Transcript Slide 1
STATUS REPORT ON THE “MASHA” SET-UP A.M.Rodin, A.V.Belozerov, S.N.Dmitriev, Yu.Ts.Oganessian, R.N.Sagaidak, V.S.Salamatin, S.V.Stepantsov, D.V.Vanin PAC for Nuclear Physics, 31st meeting, 25-25 January 2010 • • • • Introduction Status of the mass-spectrometer MASHA From ISOL technique to gas catcher Future PAC for Nuclear Physics, 31st meeting, 25-25 January 2010 Introduction Detectors MAss Separator of Heavy Atoms Ion source D1 Q1 Q2 D2 S2 Q3 General ion-optical parameters Range of energy variation, kV 15-40 Range of Br variation, Tm 0.08-0.5 Mass acceptance, % +/-2.8 Angular acceptance, mrad +/-14 Diameter the ion source exit hole, mm 5.0 Horizontal magnification at F1/F2 0.39/0.68 Mass dispersion at F1/F2, mm/% 1.5/39.0 Linear mass resolution at F1 75 Mass resolution at F2 1150 S1 D3a D3b The proposed setup is a combination of the so-called ISOL method of synthesis and separation of radioactive nuclei with the classical method of mass analysis, allowing mass identification of the synthesized nuclides in the wide mass range. PAC for Nuclear Physics, 31st meeting, 25-25 January 2010 Introduction Chemistry of the element 112 250 Po Pb experimantal data least square fit: 95% c.i. Tl Bi -Hads(Au), kJ/mol 200 150 Hg 100 At -52+20-4 kJ/mol50 Xe Rn -Hads (Au) = (1.08±0.05)*Hsubl+(10.3±6.4), kJ/mol Kr 0 0 50 100 150 200 250 Hsubl, kJ/mol Hsubl=39+23-10 kJ/mol (68%c.i.) PAC for Nuclear Physics, 31st meeting, 25-25 January 2010 Status of the mass-spectrometer MASHA Heater Hot catcher (graphite) Target 112, 114 TO ECR Heavy ion beam Separating foil First experiments: Mass identification of 112 и 114 elements synthesized at the reactions 242Pu(48Ca,3n)287114(0.5 s, a) –> 283112(4 s, a 9.95 MeV) 244Pu(48Ca,3-4n)289114 (2.7 s, a 9.82 MeV) –> 283112(4 s, a 9.95 MeV) Mass identification of 113 elements synthesized at the reaction 243Am(48Ca,3n)288115 (80 ms, a 10.5 MeV ) ->284113(0.5 s, a 10.0 MeV, (analog of Tallium) PAC for Nuclear Physics, 31st meeting, 25-25 January 2010 Status of the mass-spectrometer MASHA Mass-spectrometer MASHA at the beam line of the cyclotron U-400M • • • • • New beam line with low energy of the U-400M was built Mass-spectrometer mounted at the new beam line Hot catcher is ready Focal plane detector system is ready Start of test and first experiments – April of 2010 PAC for Nuclear Physics, 31st meeting, 25-25 January 2010 Status of the mass-spectrometer MASHA 0.15 84 Kr A 0.10 2.42 strips R=1400 0.05 86 83 82 0 0 20 40 60 80 100 120 140 160 180 Strip number Mass spectrum of Kr isotopes: Total efficiency – 47% Mass resolution - 1400 Mass measurement accuracy – 1.3x10-5 PAC for Nuclear Physics, 31st meeting, 25-25 January 2010 From ISOL technique to gas catcher Main parameters of gas catcher • • • • • Operating gas – He purity <0,1 ppm. Operating pressure into gas cell – 100 mbar. Extraction time – 10 ms. Efficiency 10-40%. Beam emittance ~1.0 p.mm.mrad PAC for Nuclear Physics, 31st meeting, 25-25 January 2010 From ISOL technique to gas catcher Ideal gas stopper • Short extraction times. Extraction times of 10 ms or less would be ideal. • Big enough efficiency. Not less than 20%. • Handling of high beam intensities. The facility should provide secondary beam intensities of up to 109 s-1. • Applicability to all fragment beams. • Universality. PAC for Nuclear Physics, 31st meeting, 25-25 January 2010 From ISOL technique to gas catcher General ion-optical parameters of MASHA Parameter Range of energy variation, kV ECR ion source Gas catcher 15-40 15-40 0.08-0.5 0.08-0.5 Mass acceptance, % 2.8 2.8 Angular spread, mrad 14 5 Diameter the ion source exit hole, mm 5.0 1.0 Horizontal magnification at F1/F2 0.39/0.68 0.24/0.90 Vertical magnification at F1/F2 2.40/3.13 8.75/1.25 Mass dispersion at F1/F2, mm/% 1.5/39.0 1.5/39.0 75 420 1150 5700 Range of Bρ variation, Tm Linear mass resolution at F1 Mass resolution at F2 PAC for Nuclear Physics, 31st meeting, 25-25 January 2010 From ISOL technique to gas catcher ~107 c-1 of 48Ca (6 MeV/n) Observation of beam rate-dependent efficiencies as a function of the ionization rate in gas stopping systems at MSU, RIKEN, GSI/SHIPTRAP, LISOL/Leuven, and ANL. PAC for Nuclear Physics, 31st meeting, 25-25 January 2010 From ISOL technique to gas catcher Gas-filled recoil separator 0.200 m Magnet: Bρmax = 2.7 Tm B0max = 6.0 T Banding angle = 82.4o Rcentre ray = 45.2 cm Centre ray length = 65 cm Pole gap, 2h = 10 cm Beam horizontal working region = ±10 cm Entrance (exit) pole tilt angle = 30o(14.7o) 30 o 1 4 ,7 0.500 m o Separator characteristics: Target – magnet distance = 1.0 m Magnet – catcher entrance distance = 1.0 m Solid angle = 10.0 msr ΘX = ± 4.6o, ΘY = ± 2.3o ∆P/P (full) = 4.5% Focal plane dispersion = 2.7 cm/%Bρ Gas – H2 at the pressure 1-5 mbar PAC for Nuclear Physics, 31st meeting, 25-25 January 2010 From ISOL technique to gas catcher Simulation for SHE Reaction: 48Ca + 238U →286112* →283112 + 3n Target: backing foil Ti(0.75 mg/cm2) + UF4 (0.4 mg/cm2) Beam: E0 (48Ca) = 234 MeV (4.88 MeV/n) diameter on target = 10 mm εX = εY = 30π mm mrad (r.m.s) ∆E/E0 = ± 0.5% (r.m.s) Total transmission – 65% 4000 4000 3000 3000 2000 2000 1000 1000 0 0 -2 -1 .5 -1 -0 .5 0 qX (Y ) ( 0 .5 1 1 .5 2 214 216 48 C a ), d e g 218 E( 48 220 222 224 C a ), M e V 2000 6000 1600 4000 1200 800 2000 400 0 0 0 2 4 6 8 10 q( 12 283 14 16 11 2 ) , d e g 18 20 22 24 24 26 28 30 E( 32 34 283 11 2 ) , M e V PAC for Nuclear Physics, 31st meeting, 25-25 January 2010 36 38 40 From ISOL technique to gas catcher Experimental facility for very heavy nuclei research G as-filled reco il separato r D etectors M ass-spectro m eter Q Ta rget Ion beam G as catcher S D PAC for Nuclear Physics, 31st meeting, 25-25 January 2010 Future Methodic development • Gas catcher and gas-filled recoil separator • New design of the silicon detectors DSD with 0.1 mm strips • Germanium detectors for Z identification • New electronics and data acquisition • Start detector based on electron emission from silicon PAC for Nuclear Physics, 31st meeting, 25-25 January 2010 Future Experimental research • Mass identification of heaviest nuclides • Mass measurements of heavy nuclides with accuracy up to 10-7 • Decay spectroscopy of neutron deficit and neutron rich nuclides with A and Z identification • Synthesis and decay research of new neutron rich nuclides • Collinear laser spectroscopy at the wide area of the nuclide chard PAC for Nuclear Physics, 31st meeting, 25-25 January 2010