Super-FRS the Next-Generation Facility for Physics with Exotic Nuclei

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Presentation transcript:

Super-FRS the Next-Generation Facility for Physics with Exotic Nuclei Hans Geissel Polish-German Meeting, Warsaw, November 24, 2003 Introduction The Superconducting FRagment Separator The Experimental Branches

Polish Contributions to Nuclear Structure Physics Maria Skłodowska * 7.11.1867 in Warsaw Discovery of Polonium The discovery of the two-proton radioactivity Marek Pfützner Institute of Experimental Physics Warsaw University

Polish Collaborations in Nuclear Structure Research at GSI At the UNILAC (SHIP, Online Separator) Theory and experimental groups for super-heavy element research, spectroscopy of fusion products near the proton dripline and gamma spectroscopy (Coulomb excitation). At the SIS18 (FRS, LAND-ALADIN, ESR) From MUSIC to the discovery of 2p radioactivity Mass measurements Halo and skin nuclei Gamma spectroscopy (RISING) At the Super-FRS Low-Energy Branch: Spectroscopy (a, b, g, p, 2p, ...) Ring Branch: Stored isomeric beams

Physics with Exotic Nuclei Superheavy Elements Fundamental Symmetries and Interactions Parity Violation and Time Reversal in Atoms Applications Sp=0 Test of the Standard Model CKM-Matrix Sn=0 r-Process and Supernovae Nuclear Astrophysics New Decay Mode 2 p-Emission rp-Process, Novae and X-ray Bursts Structure & Dynamics of Exotic Nuclei Halo, Skin, Molecule Nuclei New Shells New Shapes

Discovery of the Proton Halo High Energies RIB → Discovery of the Proton Halo 1500 MeV/u Discovery of 8B isotopes M.E. Nordberg Phys. Rev. Lett. 4 (1960) 23; 3.15 MeV 3He + 6Li  Beta-Alpha correlation measurements W. Schwab et al., Z.Phys. A350 (1995) 283 ; H. Lenske, Prog. Part. Nucl. Phys. 46 (2001)

Advantages of In-flight Separation using Projectile Fragmentation and - Fission High luminosity Secondary reactions in thick targets ~ g/cm2 In-flight separation Short half-lives (Lower time limitation by ToF , 200 ns) High selectivity and sensitivity Single-atom spectroscopy Universal separation Mono-isotopic beams of all elements Cocktail beams optional Experiments with high-energy stored nuclei Kinematic focusing Effective injection into storage rings Full solid angle coverage, complete kinematics Favorable Sudden appoximation, Glauber model Reaction Mechanism

Limitations of the Present Facility Low primary beam intensity (e.g. 108 238U ions /s) Low transmission for projectile fission fragments (4-10%) Low transmission for fragments to the experimental areas (cave B,C) and into the storage ring ESR (a few %) Limited maximum magnetic rigidity @ FRS: for U-like fragments @ ESR: cooler performance and magnets @ALADIN, to deflect break-up fragments

Solutions→ SIS-100/300, Super-FRS, CR, NESR SIS-100/300 238U ions 1012 / s Large Acceptance Superconducting FRagment Separator (Super-FRS) Ion-optical Parameters: CR, NESR

Comparison of FRS and Super-FRS H. Geissel et al. NIM B 204 (2003) 71

The Super-FRS is ideal for Studies of r-Process Nuclei K.-H. Schmidt

The International Accelerator Facility for Beams of Ions and Antiprotons

The Super-FRS and its Branches see talk by Magda Górska

The Super-FRS and its Branches

Reactions with Relativistic Radioactive Beams Experiments in the High Energy Branch of the Super-FRS T. Aumann, H. Emling, B. Jonson Experiments knockout and quasi-free scattering electromagnetic excitation charge-exchange reactions fission spallation fragmentation Physics Goals single-particle occupancies, spectral functions, correlations, clusters, resonances beyond the drip lines single-particle occupancies, astrophysical reactions (S factor), soft coherent modes, giant resonance strength, B(E2) Gamov-Teller strength, spin-dipole resonance, neutron skins shell structure, dynamical properties reaction mechanism, applications (waste transmutation, ...) g-ray spectroscopy, isospin-dependence in multifragmentation

The High Energy Experimental Setup Reactions with Relativistic Radioactive Beams R3B A versatile setup for kinematical complete measurements Large-acceptance measurements Fragments Neutrons Protons Exotic beam from Super-FRS g rays Br = mg v / Z High-resolution momentum measurement T. Aumann

The Super-FRS and its Branches

Predictive Power of Mass Models

New Isospin Dependence of Pairing Yu. Litvinov 2. Pairing-Gap energy, deduced from 5-point binding difference

Predictive Power of the Hatree-Fock- Bogoliubov Model M. Samyn et al. NP A700 (2001) 142 srms= 674 keV srms = 650 keV Yu. Litvinov

Lifetime Measurements of Short-lived Nuclei Applying Stochastic and Electronic Cooling D. Boutin

Observation of the Short-Lived Isomer 207mTl with Stochastic Cooling D. Boutin, F. Nolden

Advantage and Opportunities of eA Experiments PRL 85 (2000) 2913 H. Simon, H. Weick Coincidence with recoils

Technical Challenges at the Super-FRS Magnet System in front of the Production Target Targets, Beam Dump, Degraders (Remote Control, Shielding) Superconducting Magnets up to the First Focal Plane High Rate Detectors and Data Acquisition Isotope Separation Quality with the High Acceptance System Ion Optical Matching of the Super-FRS and the Storage Rings

International Collaborations at the Super-FRS NUSTAR, 73 Council Members, 23 Countries Super-FRS: D(JLU), F(GANIL), JPN(Riken), USA(ANL, MSU), Low-Energy Branch: B, D, E, PL, SF, UK, High-Energy Branch: D, E, NL, S, (R3B) Ring Branch: D, JPN, NL, PL, S, USA

Summary Studies of exotic atoms and exotic nuclei will contribute significantly to the basic knowledge of matter. Precision experiments with stored exotic nuclei open up a new field for nuclear structure physics and astro-physics. The next–generation facility will present unique conditions for research and education. There are many technical challenges inviting especially also the next-generation scientists.

Electron Scattering Conventional eA collider Unstable nuclei Large recoil velocities  full identification (Z,A) Kinematics  4 - geometry, small angles complete kinematics Bare ions  no atomic background Point like particle Pure electromagnetic probe  formfactors F(q) F(q) transition formfactors  high selectivity to certain multipolarities

Layout of the CR Lattice Lattice designed by A. Dolinskii

Layout of the NESR Lattice Tasks In-ring-experiments at Gas-jet-target Electron target Electron ring Deceleration to energies < 100 MeV/u

The Electron Ring Horizontal/vertical emittance [mm mrad] 0.05 Momentum spread [%] ± 0.018 Horizontal tune 3.8 Vertical tune 2.8 Luminosity [cm-2 s-1]  11028