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Search for chiral doublet structures in mass A~80 region: odd-A 79 Kr and odd-odd 80 Br with the Hyperball2 array @ CYRIC. CYRIC @Tohoku University Dept. of Physics, Tohoku University T.Fukuchi (Rikkyou University) N.Aoi (RIKEN) J.Timar ATOMKI (Hungary) K. Starosta (MSU)
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Search for chiral doublet structures in mass A~80 region: odd-A 79Kr and odd-odd 80Brwith the Hyperball2 array @ CYRIC CYRIC @Tohoku University Dept. of Physics, Tohoku University T.Fukuchi (Rikkyou University) N.Aoi (RIKEN) J.Timar ATOMKI (Hungary) K. Starosta (MSU) R. Wadsworth Univ. of York (U.K) G. Rainovski (SUNY at Stony Brook)
R jn intmd. short long jp Rh Isotpes Odd-A jn R intmd. short Odd-Odd jp long J. Timar et al. to be submitted.
A~130 Odd-Odd (ph11/2nh11/2-1) 132Cs,130Cs,128Cs,126Cs,124Cs 134La,132La,130La 134Pr,132Pr 136Pm 140Eu,138Eu Odd-A (p(h11/2)2nh11/2-1) 135Nd,135Ce A~190 Odd-Odd (ph9/2ni13/2) 188Ir Even-Even (ph11/2(d5/2,g7/2)n(h11/2)2) 136Nd A~80 (unexplored) Odd-Odd (pg9/2ng9/2-1) 80Br(?), Odd-A (p(g9/2)2ng9/2-1) 79Kr(?) A~105 Odd-Odd (pg9/2-1nh11/2) 106Ag, 106Rh,104Rh,102Rh 100Tc Odd-A (pg9/2-1n(h11/2)2) 107Ag,105Rh, 103Rh
Possible chiral structure in 79Kr 79 1~2.5% p(g9/2)2ng9/2 5~10% 50% G.D. Johns et. al, Phys. Rev. C 50,2786 (1994)
Hyperball2 frame/Rail (March ) BGO counters (April ) Target chamber Cryogenic system/LN2 transport Installation of dets. Electronic set up DAQ Making of targets (A. Lipski) Excitation functions A gg coincidence run A Road to HB2 experiment at CYRIC
gg coincidence measurement with Stony Brook array (6 Compton suppressedGe dets.) 1154 827 559 1026 1144 1144 700 1026 827
Hyperball2 runJune 14~17, 2005 (11shifts) • Reaction: 70Zn(13C,4n)79Kr • Target: 1mg/cm2 self-supporting 70% 70Zn • Beam: 13C3+ @ 65MeV • 4 Clovers + 10 single Ge dets. participating in trigger (out of 12 mounted) • Trigger • Triple or higher Ge coincidence • Compton suppressed; Peak to total=~20% • Coincidence window 150ns
Hyperball2 array performance • Total peak photo efficiency: 0.025 @ 827 keV • Dead time (pile up, reset): 0.1 • Over Compton suppression: 0.3 • Dead time due to noise: 0.2 • FWHM (intrinsic) • ~4keV (single Ge) & ~3keV (Clover) • DAQ dead time: 0.3 827keV gated 1026 1144 827
Performance improvement • Number of detectors 14 →18 • Collimator for Ge detectors • Over suppression 0.3 → 0.01 Total photo peak efficiency = 0.025 X1.3X1.4 =0.045 @ ~827 keV For triple coincidence, performance improvement by 1.823 =6
Proposed experiment with the Hyperball2 array • 70Zn(13C,4n)79Kr @ 65MeV • Pb backed 1mg/cm270Zn target (ready) • Reduction of Doppler broadening • ~200K counts for 827keV peak X 6=1.2M • 1.2MX0.01=12K for the transitions of interests in 12 shifts with triple coincidence measurement • 3 shifts for 80Br test run with the same reaction but lower energy @55MeV Total of 15 shifts
Total cross section σ=~1b Beam intensity I: 2pnA Target thickness S: 1mg/cm2 Average number of gamma rays emitted:10 Rate estimate ~106 gamma/second
σ=~500mb Beam intensity I: 2pnA Target thickness S: 1mg/cm2 Average number of gamma rays emitted:10 Total photo peak efficiency of Hyperball2: 5% 79Kr yield estimate (79Kr: 54K particle/second)X10X(0.05)3X24x3600 ~6 million g-g-g coincidence in 79Kr per day 24million g-g-g coincidence in requested 12 shifts equivalent to 72 g-g unfolded event
Doublet bands in 10545Rh60 J. Timar et al., PLB598,178 (2004). Energy [MeV] Spin [ħ]
Doublet bands in odd-even 13560Nd75S. Zhu et al., PRL 91(2003) 132501. Energy [MeV] Spin [ħ]
Hyperball2experiment @ CYRIC (Being assembled) • 70Zn(13C,4n)79Kr @58MeV or 65Cu(18O,p3n)79Kr @65MeV • [ Single Ge (60%) +BGO ] x 14 + [ Clover type Ge (125%) +BGO ] x 6 → Photopeak efficiency ~ 5% at 1 MeV • UMEM/Double buffering
Possible chiral structure in 79Kr p(g9/2)2ng9/2 G.D. Johns et. al, Phys. Rev. C 50,2786 (1994)
In-beam experiment with Hyperball2 • Advantages • Large total photo peak efficiency (g-g-g coincidence) • Transistor reset type (high counting rate→ high intensity beam) • BGO as a multiplicity filter (12x6+6x14=156 elements) • Clover detector as Compton polarimeter • Disadvantages • Few angles (detectors placed mostly around 90º) → lower angular correlation sensitivity
Ge det. status at glance • Eurisys Single Crystal Ge (r.e. ~60%) X 5 • Ortec Single Crystal Ge (r.e. ~60%) X 10 • Eurisys Clover type Ge X 6 • (r.e. ~20%, add-back 125%) Total X 21 Ready for use X 12 Being Repaired X 6 (G2,G3,G14,S/N1,S/N3,S/N4) Problematic X 3 (G1,G9,G1)
Target chamber for in-beam experiments with Hyperball2 at CYRIC
Important theme of nuclear structure studiesNuclear deformation • Spontaneous symmetry breaking • Collective degree of freedom • Nuclear Shape • Coupling of single particle degree and collective degree of freedom
132Ce Rotation
Unique Parity Orbit N=5 • Simple Harmonic Oscill. • (SHO) • p=(-1)N N=4 • SHO+l•s • Major shell consisting of • majorities of normal parity • and unique parity orbitals. N=3 N=2 • The ph11/2nh11/2 confg. • is comprised of two • unique parity orbitals. N=1 0s 0s N=0 0s1/2 SHO SHO+l•s
R jp jn Possible realization for chiral geometry:odd-odd nuclei in the A~130 region intmd. • Z=~55 N=~75 • Triaxial mass distribution (shape). • Fermi level lies • low in proton h11/2subshell, • highin neutron h11/2subshell. • Collective rotation of triaxial rotor • with irrotational flow moment of inertia. short long
Chiral Geometry in Nuclei Mutually orthogonal coupling of three angular momenta in odd-odd nuclei K.Starosta Phys. Rev. Lett. 86, 971 (2001).
134Pr Chirality