Search for Proton Radioactivity in the Trans-lead and Sub-tin Regions

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Presentation transcript:

Search for Proton Radioactivity in the Trans-lead and Sub-tin Regions Zhong Liu University of Edinburgh On behalf of the AIDA Collaboration (Edinburgh, Liverpool, STFC DL, RAL) Outline Status of the AIDA detector Overview of the g.s. proton radioactivity Search for p-emitters in the trans-lead region (submitted to GPAC) Search for p-emitters in the sub-tin region

AIDA: status Systems integrated prototypes available - prototype tested on the MARS @ Texas A&M, - some modifications made Production submitted in Q3/2010 Mezzanine: 4x 16 channel ASICs Cu cover EMI/RFI/light screen cooling FEE: 4x 16-bit ADC MUX readout (not visible) 8x octal 50MSPS 14-bit ADCs Xilinx Virtex 5 FPGA PowerPC 40x CPU core – Linux OS FEE width: 8cm Prototype – air cooling Production – recirculating coolant Gbit ethernet, clock, JTAG ports Power

Prototype AIDA Enclosure Prototype mechanical design Based on 8cm x 8cm DSSSD evaluate prior to design for 24cm x 8cm DSSSD Compatible with RISING, TAS, 4p neutron detector 12x 8cm x 8cm DSSSDs 24x AIDA FEE cards 3072 channels Design complete Mechanical assembly in progress In –beam test on the FRS approved (S390) Hope to be scheduled in the 2nd half of 2011

Overview of the proton radioactivity Proton radioactivity provides information on lp wavefunction deformation Z = 53 – 83 (except Z = 61) to extend these studies to the trans-lead and sub-tin regions

Proton drip-line and candidate p-emitters p drip-line p-emitters (Qp~1.5 MeV) 189Bi, 185Bi, 195At, 189,190At 201Fr, 197Fr, 207Ac 203Ac 213Pa. 207Pa 2–5 mass units from the lightest known isotopes.

Production and yield S235: 1A GeV 238U + beryllium target (1g/cm2) Z.Liu et al.,Nucl.Instrum.Methods Phys.Res. A543, 591 (2005) secondary beam 930MeV/u. Yeilds extrapolated at the beam intensity of 109 pps, 208Th,209Th ~100 per day and 203Ac:~10 per day

production cross-section from the fragmentation of the 1A GeV 238U th(mb) exp (mb) imp. yield / day 209 Th 2.8106 1.3106 100 208 Th 4.5107  6.7107 50 203Ac 1.2 108 10 204Ac 9.6 108 80 205Ac 6.8 107 600 199Ra 1.9  10 9 200Ra 2.0  10 8 20 201Ra 1.7  10 7 150 199Fr 3.4  10 6 3000 198Fr 4.2  10 7 350 197Fr 4.5  10 8 40 196Rn 1.9E-5 15000 195Rn 2.2E 6 2000 194Rn 2.1E 7 200 193Rn 1.7E 8 15 191At 1.8  10 7 150 190At 1.2 108 10 189At 6.7 1010 J. Kurcewicz et al. / Nuclear Physics A 767 (2006)

Spectroscopy in the p-rich trans-lead and sub-uranium region proton drip-line -- lightest known isotope -- p-emitter 189Bi, 185Bi 195At, 191At 189At 201Fr, 199Fr 197Fr, 207Ac 206Ac 203Ac 213Pa. 212Pa 207Pa 2–5 mass units from the lightest known isotopes. WKB half-life estimations for Qp = 1.5 MeV, Z = 89 Configurations 203Ac g.s. 7/2, l = 3 2nd min., 5/2 , l = 3 197Fr g.s. 11/2+, l = 6 2nd min., 5/2+ , l = 2 l t1/2 100 µs 1 1.3 ms 2 4 ms 3 30 ms 4 300 ms 5 5 s

Proton Radioactivity Candidates Below 100Sn N=Z+2 N=Z+1 N=Z N=Z-1 Z Te Ag Cd In Sn Sb 103Sb? 99Sn? 97In 95Cd 93Ag 96Cd 100Sn A/Q

Qp and T1/2 for 97In, 93Ag and 89Rh Qp and T1/2 for 97In, 93Ag and 89Rh Qp and T1/2 for 97In, 93Ag and 89Rh with T1/2 > 0.2 ms and L=4 transitions we get (using Delion et al. PRL96(2006)) the Qp values: 89Rh : reasonably good candidate Audi et al; Brown et al; Moller et al; Qp 700(200) keV 640 Kev 500 keV T1/2p 300µs 8 ms 5s (bp~2%) : beta dominate Measurable half-life range 0.5 µs < t/1/2 < 100 ms 93Ag 1.02 MeV > Qp > 0.65 MeV 89Rh 0.94 MeV > Qp > 0.60 MeV

Production and yield WKB half-life estimations for Qp = 1.5 MeV, Z = 89 Configurations 203Ac g.s. 7/2, l = 3 2nd min., 5/2 , l = 3 197Fr g.s. 11/2+, l = 6 2nd min., 5/2+ , l = 2 l t1/2 100 µs 1 1.3 ms 2 4 ms 3 30 ms 4 300 ms 5 5 s

Search for p-emitter in the sub-uranium region p-radioactivity studies have been conducted across a large swathe of the proton dripline, 50<Z<82: g.s. and low-lying isomer Z<50: high-lying, high-spin isomer 53mCo 19/2- 54mNi: 10+ 94mAg (21+) 2p decays 45Fe, 48Ni, 54Zn the heaviest proton emitter identified so far 185Bi (Z=83) Our goal is to extend these studies into the sub-uranium region