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Technical solutions for NZ Physics

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Kill it at source or live with it? Techniques for selection: Ion chamber. Bragg spectrometer ... Jasmin Schwartz thesis work on 78Rb at the back of the FMA ... – PowerPoint PPT presentation

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Title: Technical solutions for NZ Physics


1
Technical solutions for NZ Physics
  • David Jenkins

2
Outline of talk
  • Physics
  • ISOL Beam development
  • Recoil separator
  • Coulomb excitation
  • Long-lived isomers
  • New techniques

3
Defining the Physics
  • Oblate/prolate shape coexistence
  • Proton-neutron pairing
  • T0 vs T1 states
  • Alignment differences in isobaric multiplets in
    fp shell
  • Isospin mixing e.g. E1 transition matrix
    elements, B(E2) in isobaric multiplets
  • Most Physics is near the ground state not high
    spin!

4
Region of interest
5
RIB issues
  • Can be produced in thick target approach -
    replacing UCx
  • Light Kr easily produced and re-accelerated. Need
    104 pps for Coulomb excitation of e.g. 72Kr.
    Continuation of work of Saclay group
  • Electronegative elements impossible? - e.g. Br,
    Se
  • Zr and heavier (Nb, Mo) do not come out easily in
    ISOL technique - refractory elements
  • Ti-Co has similar problems

ISOLDE target yield information
6
Molecular beam techniquesCoulomb Excitation of
70Se
Se is very electronegative element Positive ions
needed for reacceleration Se extracted as SeCO
molecule and broken up in EBIS to form Se ion
555 keV 104Pd 2
945 keV 70Se 2
70Se on 104Pd target 104 pps June 2005 -
REX-ISOLDE
7
RIB composition
  • Issue of isobaric contamination
  • Kill it at source or live with it?
  • Techniques for selection
  • Ion chamber
  • Bragg spectrometer

Preliminary design of Bragg spectrometer for
REX-ISOLDE
8
Case for a separator
Issues Residues too slow Problem with Z
separation in a transmission ion chamber e.g.
40Ca(40Ca,2n)78Zr Residues too fast FMA-type
separator has insufficient rigidity to bend
residues from very inverse reactions e.g. 40Ca12C
9
Solutions
  • Build a more rigid separator
  • Needs higher electric fields - physically larger
    plates
  • Problems with conditioning
  • Reaccelerate residues to 2 MeV/u for good Z
    separation
  • Wide range in residue energy
  • Beam needs focussing/rebunching

10
Transmission ion chamber
  • 12C(40Ca,3n)49Fe test with FMA at Argonne
  • 230 MeV beam energy
  • Residue energy too high for FMA so degrader foils
    were used - not satisfactory introduces
    scattering and energy spreading
  • Can clean up by gating on Et2 (dimensions of mass)

11
Reacceleration - pipe dream?
1 MeV/u
2 MeV/u
Recoil separator
RF cavity
Wien Filter
Ion Chamber
12
Separator Physics
  • In-beam spectroscopy
  • Reactions with unstable beams
  • Start closer to dripline - fewer residues and
    exotica more abundant
  • Lower gamma counting rates from reactions - but
    rate from potentially gamma emitting beam
  • Reactions with stable beams
  • High beam currents - rotating targets
  • High counting rates in target ge array
  • Exotic channels needle-in-haystack
  • Coulomb excitation at the focal plane

13
Reactions with RIBS
  • 34Ar 40Ca (105-120 MeV)
  • 69Br ?p 1 mb
  • 71Kr 2pn 5 mb
  • 68Br ?pn 0.2 mb
  • 72Rb pn 0.1 mb
  • How do we study the proton unbound cases e.g.
    69Br?
  • 58Cu 28Si (200 MeV)
  • 81Nb ?n 0.1 mb
  • 56Ni 28Si (200MeV)
  • 79Zr ?n 0.2 mb

14
Stable beam reactions
  • Examples
  • Classic
  • 58Ni24Mg - 80Zr 2n
  • Would benefit from more rigid separator
  • Could improve in-beam spectroscopy or produce
    intense beam for focal plane Coulomb excitation
  • How fast can ge array run?
  • New
  • 40Ca40Ca - 78Zr 2n
  • 36Ar40Ca - 74Sr 2n
  • These would need reacceleration to work well with
    the ion chamber
  • Calcium is poor target -oxidation

15
Coulomb excitation at focal plane
  • Jasmin Schwartz thesis work on 78Rb at the back
    of the FMA
  • Beam energy low (2 MeV/u) but currents in
    principle enough e.g. 104 pps
  • Ideas
  • Coulex of 80Zr - very deformed nucleus
  • Coulex of 68Se and 72Kr - deduce B(E2) and sign
    of quadrupole moment. Locate unknown non-yrast 2
    states

16
Coulex of isobaric chains
  • Determine extent of isospin mixing into B(E2)
    rates - most pronounced for odd-odd NZ nucleus
  • Perform Coulomb excitation of isobaric chains
    e.g.
  • 30S,30P,30Si - not easy from ISOL
  • 46Ti,46V, 46Cr - ditto
  • Need high stats (1-2 effects) - but systematic
    errors constrained through simultaneous
    measurements of B(E2)s

17
Long-lived isomers in odd-odd NZ nuclei
18
Total absorption measurements
  • 70Br produced in 36Ar(40Ca,apn) at 145 MeV
  • Recoils into gaseous discharge ion source
  • Produced 55 keV beam of 70Br suitable for TAS
    measurement - Karny et al, Phys. Rev. C 70,
    014310 (2004)
  • Showed that 9 isomer is at 2293 keV in 70Br
  • Where is 5.6 s (5) isomer in 78Y?
  • High current 40Ca40Ca??

19
New technique IRecoil beta tagging
  • Test experiment at JYFL 40Ca(36Ar,pn)74Rb _at_ 95
    MeV
  • Implant residues in focal plane
  • Thick DSSD and planar germanium serve as DE-E
    combination to discriminate high energy betas
    e.g. from Fermi superallowed decays
  • Would benefit from mass separation
  • How competitive is this with charged
    particle/neutron detection?

20
New technique IIBeta-delayed proton tagging
  • Route to study Tz-3/2 nuclei e.g. 69Kr, 65Se,
    57Zn
  • Cleaner tag than betas - use characteristic
    proton energy
  • Programme initiated by Dave Joss, Liverpool

21
New technique 3 Radiative capture
  • 90Zr(90Zr,0n)180Hg studied by Kondev et al.,
    Phys. Rev. C 62, 044305 (2000)
  • 0n cross-section is 30 ?b due to cold-fusion
    reaction
  • Potential for 40Ca40Ca??

22
Conversion electrons
  • Well-known E0 0 -0 in 72Kr
  • Shape coexistence suggests missing 0 states in
    68Se,70Se, 70Br
  • Locating such states would constrain shape mixing
    etc.
  • Electron detection is important (in conjunction
    with gamma detection)
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