This project is funded by the NSF through grant PHY0216783, and the Universities of JINA. The Joint Institute for Nuclear Astrophysics Henderson DUSEL.

Slides:



Advertisements
Similar presentations
The 26g Al(p, ) 27 Si Reaction at DRAGON Heather Crawford Simon Fraser University TRIUMF Student Symposium July 27, 2005.
Advertisements

Saed Dababneh. Seventh Symposium on Use of Nuclear Techniques in Environmental Studies. Yarmouk University, JORDAN. 3-5 Sept Manipulated Gamma Spectroscopy:
Hadron physics with GeV photons at SPring-8/LEPS II
Advanced GAmma Tracking Array
Coulomb excitation with radioactive ion beams
GEANT4 Simulations of TIGRESS
Progress on the 40 Ca(α,  ) 44 Ti reaction using DRAGON Chris Ouellet Supervisor: Alan Chen Experiment leader: Christof Vockenhuber ● Background on the.
197 A u at the End of the Dragon Evan O’Connor University of PEI August 2 nd, 2006.
Ion Beam Analysis techniques:
Owned and operated as a joint venture by a consortium of Canadian universities via a contribution through the National Research Council Canada Propriété.
W. Udo Schröder, 2009 Rad. Int. with Matter: Gammas Interaction of Radiation with Matter Gamma Rays 1.
Direct measurement of 4 He( 12 C, 16 O)  reaction near stellar energy Kunihiro FUJITA K. Sagara, T. Teranishi, T. Goto, R. Iwabuchi, S. Matsuda, K. Nakano,
The 12C+12C fusion reaction: a new opportunity at ATLAS Xiaodong Tang 1 & Chenglie Jiang 2 1) Univ. of Notre Dame 2) ANL.
Low energy radioactive beams Carmen Angulo, CRC Louvain-la-Neuve, Belgium FINUPHY meetingLouvain-la-Neuve, Belgium3-4 May 2004 Recent highlights on nuclear.
Studying the  p-process at ATLAS Catherine M. Deibel Joint Institute for Nuclear Astrophysics Michigan State University Physics Division Argonne National.
The AGATA project concept of  - ray tracking design and development Witek Męczyński The Henryk Niewodniczański Institute of Nuclear Physics Polish Academy.
Reaction rates in the Laboratory Example I: 14 N(p,  ) 15 O stable target  can be measured directly: slowest reaction in the CNO cycle  Controls duration.
Status of TACTIC: A detector for nuclear astrophysics Alison Laird University of York.
1 An Introduction to Ion-Optics Series of Five Lectures JINA, University of Notre Dame Sept. 30 – Dec. 9, 2005 Georg P. Berg.
Reaction rates in the Laboratory Example I: 14 N(p,  ) 15 O stable target  can be measured directly: slowest reaction in the CNO cycle  Controls duration.
Reaction rates in the Laboratory Example I: 14 N(p,  ) 15 O stable target  can be measured directly: slowest reaction in the CNO cycle  Controls duration.
AGATA Demonstrator Test With a 252 Cf Source: Neutron-Gamma Discrimination Menekşe ŞENYİĞİT.
Superheavy Element Studies Sub-task members: Paul GreenleesJyväskylä Rodi Herzberg, Peter Butler, RDPLiverpool Christophe TheisenCEA Saclay Fritz HessbergerGSI.
30 Ge & Si Crystals Arranged in verticals stacks of 6 called “towers” Shielding composed of lead, poly, and a muon veto not described. 7.6 cm diameter.
Astrophysics with DRAGON: The 26g Al (p,γ) 27 Si Reaction Heather Crawford a,1 for the DRAGON Collaboration b a Simon Fraser University, Burnaby, B.C.,
I NSTITUTE FOR S TRUCTURE AND N UCLEAR A STROPHYSICS N UCLEAR S CIENCE L ABORATORY Research:Stellar Burning – nuclear reactions with stable beams Explosive.
Stuttgart Dynamitron at Bucharest - Perspectives and New Activities
Direct measurement of 12 C + 4 He fusion cross section at Ecm=1.5MeV at KUTL H.Yamaguchi K. Sagara, K. Fujita, T. Teranishi, M. taniguchi, S.Liu, S. Matsua,
Background Subtraction in Next Generation 0  Experiments Double-Beta Decay Challenges in 0  Decay Detection Small 0νββ decay half-life leads to low.
Abstract The 13 N(p,γ) 14 O reaction is very important for our understanding of explosive astrophysical sites, such as novae and supernovae. This reaction.
Cross section measurements at LNL M.Mezzetto (INFN-Pd) on behalf of INFN-LNL: M. Cinausero, G. De Angelis,G. Prete.
Recoil Separator Techniques J.C. Blackmon, Physics Division, ORNL RMS - ORNL WF QT QD Q D Target FP ERNA - Bochum WF Target D QT FP DRS ORNL QD VF D VAMOS.
New methods to measure the cross sections of 12 C+ 12 C fusion reaction Xiao Fang Department of Physics University of Notre Dame.
Nuclear Astrophysics with the PJ Woods, University of Edinburgh.
Study of the 40 Ca(  ) 44 Ti reaction at stellar temperatures with DRAGON Christof Vockenhuber for the DRAGON collaboration Vancouver, B.C., Canada.
Setup for hypernuclear gamma-ray spectroscopy at J-PARC K.Shirotori Tohoku Univ. Japan for the Hyperball-J collaboration J-PARC E13 hypernuclear  -ray.
M2 NPAC – Laboratory CEA Saclay Stefano PANEBIANCO – Neutron-gamma discrimination.
abrasion ablation  σ f [cm 2 ] for projectile fragmentation + fission  luminosity [atoms cm -2 s -1 ]  70% transmission SIS – FRS  ε trans transmission.
Neutron scattering systems for calibration of dark matter search and low-energy neutrino detectors A.Bondar, A.Buzulutskov, A.Burdakov, E.Grishnjaev, A.Dolgov,
Digital analysis of scintillator pulses generated by high-energy neutrons. Jan Novák, Mitja Majerle, Pavel Bém, Z. Matěj 1, František Cvachovec 2, 1 Faculty.
I NSTITUTE FOR S TRUCTURE AND N UCLEAR A STROPHYSICS N UCLEAR S CIENCE L ABORATORY CASPAR An underground Accelerator Laboratory for Nuclear Astrophysics.
Ultra-low background HPGe detector at ChyeongPyung Underground Laboratory TaeYeon Kim and KIMS(Korea Invisible Mass Search) Collaboration. * Contents *
 -capture measurements with the Recoil-Separator ERNA Frank Strieder Institut für Physik mit Ionenstrahlen Ruhr-Universität Bochum HRIBF Workshop – Nuclear.
Interaction of Radiation with Matter Gamma Rays
A Study of Background Particles for the Implementation of a Neutron Veto into SuperCDMS Johanna-Laina Fischer 1, Dr. Lauren Hsu 2 1 Physics and Space Sciences.
Experimental Nuclear Physics Some Recent Activities 1.Development of a detector for low-energy neutrons a. Hardware -- A Novel Design Idea b. Measure the.
R&D on complementary detectors and devices for nuclear structure and reaction mechanism studies R&D on complementary detectors and devices for nuclear.
Study of unbound 19 Ne states via the proton transfer reaction 2 H( 18 F,  + 15 O)n HRIBF Workshop – Nuclear Measurements for Astrophysics C.R. Brune,
ALNA- Accelerator Laboratory for Nuclear Astrophysics Underground Heide Costantini University of Notre Dame, IN, USA INFN, Genova, Italy.
Physics Colloquium Ⅱ Shibata Laboratory OKA, Hiroki Nucleosyntheses studied with a Van de Graaff Accelerator [Contents] 1. Objective.
KPS Chonbuk University 2005/10/22 HYUNSU LEE Status of the KIMS dark matter search experiment with CsI(Tl) crystals Hyun Su Lee Seoul National.
Institute for Structure and Nuclear Astrophysics Nuclear Science Laboratory E381: Search of potential resonances in the 12 C+ 12 C fusion reaction using.
ERNA: Measurement and R-Matrix analysis of 12 C(  ) 16 O Daniel Schürmann University of Notre Dame Workshop on R-Matrix and Nuclear Reactions in Stellar.
Nuclear Astrophysics ARUNA Workshop, Notre Dame, IN Carl R. Brune Ohio University, Athens Ohio June 12-13, 2014.
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,
Background Subtraction in Next Generation 0  Experiments Double-Beta Decay Challenges in 0  Decay Detection Benjamin Spaun Whitworth College Advisors:
J-PARC でのハイパー核ガンマ線分光実験用 散乱粒子磁気スペクトロメータ検出器の準備 状況 東北大理, 岐阜大教 A, KEK B 白鳥昂太郎, 田村裕和, 鵜養美冬 A, 石元茂 B, 大谷友和, 小池武志, 佐藤美沙子, 千賀信幸, 細見健二, 馬越, 三輪浩司, 山本剛史, 他 Hyperball-J.
Master thesis 2006 Shirotori1 Hypernuclear gamma-ray spectroscopy at J-PARC K1.8 beam line 東北大学大学院理学研究科 原子核物理 白鳥昂太郎.
DARK MATTER SEARCH Carter Hall, University of Maryland.
J-PARC における 4  He の生成と構造の研究 東北大学 大学院理学研究科 白鳥昂太郎 for the Hyperball-J Collaboration.
Breakout from the CNO Cycle Joachim Görres University of Notre Dame And Joint Institute for Nuclear Astrophysics
Jun Chen Department of Physics and Astronomy, McMaster University, Canada For the McMaster-NSCL and McMaster-CNS collaborations (5.945, 3+ : **) (5.914,
Advanced Gamma Tracking Array Andy Boston The Advanced Gamma Tracking Array
 -capture measurements with a Recoil-Separator Frank Strieder Institut für Physik mit Ionenstrahlen Ruhr-Universität Bochum Int. Workshop on Gross Properties.
WIMPs Direct Search with Dual Light-emitting Crystals Xilei Sun IHEP International Symposium on Neutrino Physics and Beyond
Fast neutron flux measurement in CJPL
Triangle Universities Nuclear Laboratory
1. Introduction Secondary Heavy charged particle (fragment) production
Ch. THEISEN – CEA Saclay MUSETT: the segmented Si array for the focal plane of the VAMOS spectrometer Ch. THEISEN – CEA Saclay.
Triangle Universities Nuclear Laboratory
Presentation transcript:

This project is funded by the NSF through grant PHY , and the Universities of JINA. The Joint Institute for Nuclear Astrophysics Henderson DUSEL Capstone Workshop A Recoil Separator for ALNA-Phase2 Manoël Couder University of Notre Dame Joint Institute for Nuclear Astrophysics

This project is funded by the NSF through grant PHY , and the Universities of JINA. The Joint Institute for Nuclear Astrophysics Henderson DUSEL Capstone Workshop Charged particles cross section measurements at low energy Effort to extract the signal at low energy are needed because cross section drops exponentially  Increase the number of interactions Beam intensity increased Gas target are more and more elaborated  Improved detection techniques Gamma detector: 4  segmented Active shielding

Tracking Arrays based on Position Sensitive Ge Detectors Large Gamma Arrays based on Compton Suppressed Spectrometers   40 — 20 % ( M  =1 — M  =30)   10 — 5 % ( M  =1 — M  =30) GAMMASPHEREEUROBALLGRETAAGATA Slide from: J. Simpson, “The AGATA project”, NPDC19, 2005

This project is funded by the NSF through grant PHY , and the Universities of JINA. The Joint Institute for Nuclear Astrophysics Henderson DUSEL Capstone Workshop Charge particles Cross section measurements at low energy – Status Effort to extract the signal at low energy (fight against background) are needed because cross section drops exponentially:  Increase the number of interactions Beam intensity increased Gas target are more and more elaborated  Try to extract more by improving detection techniques Gamma detector: 4  segmented Active shielding  Underground laboratory

This project is funded by the NSF through grant PHY , and the Universities of JINA. The Joint Institute for Nuclear Astrophysics Henderson DUSEL Capstone Workshop p, 4 He beam Target  rays Direct kinematics: Light ion beam on heavy target Find additional tags to improve detection for (p,) and (,) No additional tag possible only fight to increase signal to noise ratio.  rays p, 4 He target Inverse kinematics: “Heavy ion” beam on light target HI beam Reaction products 10  A for 1 recoil/10 min Require rejection of the beam-> RMS Existing device: Triumf Bochum …

This project is funded by the NSF through grant PHY , and the Universities of JINA. The Joint Institute for Nuclear Astrophysics Henderson DUSEL Capstone Workshop Triumf DRAGON ISAC Radioactive beam induce reaction -> Inverse kinematics is the only solution. Example with stable beam induce reaction 21 Ne(p,g) 22 Na Spectrum and picture from S. Engels Thesis, Recoil energy spectra in singles and coincidence mode for 21 Ne(p,  ) 22 Na at Ecm = keV Gamma energy spectrum in singles and coincidence mode Residual beam

This project is funded by the NSF through grant PHY , and the Universities of JINA. The Joint Institute for Nuclear Astrophysics Henderson DUSEL Capstone Workshop 12 C(,) 16 ERNA - Ecm = 3.2 MeV D. Schürmann, Santa Tecla 2005 Spectrum from D. Schürmann, Santa Tecla 2005 BaF 2  detector Signal Cosmic and room background Beam induced background F. Strieder, Tuckson 2003 Spectrum from F. Strieder, Tuckson 2003

This project is funded by the NSF through grant PHY , and the Universities of JINA. The Joint Institute for Nuclear Astrophysics Henderson DUSEL Capstone Workshop Why a RMS underground ?  The dramatic cosmic background reduction leaves the environmental and beam induce background.  The number of bad  – HI coincidence decrease !! The Notre Dame Recoil Mass separator  Design of a RMS for ( ,  ) reaction studies at low energy for beam with 16<A<40. Large acceptance  <40 mrad  E/E<7.4%  Required for reaction of interest: 22 Ne( ,  ) 26 Mg, 18 O( ,  ) 22 Ne  Mass separation achieved with a Wien filter  New design of the electrodes  First beam expected late 2007  Good prototype for underground laboratory  High intensity AC accelerator is required for beam up to A=40  Source and accelerator LBNL

This project is funded by the NSF through grant PHY , and the Universities of JINA. The Joint Institute for Nuclear Astrophysics Henderson DUSEL Capstone Workshop The Notre Dame RMS Charge selection Jet gas target + post-stripper  detectors Wien Filter – Mass separation Detection system 8cm Recoil Beam Recoil+Beam q selected Beam q+2 q+1

This project is funded by the NSF through grant PHY , and the Universities of JINA. The Joint Institute for Nuclear Astrophysics Henderson DUSEL Capstone Workshop G.P.A. Berg 1, M. Couder 1, J. Görres 1, J. Hinnefeld 2, L.O. Lamm 1, P.J. Leblanc 1, E. Stech 1, M. Wiescher 1 1 University of Notre Dame. 2 Indiana University, South Bend. Summary:  RMS must accept ALL the recoils  Large angular and energy acceptance  Low event rate ~1/few hours  Rejection important >10 20 beam ions  Low energy  No ID of the heavy ion, no additional discrimination   ray – HI coincidence is crucial to make a TRUE EVENT ID