGISOL group University of Jyväskylä, Finland Quick orientation Jyväskylä JYFLTRAP JYFL accelerator laboratory Me Spectrscopy line IGISOL-4
More informationLaser spectroscopy of actinides at the IGISOL facility, JYFL. Iain Moore University of Jyväskylä, Finland
Laser spectroscopy of actinides at the IGISOL facility, JYFL Iain Moore University of Jyväskylä, Finland Outline Motivation for heavy element studies Laser ionization and spectroscopy of plutonium Comparison
More informationCollinear laser spectroscopy of radioactive isotopes at IGISOL 4 Liam Vormawah
Collinear laser spectroscopy of radioactive isotopes at IGISOL 4 Liam Vormawah University of Liverpool Introduction Collinear laser spectroscopy Nuclear properties from hyperfine structures Isotope shifts
More informationMass measurements of n-rich nuclei with A~70-150
Mass measurements of n-rich nuclei with A~70-150 Juha Äystö Helsinki Institute of Physics, Helsinki, Finland in collaboration with: T. Eronen, A. Jokinen, A. Kankainen & IGISOL Coll. with theory support
More informationDecay studies of 170,171 Au, Hg, and 176 Tl
PHYSICAL REVIEW C 69, 054323 (2004) Decay studies of 170,171 Au, 171 173 Hg, and 176 Tl H. Kettunen, T. Enqvist, T. Grahn, P. T. Greenlees, P. Jones, R. Julin, S. Juutinen, A. Keenan, P. Kuusiniemi, M.
More informationIon Beam Cocktail Development and ECR Ion Source Plasma Physics Experiments at JYFL
Ion Beam Cocktail Development and ECR Ion Source Plasma Physics Experiments at JYFL Olli Tarvainen 11th International Conference on Heavy Ion Accelerator Technology Venice, Italy 8-12 June 29 Outline JYFL
More informationNuclear Structure Studies with Penning Traps
ASRC Workshop Tokai 2014 Nuclear Structure Studies with Penning Traps Michael Block Unique Combination for SHE Studies ECR/PIG + UNILAC Stable targets SHIP SHIPTRAP Beam TRIGA- Actinide targets TASCA TASISpec
More informationOpportunities with collinear laser spectroscopy at DESIR:
Opportunities with collinear laser spectroscopy at DESIR: the LUMIERE facility GOALS of LUMIERE experiments: Gerda Neyens, K.U. Leuven, Belgium (1) measure ground state properties of exotic isotopes: (see
More informationIntroduction to REX-ISOLDE concept and overview of (future) European projects
Introduction to REX-ISOLDE concept and overview of (future) European projects Thanks to: Y. Blumenfeld, P. Butler, M. Huyse, M. Lindroos, K. Riisager, P. Van Duppen Energetic Radioactive Beam Facilities
More informationThis is an electronic reprint of the original article. This reprint may differ from the original in pagination and typographic detail.
This is an electronic reprint of the original article. This reprint may differ from the original in pagination and typographic detail. Author(s): Canete, Laetitia; Eronen, Tommi; Jokinen, Ari; Kankainen,
More informationAndree Welker ENSAR2 Town Meeting Groningen
Exploration of the nuclear mass surface one proton above the potentially doubly-magic nuclide 78 Ni and the commissioning of the Phase-Imaging Ion-Cyclotron-Resonance technique at ISOLTRAP Andree Welker
More informationIn-trap decay and trap-assisted decay spectroscopy at ISOLTRAP
In-trap decay and trap-assisted decay spectroscopy at ISOLTRAP ISOLTRAP experimental setup In-trap decay: principle application for mass measurements Trap-assisted decay spectroscopy: principle and purpose
More informationHEIDI WATKINS. Plunger Measurements of Shape Coexistence in the Neutron Deficient 174 Pt Nuclei
Plunger Measurements of Shape Coexistence in the Neutron Deficient 174 Pt Nuclei HEIDI WATKINS 2009 IoP NUCLEAR PHYSICS CONFERENCE UNIVERSITY OF BIRMINGHAM OVERVIEW Physics Motivation. Shape Coexistence
More informationPrecision Nuclear Mass Measurements Matthew Redshaw Exotic Beam Summer School, Florida State University Aug 7 th 2015
Precision Nuclear Mass Measurements Matthew Redshaw Exotic Beam Summer School, Florida State University Aug 7 th 2015 Outline WHAT are we measuring? - Nuclear/atomic masses WHY do we need/want to measure
More informationThe SPIRAL2 Project and experiments with high-intensity rare isotope beams
The SPIRAL2 Project and experiments with high-intensity rare isotope beams Marek Lewitowicz GANIL, CEA/DSM-CNRS/IN2P3, BP 55027, 14076 Caen Cedex, France Lewitowicz@ganil.fr Abstract. The SPIRAL2 facility
More informationPhotofission of 238-U Nuclei
Photofission of 238-U Nuclei International Thorium Energy Conference - ThEC18, 29-31st of October 2018, Belgium İsmail Boztosun This research has been supported by TÜBİTAK with grant number 114F220 Motivations
More informationBeams from the Super Separator Spectrometer
Beams from the Super Separator Spectrometer Hervé Savajols GANIL, France on behalf the S 3 Collaborations GANIL/SPIRAL1/SPIRAL2 facility GANIL/SPIRAL 1 today DESIR Facility low energy RIB S3 separatorspectrometer
More informationProbing neutron-rich isotopes around doubly closed-shell 132 Sn and doubly mid-shell 170 Dy by combined β-γ and isomer spectroscopy.
Probing neutron-rich isotopes around doubly closed-shell 132 Sn and doubly mid-shell 170 Dy by combined β-γ and isomer spectroscopy Hiroshi Watanabe Outline Prospects for decay spectroscopy of neutron-rich
More informationNuclear and Radiation Physics
501503742 Nuclear and Radiation Physics Why nuclear physics? Why radiation physics? Why in Jordan? Interdisciplinary. Applied? 1 Subjects to be covered Nuclear properties. Nuclear forces. Nuclear matter.
More informationBertram Blank CEN Bordeaux-Gradignan. Germanium detector calibration experimental studies: b decay mirror b decay future work
Bertram Blank CEN Bordeaux-Gradignan Germanium detector calibration experimental studies: 0 + - 0 + b decay mirror b decay future work Beta-Decay Weak Interaction Studies in the Era of the LHC International
More informationNuclear physics: Magdalena Kowalska CERN, PH Dept.
Nuclear physics: the ISOLDE facility Magdalena Kowalska CERN, PH Dept on behalf of the CERN ISOLDE team www.cern.ch/isolde Outline Forces inside atomic nuclei Nuclei and QCD, nuclear models Nuclear landscape
More informationNuclear Masses and their Importance for Nuclear Structure, Astrophysics and Fundamental Physics
Winter Meeting on Nuclear Physics, Bormio, Italy 2014 Nuclear Masses and their Importance for Nuclear Structure, Astrophysics and Fundamental Physics Klaus Blaum Jan 27, 2014 Klaus.blaum@mpi-hd.mpg.de
More informationConversion Electron Spectroscopy in Transfermium Nuclei
Conversion Electron Spectroscopy in Transfermium Nuclei R.-D. Herzberg University of iverpool, iverpool, 69 7ZE, UK Abstract Conversion electron spectroscopy is an essential tool for the spectroscopy of
More informationCapabilities at the National Superconducting Cyclotron Laboratory. Sean Liddick NDNCA workshop, May 26-29, 2015
Capabilities at the National Superconducting Cyclotron Laboratory Sean Liddick NDNCA workshop, May 26-29, 2015 NSCL and FRIB Laboratory NSCL is funded by the U.S. National Science Foundation to operate
More informationErice, September, 2017,
Erice, September, 2017, Double beta (bb) decay neutrinoless double beta (0nbb) decay NME the specialties of 96 Zr/ 96 Nb for b and bb decay Mass measurements using the JYFLTRAP ion trap Results and the
More informationBertram Blank CEN Bordeaux-Gradignan. Germanium detector calibration experimental studies: decay mirror decay future work
Bertram Blank CEN Bordeaux-Gradignan Germanium detector calibration experimental studies: 0 + -0 + decay mirror decay future work 20 th Colloque de GANIL, Amboise, October 15th 20th, 2017 Nuclear beta
More informationAccelerated radioactive beams and the future of nuclear physics. David Jenkins
Accelerated radioactive beams and the future of nuclear physics David Jenkins Particle accelerators 1930s: Cockcroft and Walton 1990s: Superconducting niobium cavities Energetic Radioactive Beam Facilities
More informationPrecision mass measurements of radioactive nuclei at JYFLTRAP
EPJ manuscript No. (will be inserted by the editor) Precision mass measurements of radioactive nuclei at JYFLTRAP S. Rahaman a, V.-V. Elomaa, T. Eronen, U. Hager, J. Hakala, A. Jokinen, A. Kankainen, I.D.
More informationFAIR. Reiner Krücken for the NUSTAR collaboration
NUSTAR @ FAIR Reiner Krücken for the NUSTAR collaboration Physik Department E12 Technische Universität München & Maier-Leibnitz-Laboratory for Nuclear and Particle Physics NUSTAR @ FAIR Nuclear Structure
More information2007 Fall Nuc Med Physics Lectures
2007 Fall Nuc Med Physics Lectures Tuesdays, 9:30am, NN203 Date Title Lecturer 9/4/07 Introduction to Nuclear Physics RS 9/11/07 Decay of radioactivity RS 9/18/07 Interactions with matter RM 9/25/07 Radiation
More informationReport on Nuclear Spectroscopy at JYFL
Report on on Report Nuclear Spectroscopy Spectroscopy Nuclear at JYFL JYFL at In-beam & Decay Spectroscopy (Daresbury, Liverpool, Manchester, Paisley, Surrey, York) Collinear Laser Spectroscopy (Birmingham,
More informationExploring the Structure of Cold and Warm Nuclei Using Particle Accelerators in India
Exploring the Structure of Cold and Warm Nuclei Using Particle Accelerators in India GOPAL MUKHERJEE VARIABLE ENERGY CYCLOTRON CENTRE, KOLKATA ABSTRACT The Indian National Gamma Array (INGA) and the VECC
More informationThe heavy ion irradiation facility at KVI-CART
The heavy ion irradiation facility at KVI-CART Brian N. Jones 1, Marc-Jan van Goethem 1,2, Rob Kremers 1, Harry Kiewiet 1, Emiel van der Graaf 1, Sytze Brandenburg 1 1 University of Groningen, KVI-Center
More informationTAMU-TRAP facility for Weak Interaction Physics. P.D. Shidling Cyclotron Institute, Texas A&M University
TAMU-TRAP facility for Weak Interaction Physics P.D. Shidling Cyclotron Institute, Texas A&M University Outline of the talk Low energy test of Standard Model T =2 Superallowed transition Facility T-REX
More informationTHE SUPER SEPARATOR SPECTROMETER S 3
THE SUPER SEPARATOR SPECTROMETER S 3 Hervé Savajols (GANIL) LINAC stable beams Very high intensity stable beams over a wide mass range Very high intensity stable beams over a wide mass range 6.10 14 pps
More informationSpin Cut-off Parameter of Nuclear Level Density and Effective Moment of Inertia
Commun. Theor. Phys. (Beijing, China) 43 (005) pp. 709 718 c International Academic Publishers Vol. 43, No. 4, April 15, 005 Spin Cut-off Parameter of Nuclear Level Density and Effective Moment of Inertia
More informationCoulomb excitation experiments at JAEA (Japan Atomic Energy Institute)
Japan Atomic Energy Agency GOSIA work shop 2008/4/8-10 Warsaw, Poland Coulomb excitation experiments at JAEA (Japan Atomic Energy Institute) JAEA, Chiba Inst.Tech. a, Kyusyu Univ. b, Hiroshima Univ. c,
More informationRadioactivity at the limits of nuclear existence
Radioactivity at the limits of nuclear existence Zenon Janas Institute of Experimental Physics University of Warsaw Chart of nuclei - stable - β + - β - - α - fission - p p and 2p radioactivty proton radioactivity
More informationtwo-proton radioactivity discovery of two-proton radioactivity experimental results with TPC s future studies
two-proton radioactivity discovery of two-proton radioactivity experimental results with TPC s future studies Bertram Blank CEN Bordeaux-Gradignan EPS European Nuclear Physics Conference 2009 Spring meeting
More informationECT* Trento The Lead Radius. Precision measurements of nuclear ground state properties for nuclear structure studies. Klaus Blaum
ECT* Trento The Lead Radius Precision measurements of nuclear ground state properties for nuclear structure studies Klaus Blaum 04.08.2009 Outline Introduction, history and methods Principle of laser spectroscopy
More information5 questions, 3 points each, 15 points total possible. 26 Fe Cu Ni Co Pd Ag Ru 101.
Physical Chemistry II Lab CHEM 4644 spring 2017 final exam KEY 5 questions, 3 points each, 15 points total possible h = 6.626 10-34 J s c = 3.00 10 8 m/s 1 GHz = 10 9 s -1. B= h 8π 2 I ν= 1 2 π k μ 6 P
More informationSpectroscopy of 252No to Investigate its K-isomer
Spectroscopy of to Investigate its K-isomer Edward Parr Motivation in Superheavies PROTONS Single Particle Energy (MeV) Single Particle Energy (MeV) NEUTRONS Next shell gaps predicted for Superheavy spherical
More informationSome Beta-Decay Basics. Michael Edmison. Bluffton University
Some Beta-Decay Basics Michael Edmiston Bluffton University The figure at bottom of the page is known as a Segrè Chart. The Segrè Chart is one way to arrange and observe information about nuclei. A Segrè
More informationFrom JYFLTRAP to MATS
From JYFLTRAP to MATS Ari Jokinen Department of Physics, University of Jyväskylä Helsinki Institute of Physics 1) Introduction to trap projects 2) JYFLTRAP at IGISOL 3) JYFLRAP physics program; summary,
More informationLetter of Intent: Nuclear Fusion Reactions from laser-accelerated fissile ion beams
Letter of Intent: Nuclear Fusion Reactions from laser-accelerated fissile ion beams Peter G. Thirolf, LMU Munich D. Habs, H. Ruhl, J. Schreiber, LMU Munich, MPQ Garching T. Dickel, H. Geissel, W. Plass,
More informationICALEPCS Oct. 6-11, 2013
Outline 2 SOHO (ESA & NASA) 3 SOHO (ESA & NASA) 4 SOHO (ESA & NASA) EGRET Team 5 Heavy Ions Charged Ionizing Radiation Outer-Space is full of them Figures reproduced from: 1.Mewaldt, R.A., "Elemental Composition
More informationGANIL / SPIRAL1 / SPIRAL2
Nuclear Structure, Reaction and Dynamics GANIL / SPIRAL1 / SPIRAL2 A huge discovery potential Exotic Nuclei Proton number Z Which force? 3-body, tensor, spin-orbit, Isospin dependence, Continuum coupling
More informationA taste of Proton-rich nuclei. David Jenkins
A taste of Proton-rich nuclei David Jenkins even%a% odd%a%!2%%%%%%%%%%%%%!1%%%%%%%%%%%%%%0%%%%%%%%%%%%%%1%%%%%%%%%%%%%%2%!5/2%%%%%%%%%!3/2%%%%%%%%%!1/2%%%%%%%%%%1/2%%%%%%%%%%3/2%%%%%%%%%%5/2% Isobaric
More informationThe new isotopes 240 Es and 236 Bk
The new isotopes 240 Es and 236 Bk Joonas Konki Department of Physics University of Jyväskylä TASCA 16 The 15th Workshop on Recoil Separator for Superheavy Element Chemistry 26.8.2016 GSI, Darmstadt, Germany
More informationTrap assisted decay spectroscopy setup at ISOLTRAP
Trap assisted decay spectroscopy setup at ISOLTRAP Motivation Penning traps: masses and isobaric selectivity ISOLTRAP mass spectrometer at ISOLDE/CERN Decay spectroscopy at ISOLTRAP: setup and 1 st run
More informationExtreme Light Infrastructure - Nuclear Physics ELI - NP
Extreme Light Infrastructure - Nuclear Physics ELI - NP Nicolae-Victor Zamfir National Institute for Physics and Nuclear Engineering (IFIN-HH) Bucharest-Magurele, Romania www.eli-np.ro Bucharest-Magurele
More informationThe Ring Branch. Nuclear Reactions at. Mass- and Lifetime Measurements. off Exotic Nuclei. Internal Targets. Electron and p. Experiments: Scattering
stochastic cooling Exotic nuclei from Super-FRS Degrader for fast slowing down The Ring Branch TOF Detector MCPs E anode ion B CR Electron cooler NESR secondary electrons Experiments: Mass- and Lifetime
More informationLecture Series: Atomic Physics Tools in Nuclear Physics IV. High-Precision Penning Trap Mass Spectrometry
Euroschool on Physics with Exotic Beams, Mainz 005 Lecture Series: Atomic Physics Tools in Nuclear Physics IV. High-Precision Penning Trap Mass Spectrometry Klaus Blaum Johannes Gutenberg-University Mainz
More informationThis is an electronic reprint of the original article. This reprint may differ from the original in pagination and typographic detail.
This is an electronic reprint of the original article. This reprint may differ from the original in pagination and typographic detail. Author(s): Pomp, Stephan; Mattera, Andrea; Rakopoulos, Vasileios;
More informationThe new operation modes of JYFLTRAP. tio. M ore
The new operation modes of JYFLTRAP M M ore Fa ore be st re am er s! olu... tio n.., V. V. Elomaa, U. Hager, J. Hakala, A. Jokinen, S. Rahaman, J. Rissanen, C. Weber, J. Äystö and the IGISOL group JYFL
More informationRNB at GANIL from SPIRAL to SPIRAL 2
RNB at GANIL from SPIRAL to SPIRAL 2 GANIL/SPIRAL facility Recent highlights Future SPIRAL 2 facility Layout of the facility Scientific opportunities Letters of Intent for SPIRAL 2 See also talks of: Y.
More informationExperimental Initiatives in Nuclear Astrophysics
Experimental Initiatives in Nuclear Astrophysics Carl Brune Astrophysics: H and He burning, S process Facilities: neutron and gamma beams, underground accelerators, ICF plasmas Joint DNP Town Meetings
More informationEstec final presentation days 2018
Estec final presentation days 2018 Background VESPER Facility Conclusion & Outlook Jovian environment Radiation Effects VESPER history VESPER status Overview Experimental Results External Campaign Summary
More informationNuclear Chemistry Notes
Nuclear Chemistry Notes Definitions Nucleons: Subatomic particles in the nucleus : protons and neutrons Radionuclides: Radioactive nuclei. Unstable nuclei that spontaneously emit particles and electromagnetic
More informationISOMER BEAMS. P.M. WALKER Department of Physics, University of Surrey, Guildford GU2 7XH, UK
International Journal of Modern Physics E c World Scientific Publishing Company ISOMER BEAMS P.M. WALKER Department of Physics, University of Surrey, Guildford GU2 7XH, UK p.@surrey.ac.uk Received (received
More information'Nuclear Structure of the Neutron Rich Region around Z=28 towards and beyond N=50' WOG workshop Leuven March 9 11, 2009 Mark Huyse
'Nuclear Structure of the Neutron Rich Region around Z=28 towards and beyond N=50' WOG workshop Leuven March 9 11, 2009 Mark Huyse 7/05/2009 Mark Huyse 1 The program Laser spectroscopy Masses Theory Decay
More informationPhysics with stopped beams at TRIP-TRAP Facility. P.D. Shidling Cyclotron Institute, Texas A&M University
Physics with stopped beams at TRIP-TRAP Facility P.D. Shidling Cyclotron Institute, Texas A&M University Physics with stopped beams Experiments require high purity low energy ions for studying various
More informationObjectives: Atomic Structure: The Basics
Objectives: Atomic Structure: The Basics 1. To be able to sketch an atom and indicate the location of the nucleus, the shells, and the electronic orbitals 2. To be able to calculate the maximum number
More informationNuclear Physics and Astrophysics
Nuclear Physics and Astrophysics PHY-302 Dr. E. Rizvi Lecture 13 - Gamma Radiation Material For This Lecture Gamma decay: Definition Quantum interpretation Uses of gamma spectroscopy 2 Turn to γ decay
More informationQuantum-State Selective Decay Spectroscopy of 213 Ra and 53 Co m
Quantum-State Selective Decay Spectroscopy of 213 Ra and 53 Co m Ch. Lorenz 1, L.G. Sarmiento 1, D. Rudolph 1, C. Fahlander 1, U. Forsberg 1, P. Golubev 1, R. Hoischen 1, N. Lalović 1,2, A. Kankainen 3,
More informationSome nuclei are unstable Become stable by ejecting excess energy and often a particle in the process Types of radiation particle - particle
Radioactivity George Starkschall, Ph.D. Lecture Objectives Identify methods for making radioactive isotopes Recognize the various types of radioactive decay Interpret an energy level diagram for radioactive
More informationDevelopments of the RCNP cyclotron cascade
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,
More informationAddendum to the ISOLDE and Neutron Time-of-Flight Committee
` EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH Addendum to the ISOLDE and Neutron Time-of-Flight Committee IS530: Properties of low-lying intruder states in 34 Al and 34 Si sequentially populated in beta-decay
More informationR. P. Redwine. Bates Linear Accelerator Center Laboratory for Nuclear Science Department of Physics Massachusetts Institute of Technology
Pion Physics in the Meson Factory Era R. P. Redwine Bates Linear Accelerator Center Laboratory for Nuclear Science Department of Physics Massachusetts Institute of Technology Bates Symposium 1 Meson Factories
More informationFission fragment mass distributions via prompt γ -ray spectroscopy
PRAMANA c Indian Academy of Sciences Vol. 85, No. 3 journal of September 2015 physics pp. 379 384 Fission fragment mass distributions via prompt γ -ray spectroscopy L S DANU, D C BISWAS, B K NAYAK and
More informationLawrence Berkeley National Laboratory Lawrence Berkeley National Laboratory
Lawrence Berkeley National Laboratory Lawrence Berkeley National Laboratory Title New ion-guide for the production of beams of neutron-rich nuclei between Z = 20-28 Permalink https://escholarship.org/uc/item/96s4p5pr
More informationNSCL and Physics and Astronomy Department, Michigan State University Joint Institute for Nuclear Astrophysics
National Superconducting Cyclotron Laboratory An overview Ana D. Becerril NSCL and Physics and Astronomy Department, Michigan State University Joint Institute for Nuclear Astrophysics University of North
More informationMagdalena Matejska-Minda HIL, University of Warsaw. NUSPIN 2017, June 2017, GSI
Magdalena Matejska-Minda HIL, University of Warsaw NUSPIN 2017, 26-29 June 2017, GSI AGENDA Why Sc? Overview Experimental setup Gosia analysis Results Summarize and next steps Why Sc? Z=20 Sc N=20 N=28
More informationSpectroscopy of fission fragments using prompt-delayed coincidence technique
PRAMANA c Indian Academy of Sciences Vol. 85, No. journal of September 5 physics pp. 95 Spectroscopy of fission fragments using prompt-delayed coincidence technique RPALIT and S BISWAS Department of Nuclear
More informationHigh-resolution Study of Gamow-Teller Transitions
High-resolution Study of Gamow-Teller Transitions Yoshitaka Fujita, Osaka Univ. @CNS-SS, 04.Aug.17-20 Nucleus : 3 active interactions out of 4 Strong, Weak, EM Comparison of Analogous Transitions High
More informationEXO experiment. Jesse Wodin EXO group Sept 13, DOE Site Visit: Sept 13-14,
EXO experiment Jesse Wodin EXO group Sept 13, 2010 DOE Site Visit: Sept 13-14, 2010 1 EXO program A phased program aimed at building an enriched xenon double beta decay experiment with a one or more tonne
More informationThe Groningen Cyclotron at Demokritos Athens
The Groningen Cyclotron at Demokritos Athens Anastasios Lagoyannis Tandem Accelerator Laboratory N.C.S.R. Demokritos Outline N.C.S.R. Demokritos The Tandem @ I.N.P. P. Basic Infrastructure - Research Interests
More informationQUIZ: Physics of Nuclear Medicine Atomic Structure, Radioactive Decay, Interaction of Ionizing Radiation with Matter
QUIZ: Physics of Nuclear Medicine Atomic Structure, Radioactive Decay, Interaction of Ionizing Radiation with Matter 1. An atomic nucleus contains 39 protons and 50 neutrons. Its mass number (A) is a)
More informationGSI. Overview of last years activities: technical developments and investigations mass measurements. TRAPSPEC related tasks and issues
SHIPTRAP @ GSI Overview of last years activities: technical developments and investigations mass measurements TRAPSPEC related tasks and issues Conclusion and outlook Frank Herfurth for the SHIPTRAP collaboration
More informationOverview. Scientific Case
Overview In the report published by the Nuclear Physics European Community Committee (NuPECC) entitled Radioactive Nuclear Beam Facilities it was stated that the next generation of radioactive ion beam
More informationNew data on β decay of exotic nuclei close to 100 Sn:
New data on β decay of exotic nuclei close to 1 Sn: 94 Ag and 1 In C. Plettner 1, I. Mukha 1, J. Döring 1, L. Batist 2, H. Grawe 1, A. Blazhev 1,3, C. R. Hoffman 4, Z. Janas 5, R. Kirchner 1, M. La Commara
More informationSimple Atom, Extreme Nucleus: Laser Trapping and Probing of He-8. Zheng-Tian Lu Argonne National Laboratory University of Chicago
Simple Atom, Extreme Nucleus: Laser Trapping and Probing of He-8 Zheng-Tian Lu Argonne National Laboratory University of Chicago Funding: DOE, Office of Nuclear Physics Helium Atom fm Å e - Ionization
More informationPROOF/ÉPREUVE ISO INTERNATIONAL STANDARD. Space environment (natural and artificial) Galactic cosmic ray model
INTERNATIONAL STANDARD ISO 15390 First edition 2004-##-## Space environment (natural and artificial) Galactic cosmic ray model Environnement spatial (naturel et artificiel) Modèle de rayonnement cosmique
More informationLaser Ion Acceleration: Status and Perspectives for Fusion
Laser Ion Acceleration: Status and Perspectives for Fusion Peter G. Thirolf, LMU Munich Outline: laser-particle acceleration fission-fusion mechanism: with ultra-dense ion beams towards r-process path
More informationTowards TASCA
TASCA Workshop 2009 Towards SHIPTRAP @ TASCA Michael Block SHIPTRAP Physics Program High-Precision Mass Measurements Trap-Assisted Nuclear Spectroscopy In-Trap Nuclear Spectroscopy Laser Spectroscopy Chemistry?
More informationFirst results from the AGATA Demonstrator. Francesco Recchia Università di Padova
First results from the AGATA Demonstrator Francesco Recchia Università di Padova XCVII Congresso Nazionale SIF L'Aquila, 26-30 Settembre, 2011 Challenges in Nuclear Structure Shell structure in nuclei
More informationLASER SPECTROSCOPIC STUDIES OF NEUTRON-DEFICIENT EUROPIUM AND GADOLINIUM ISOTOPES
LASER SPECTROSCOPIC STUDIES OF NEUTRON-DEFICIENT EUROPIUM AND GADOLINIUM ISOTOPES A.E. Barzakh, D.V. Fedorov, A.M. Ionan, V.S. Ivanov, F.V. Moroz, K.A. Mezilev, S.Yu. Orlov, V.N. Panteleev, Yu.M. Volkov
More informationDSAM lifetime measurements at ReA - from stable Sn to exotic Ca. Hiro IWASAKI (NSCL/MSU)
DSAM lifetime measurements at ReA - from stable to exotic Ca Hiro IWASAKI (NSCL/MSU) 8/20/2015 ReA3 upgrade workshop 1 Evolution of halo properties N=28 pf-shell N>40 gds-shell E0,E? Efimov? 62 Ca? N=8
More informationStatus and perspectives of the GANIL Campaign ACC meeting - Venice
Status and perspectives of the GANIL Campaign 2016 ACC meeting - Venice The GANIL Campaign Charged particles detectors for Coulex and nucleon transfer Post-accelerated RIB from SPIRAL1 Neutron and charged
More informationOblate nuclear shapes and shape coexistence in neutron-deficient rare earth isotopes
Oblate nuclear shapes and shape coexistence in neutron-deficient rare earth isotopes Andreas Görgen Service de Physique Nucléaire CEA Saclay Sunniva Siem Department of Physics University of Oslo 1 Context
More informationLEAP, Kanazawa, Japan 2016
Klaus.blaum@mpi-hd.mpg.de LEAP, Kanazawa, Japan 2016 Precision atomic and nuclear masses and their importance for nuclear structure, astrophysics and fundamental studies Motivation for precision mass data
More informationDeuteron activation cross section measurements at the NPI cyclotron
Nuclear Physics Institute Řež EAF 2011 Deuteron activation cross section measurements at the NPI cyclotron E. Šimečková, P. Bém, M. Honusek, J. Mrázek, M. Štefánik, L. Závorka Nuclear Physics Institute
More information