Development of a rapid solvent extraction apparatus coupled to the GARIS gas-jet transport system for aqueous chemistry of the heaviest elements

Similar documents
Development of a rapid solvent extraction apparatus for aqueous chemistry of the heaviest elements

Production and decay studies of 261 Rf, 262. Db, 265 Sg, and 266 Bh for superheavy element chemistry at RIKEN GARIS

RIKEN GARIS for Superheavy Element Chemistry

Perspectives of the superheavy element chemistry at RIKEN GARIS

Chemistry GARIS

Present status of the heaviest elements study using GARIS at RIKEN

Aqueous Chemistry of Rf and Db Y. Nagame for JAEA-RIKEN-Osaka-Niigata-TMU-Tsukuba- Kanazawa-Shizuoka-GSI-Mainz collaboration

First synthesis and investigation

SHE experiments with GARIS-I/-II at RIKEN

Performance of the Gas-jet Transport System Coupled to the RIKEN Gas-filled Recoil Ion Separator GARIS for the 238 U( 22 Ne, 5n) 255 No Reaction

Chemistry of the Heaviest Elements

Method of active correlations in the experiment 249 Cf+ 48 Ca n

The SISAK System (part 1) On-line LS Detection (part 2)

Measurement of activation of helium gas by 238 U beam irradiation at about 11 A MeV

Present status of SISAK and future plans


COMPARATIVE STUDY OF PIGE, PIXE AND NAA ANALYTICAL TECHNIQUES FOR THE DETERMINATION OF MINOR ELEMENTS IN STEELS

Charge-state distribution measurements using gas charge stripper toward

TECHNETIUM-99 IN SOIL

7. Relax and do well.

D1. TASCA Focal Plane Detector Setup (Physics) - first mounting and detector tests

KEK isotope separation system for β-decay spectroscopy of r-process nuclei

Study of multinucleon transfer (MNT) reactions of 136 Xe Pt for production of exotic nuclei

Particle Size of Radioactive Aerosols Generated During Machine Operation in High-energy Proton Accelerators

Status of the magnetic spectrometer PRISMA

anti-compton BGO detector

ORTEC AN34 Experiment 10 Compton Scattering

Synthesis and stability of [ 77 Br]-m-Bromobenzylguanidine ( 77 Br-MBBG)

What do we know experimentally about the N=149, N=151 and N=153 isotones?

Detectors for the measurement of ionizing radiation

Review of ISOL-type Radioactive Beam Facilities

Determination of 126 Sn in nuclear wastes by using TEVA resin

Hiroyasu Hotokezaka 1, Manabu Tokeshi 2, Masayuki Harada 1, Takehiko Kitamori 2,3, and Yasuhisa Ikeda 1

Application of positrons in materials research

Role of Hexadecupole Deformation in the Shape Evolution of Neutron-rich Nd Isotopes

RITU and the GREAT Spectrometer

MRTOF mass measurements at GARIS-II: Toward SHE identification via mass spectroscopy

Ultra-Pure 163 Ho Samples for Neutrino Mass Measurements

7. Relax and do well.

Development of Secondary Electron Time Detector for Ion Beams

Patricia Paviet-Hartmann Los Alamos National Laboratory, Carlsbad Operations Environmental Science and Waste Technology Division Carlsbad, NM 88220

Detection of explosives and fissile material based on neutron generators, survey of techniques and methods. M. Bruggeman

Measurement of induced radioactivity in air and water for medical accelerators

Rivelazione di neutrini solari - Borexino Lino Miramonti 6 Giugno 2006 Gran Sasso

A Comparison between Channel Selections in Heavy Ion Reactions

5 questions, 3 points each, 15 points total possible. 26 Fe Cu Ni Co Pd Ag Ru 101.

RADIOLOGICAL CHARACTERIZATION Laboratory Procedures

VI. 1. Development of a Simplified MA Separation Process Using Novel R-BTP Adsorbents II

Megan E. Bennett, Dmitriy A. Mayorov, Kyle D. Chapkin, Marisa C. Alfonso, Tyler A. Werke, and Charles M. Folden III

G SI Darmstadt. TASCA TransActinide Separator and Chemistry Apparatus

New Concept of EPOS Progress of the Mono-energetic Positron Beam (MePS) Gamma-induced Positron Spectroscopy (GiPS)

J, RADIOANAL.NUCL.CHEM., LETTERS 85 /5/ /1984/ PRODUCTION OF 232pa FROM THORIUM. G.T. Baldwin x, H.C. Griffin, G.F. Knoll

O WILEY- MODERN NUCLEAR CHEMISTRY. WALTER D. LOVELAND Oregon State University. DAVID J. MORRISSEY Michigan State University

EXPERIENCE WITH STRIPPING HEAVY ION BEAMS

Effect of Carrier Gas Flow Behavior on Performance of Separation by Using Ultrasonic Atomization

2016 Update of the discoveries of nuclides

Production of Fluorine-18 by Small Research Reactor

Differential Mobility Particle Sizer (Aerosol measurements)

Synthesis of New Elements and New Approaches in SHE Research

V. 3. Development of an Accelerator Beam Loss Monitor Using an Optical Fiber

Capture barrier distributions and superheavy elements

Development of Zeolite Nonwoven for the Adsorption of Radioactive Cesium-13288

Gas-phase chemistry of element 114, flerovium

for (n,f) of MAs 1. Introduction

Development of Ring-Imaging Cherenkov Counter for Heavy Ions

TECHNETIUM-99 IN WATER

Temperature effect on lyoluminescence of potassium halide microcrystals in luminol solution

* * TASCA in Small Image Mode Spectroscopy

Visualization of Xe and Sn Atoms Generated from Laser-Produced Plasma for EUV Light Source

Acronyms, Abbreviations, and Symbols Foreword to the First Edition Foreword to the Second Edition Preface to the First Edition Preface to the Second

8. Relax and do well.

Measurements of the first ionization potentials of the heaviest actinides. T. K. Sato. Advanced Science Research Center Japan Atomic Energy Agency

Structure of neutron-rich Mg isotopes explored by beta-decay of spin-polarized Na isotopes

Fission research at JAEA and opportunity with J-PARC for fission and nuclear data

Survey of the performance of scintillation materials at low temperatures

DETERMINING FUNDAMENTAL PARAMETERS OF A SINGLE-PHOTOTUBE LIQUID SCINTILLATION COUNTER

samples before and after the Fukushima Daiichi Nuclear Power Plant accident

Radiochemical Studies of the Transactinide Element, Rutherfordium (Rf) at JAERI

Experimental Study of Stellar Reactions at CNS

1.E Neutron Energy (MeV)

Department of Physics, Techno India Batanagar (Techno India Group), Kolkata , West Bengal, India.

Three sources and three components of success in detection of ultra-rare alpha decays at the Dubna Gas-Filled Recoil separator Yu.S.

REFERENCE SOURCES FOR THE CALIBRATION OF THE AUTOCORRELATION SINGLE-CRYSTAL SCINTILLATION TIME SPECTROMETER

MODULE 4.3 Atmospheric analysis of particulates

Solutions and Ions. Pure Substances

Measurements for 44 Ti at TRIUMF-ISAC 40

Determination of the activity of radionuclides

7. Relax and do well.

Experiment Radioactive Decay of 220 Rn and 232 Th Physics 2150 Experiment No. 10 University of Colorado

Reduction of Radioactive Waste by Accelerators

Physics with Exotic Nuclei

Shielded Scintillator for Neutron Characterization

arxiv: v1 [nucl-ex] 24 Apr 2017

Lab Day and Time: Instructions. 1. Do not open the exam until you are told to start. Page # Points possible Points awarded

2. Which of the following statements help(s) to explain why gas can fill the vessel containing it completely while liquid cannot?

DEVELOPMENT OF A NEW POSITRON LIFETIME SPECTROSCOPY TECHNIQUE FOR DEFECT CHARACTERIZATION IN THICK MATERIALS

First on the South Pole, 14 December, 1911

Experimental data analysis at the MASHA setup. Prepared by: Abeer M. Attia Supervisor: Lubos Krupa LOGO. Aleksey Novoselov

Mass Determination of Rn and Hg isotopes using MASHA

XMASS 1.5, the next step of the XMASS experiment

Transcription:

Development of a rapid solvent extraction apparatus coupled to the GARIS gas-jet transport system for aqueous chemistry of the heaviest elements Y. Komori 1, H. Haba 1, K. Ooe 2, D. Kaji 1, Y. Kasamatsu 3, H. Kikunaga 4, A. Mitsukai 5, K. Morimoto 1, R. Motoyama 2, J. P. Omtvedt 6, Z. Qin 7, D. Sato 2, N. Sato 1, Y. Shigekawa 3, T. Tanaka 1, A. Toyoshima 5, K. Tsukada 5, Y. Wang 7, K. Watanabe 1, S. Wulff 6, S. Yamaki 1, S. Yano 1, and Y. Yasuda 3 1 RIKEN Nishina Center, 2 Grad. School of Sci. and Technol., Niigata Univ., 3 Grad. School of Sci., Osaka Univ., 4 ELPH, Tohoku Univ., 5 ASRC, JAEA, 6 Univ. Oslo, 7 IMP

Introduction: Aqueous chemistry of SHEs Gas phase: Z = 104 108, 112 114 Liquid phase: Z = 104 106 Most of the aqueous chemistry of SHEs have been performed using a batch-wise column chromatography apparatus (ARCA) with Si detectors. Nuclide Half-life (s) Production rate* (atoms/h) 261 Rf a 68 420 262 Db 34 70 265 Sg a,b 8.5, 14.4 12 266 Bh 10.0 1.7 * 248 Cm target thickness: 300 μg/cm 2 ; Beam intensity: 2 pμa Pioneering cation-exchange studies of Sg in HNO 3 /HF and HNO 3 Schädel et al., Radiochim. Acta 77, 149 (1997).; Radiochim. Acta 83, 163 (1998). Decay loss during aerosol collection and α-source preparation (~30 s) Low detection efficiency: eff.(α) = ~30% eff.(α-α) = ~9%; eff.(α-α-α) = ~3% A huge amount of background radioactivities of by-products Requirements for the aqueous chemistry studies of Sg and Bh Continuous, rapid, and efficient chemistry apparatus Low-background condition for α/sf detection 1

RIKEN GARIS gas-jet system RIKEN GARIS Gas-jet transport system Differential pumping section Evaporation Beam from RILAC Residues (ERs) Beam dump Gas inlet Focal plane Mylar window 50 kpa ERs Rotating target 33 Pa Elastic scattering beam monitor D1 Q1 Q2 Haba et al., Chem. Lett. 38, 426 (2009). 0 D2 1 2 m He/KCl 0 100 mm By-products are removed almost completely. Production and decay studies of 265 Sg a,b and 266 Bh were successfully performed: 248 Cm( 22 Ne,5n) 265 Sg a,b Haba et al., Phys. Rev. C 85, 024611 (2012). 248 Cm( 23 Na,5n) 266 Bh Haba et al., APSORC 17, A-049 Pre-separated 265 Sg a,b and 266 Bh are ready for the chemistry experiments at GARIS. 2

Continuous and rapid solvent extraction apparatus coupled to the GARIS gas-jet system GARIS gas-jet system He/KCl aerosols 265 Sg a,b, 266 Bh Membrane DeGasser (MDG) Gas out Flow Solvent Extractor (FSE) Membrane filter Organic phase () Membrane filter Photomultiplier tube Mylar window Irradiation room Aqueous solution () Chemistry laboratory Teflon capillary (i.d. = 0.5 mm) Phase separator Liquid scintillator Liquid scintillation α/sf detectors Continuous dissolution, solvent extraction, and radiation detection Minimization of decay loss of 265 Sg a,b and 266 Bh Efficient α/sf detection with LS: eff.(α-α/sf) = ~100% By using this apparatus, we can expect 60 100 times larger event rate of 265 Sg a,b and 266 Bh than those by using the conventional apparatus. 3

This study Toward the aqueous chemistry of element 107, Bh Development of Membrane DeGasser (MDG) and Flow Solvent Extractor (FSE) On-line solvent extraction of Re with the MDG-FSE coupled to the GARIS gas-jet system Measurement of gas-jet transport, dissolution, and solvent extraction times of Re in the MDG-FSE 4

Experimental (1): Production of Re isotopes RIKEN GARIS Rotating nat Gd 2 O 3 target Differential pumping section Elastic scattering beam monitor 23 Na beam ERs ( 174 Re) from RILAC Beam dump D1 Q1 Q2 Irradiation room Gas inlet D2 0 Focal plane ERs 1 2 m 33 Pa Gas-jet transport system Mylar window: 2.5 µm He/KCl 0 100 mm nat Gd 2 O 3 target nat Gd( 23 Na,xn) 174 Re (T 1/2 = 2.4 min) 176 Re (T 1/2 = 5.3 min) Beam: 124.3-MeV 23 Na 7+, 1.6 particle μa Target: 349 µg/cm 2 nat Gd 2 O 3 on 3-µm Ti GARIS Bρ: 1.73 Tm Gas-jet chamber 5

Experimental (1): Solvent extraction of Re isotopes GARIS gas-jet system Gas out H + + [ReO 4 ] + TOA [HReO 4 TOA] org. 174 Re He/KCl aerosols Membrane filter Organic phase () Teflon capillary (i.d. = 0.5 mm) Membrane filter γ-ray spectrometry Mylar window: 2.5 µm Irradiation room Aqueous solution () He: 1.5 L/min Chemistry laboratory Collection on glass fiber filter γ-ray spectrometry Distribution ratio, D = [A] org. /[A] aq. (A: radioactivities) Chemical yield, C.Y. = ([A] org. + [A] aq. ) 100/[A] glass fiber filter D vs. Capillary length D vs. [TOA] phase 0.5 M HNO 3 0.5 M HNO 3 phase 0.01, 0.1 M TOA / toluene 0.005 0.1 M TOA / toluene Capillary length (30), 40, (50), 70, 100 cm 40 cm Extraction equilibrium time, applicable D range 6

MDG and FSE Membrane DeGasser (MDG) Flow Solvent Extractor (FSE) Gas out Teflon capillary (i.d. = 0.5 mm) out in Gas-jet in Ooe et al., J. Radioanal. Nucl. Chem. 303, 1317 (2015). Flow Solvent Extractor (FSE) PTFE Membrane filter AVDAVNTEC No. T300A013A Pore size: 3.0 µm Phase separator Komori et al., RIKEN Accel. Prog. Rep. 49,29 (2016). 7

Experimental (1): Solvent extraction of Re isotopes GARIS gas-jet system Gas out H + + [ReO 4 ] + TOA [HReO 4 TOA] org. 174 Re He/KCl aerosols Membrane filter Organic phase () Teflon capillary (i.d. = 0.5 mm) Membrane filter γ-ray spectrometry Mylar window: 2.5 µm Irradiation room Aqueous solution () He: 1.5 L/min Chemistry laboratory Collection on glass fiber filter γ-ray spectrometry Distribution ratio, D = [A] org. /[A] aq. (A: radioactivities) Chemical yield, C.Y. = ([A] org. + [A] aq. ) 100/[A] glass fiber filter D vs. Capillary length D vs. [TOA] phase 0.5 M HNO 3 0.5 M HNO 3 phase 0.01, 0.1 M TOA / toluene 0.005 0.1 M TOA / toluene Capillary length (30), 40, (50), 70, 100 cm 40 cm Extraction equilibrium time, applicable D range 8

Experimental (2): Measurement of gas-jet transport, dissolution, and extraction times 152 Gd( 23 Na,5n) 170 Re (T 1/2 = 9.2 s) ~ 265 Sg and 266 Bh 170 Re (9.2 s) Irradiation room He/KCl aerosols Membrane filter Gas out Chemistry laboratory Extraction capillary i.d. = 0.5 mm L = 100 cm Mylar window: 3.5 µm He: 1.5 L/min γ-ray spectrometry Phase separator Glass fiber filter (ADVANTEC GB-100R) Radioactivity Beam on 10 s Beam off 110 s Radioactivity Beam on 10 s Beam off 110 s Delay Elapsed time Elapsed time 8

Experimental (2): Measurement of gas-jet transport, dissolution, and extraction times 152 Gd( 23 Na,5n) 170 Re (T 1/2 = 9.2 s) ~ 265 Sg and 266 Bh 170 Re (9.2 s) Irradiation room He/KCl aerosols Membrane filter Gas out Chemistry laboratory Extraction capillary i.d. = 0.5 mm L = 100 cm Mylar window: 3.5 µm Phase separator Radioactivity Beam on 10 s He: 1.5 L/min Beam off 110 s Delay Glass fiber filter (ADVANTEC GB-100R) Time distributions of radioactivity were measured by γ-ray spectrometry. Elapsed time 9

Results and discussion (1): Solvent extraction of Re isotopes Counts / 0.5 kev 10 5 10 4 10 3 10 2 109.1 176 Re 113.0 174 Re 123.2 172 Re 130.2 173 W 148? 181.5 173 Re γ-ray spectrum 184.5 175 Re 190.7 173 Re 196.9 177 Re 240.2 176 Re ( T 1/2 = 5.3 min) 243.4 174 Re (T 1/2 = 2.4 min) 253.9 172 Re RUN: F07-1 Aerosol coll.: 60 s Cooling time: 60 s Meas. time: 60 s 349.5 174 Re, 351.2 176 Re 373.6 173 Re D 1 D vs. Capillary length 10 0.5 M HNO 3 [TOA] = 0.01 M 174 Re MDG-FSE 176 Re MDG-FSE 181 Re Batch ext. 10 1 195? 120 180 240 300 360 Energy / kev 0.1 0 20 40 60 80 100 Capillary length / cm Extraction equilibrium of 174,176 Re is attained with a 30-cm capillary. Time required for solutions to pass through the capillary: ~1.8 s. Average chemical yields of 174,176 Re: ~75% 10

Results and discussion (1): Solvent extraction of Re isotopes D vs. TOA concentration Capillary length (L) = 40 cm 100 0.5 M HNO 3 D vs. Capillary length 100 0.5 M HNO 3 [TOA] = 0.1 M 10 D D 10 1 174 Re MDG-FSE 176 Re MDG-FSE 181 Re Batch ext. 174 Re MDG-FSE 176 Re MDG-FSE 181 Re Batch ext. 0.1 10-3 10-2 10-1 10 0 TOA concentration / M 1 0 20 40 60 80 100 Capillary length / cm D values of 174,176 Re agree well with those of 181 Re in equilibrium at [TOA] 0.01 M. The 40-cm capillary is too short for Re to reach the extraction equilibrium at [TOA] 0.05 M. MDG-FSE is applicable in the wide range of D = 0.3 20 with the 100-cm capillary. 12

Results and discussion (2): Measurement of gas-jet transport, dissolution, and extraction times Net counts per 1 s Net counts per 1 s 300 200 100 Cumulative and differential time distribution of 170 Re Beam on (10 s) GARIS Aerosol Beam on (10 s) collection apparatus ΔT Net counts of 170 Re (305.7 kev) Run 1 (Accumulation and decay of radioactivity) Net counts of 170Re (305.7 kev) Fit with Fit with a "LogNormal lognormal function" Time distribution of 170Re Differential time distribution of 170 Re (arb. unit) Aerosol collection apparatus Net counts per 1 s Net counts per 1 s 200 150 100 50 ΔT GARIS Outlet of the MDG Run The 3 fitted experimental data were deconvoluted with Net counts of 170Re (305.7 kev) a response Fit with "LogNormal function function" Time distribution of 170Re exp( ln(2)*t/9.2) MDG + (5 + 20) cm capillary 0 0 0 10 20 30 40 50 60 70 80 Time since start of beam irradiation [s] Time since start of beam irradiation [s] 0 0 0 10 20 30 40 50 60 70 80 0 10 20 30 40 50 60 70 80 Time since start of beam irradiation [s] Time since start of beam irradiation [s] Average transport time (ΔT): time interval from a half of the irradiation time (5 s) to the time that gives 50% of the integral value of the differential time distribution of 170 Re 13

Results and discussion (2): Measurement of gas-jet transport, dissolution, and extraction times GARIS gas-jet system Gas out Chemistry laboratory 170 Re He/KCl aerosols Membrane filter Mylar window Irradiation room He: 1.5 L/min Extraction capillary (EC) i.d. = 0.5 mm L = 100 cm Phase separator (PS) 114 kpa 154 kpa 3.1 s 5.1 s 114 kpa 13.2 s 145 kpa 18.6 s 154 kpa 22.7 s Gas-jet chamber Aerosol collection apparatus Outlet of MDG Outlet of EC Outlet of PS 13

Results and discussion (2): Measurement of gas-jet transport, dissolution, and extraction times GARIS gas-jet system 170 Re He/KCl aerosols Membrane filter Gas out Chemistry laboratory 114 kpa 154 kpa Mylar window Irradiation room He: 1.5 L/min Gas-jet transport 3.1 s 5.1 s Extraction capillary (EC) i.d. = 0.5 mm L = 100 cm Phase separator (PS) 114 kpa 145 kpa 13.2 s 18.6 s 154 kpa 22.7 s Gas-jet chamber Aerosol collection apparatus Outlet of MDG Outlet of EC Outlet of PS 13

Results and discussion (2): Measurement of gas-jet transport, dissolution, and extraction times GARIS gas-jet system 170 Re He/KCl aerosols Membrane filter Gas out Chemistry laboratory 114 kpa 154 kpa 114 kpa 145 kpa Mylar window Irradiation room He: 1.5 L/min Gas-jet transport 3.1 s 5.1 s 13.2 s 18.6 s 10.1 s (Calc. 4.4 s) Dissolution Extraction capillary (EC) i.d. = 0.5 mm L = 100 cm Phase separator (PS) 154 kpa 22.7 s Gas-jet chamber Aerosol collection apparatus Outlet of MDG Outlet of EC Outlet of PS 13

Results and discussion (2): Measurement of gas-jet transport, dissolution, and extraction times GARIS gas-jet system 170 Re He/KCl aerosols Membrane filter Gas out Chemistry laboratory 114 kpa 154 kpa 114 kpa 145 kpa Mylar window Irradiation room He: 1.5 L/min Gas-jet transport 3.1 s 5.1 s 13.2 s 18.6 s 10.1 s (Calc. 4.4 s) Dissolution Extraction capillary (EC) i.d. = 0.5 mm L = 100 cm Extraction 6.3 s (Calc. 5.9 s) Phase separator (PS) 154 kpa 22.7 s Gas-jet chamber Aerosol collection apparatus Outlet of MDG Outlet of EC Outlet of PS 13

Results and discussion (2): Measurement of gas-jet transport, dissolution, and extraction times GARIS gas-jet system 170 Re He/KCl aerosols Membrane filter Gas out Chemistry laboratory 114 kpa 154 kpa 114 kpa 145 kpa Mylar window Irradiation room He: 1.5 L/min Gas-jet transport 3.1 s 5.1 s 13.2 s 18.6 s 10.1 s (Calc. 4.4 s) Dissolution Extraction capillary (EC) i.d. = 0.5 mm L = 100 cm Extraction 6.3 s (Calc. 5.9 s) Phase separator (PS) Phase separation 3.6 s (Calc. 3.1 s) 154 kpa 22.7 s Gas-jet chamber Aerosol collection apparatus Outlet of MDG Outlet of EC Outlet of PS 13

Summary We have been developing a new rapid solvent extraction apparatus consisting of MDG and FSE coupled to the GARIS gas-jet system for the future aqueous chemistry of Sg and Bh. On-line solvent extraction of Re was successfully performed using MDG-FSE coupled to the GARIS gas-jet system. Rapid equilibrium time: ~2 6 s (30 100 cm capirrary) Wide applicable D range of D = 0.3 20 High chemical yield: ~75% Gas-jet transport, dissolution, and solvent extraction times of Re in the developed apparatus were investigated. Gas-jet transport time: 5.1 s at 154 kpa Overall time: Dissolution time in the MDG: 10.1 s ~25 s Solvent extraction time in the FSE: 6.3 s (100-cm extraction capillary) + 3.6 s (phase separator) 14

Future outlook We will modify the MDG to shorten the dissolution time. A flow liquid scintillation detection system will be developed. Interesting chemistry systems for Sg and Bh are under study using radiotracers of their homologues. Hydrolysis and fluoride complex formation of Sg(VI) Refs: A. Kronenberg et al., Radiochimica Acta 92, 395 (2004). X. H. Liang et al., J. Radioanal. Nucl. Chem. 292, 917 (2012). Formation of anionic species of Bh(VII), [BhO 4 ] Redox studies of Bh(VII) Bh(IV) Ref: M. Schädel, D. Shaughnessy, The Chemistry of Superheavy Elements, Second Edition, Springer, Heidelberg, 2014. 15

21

Feasibility of aqueous chemistry of Sg and Bh Continuous solvent extraction and LS detection (Present apparatus) Nuclide T 1/2 [s] σ [pb] Target [μg/cm 2 ] Beam [pμa] Cool. T. [s] Chem. Y. [%] Detec. eff.* [%] Event rate for α-α [1/d] 265 Sg a 8.5 180 300 4 10 50 100 2.8 265 Sg b 14.4 200 300 4 10 50 100 4.9 266 Bh 10.0 57 300 4 10 50 100 1.0 Batch-wise chemical separation (e.g. ARCA and AIDA) Nuclide T 1/2 [s] σ [pb] Target [μg/cm 2 ] Beam [pμa] Coll. T. [s] Cool. T. [s] Chem. Y. [%] Detec.* eff. [%] Event rate for α-α [1/d] 265 Sg a 8.5 180 300 4 30 30 50 9 0.02 265 Sg b 14.4 200 300 4 30 30 50 9 0.1 266 Bh 10.0 57 300 4 30 30 50 9 0.01 * Efficiencies for α-α correlations. 22

Experimental (2): Measurement of gas-jet transport, dissolution, and extraction times 152 Gd( 23 Na,5n) 170 Re (T 1/2 = 9.2 s) ~ 265 Sg and 266 Bh 170 Re (9.2 s) Irradiation room He/KCl aerosols Membrane filter Gas out Chemistry laboratory Extraction capillary i.d. = 0.5 mm L = 100 cm Mylar window: 3.5 µm Phase separator Radioactivity Beam on 10 s He: 1.5 L/min Beam off 110 s Delay Glass fiber filter (ADVANTEC GB-100R) Time distributions of radioactivity were measured by γ-ray spectrometry. Elapsed time 9

Convolution and deconvolution A convolution of two functions, f and g is written as f g. ff gg tt = ff ττ gg tt ττ ddττ ff : (Differential) time distribution of radioactivity gg : Decay of radioactivity, exp( ln(2)*t/9.2) Algorithms for deconvolution Deconvolution is performed based on the convolution theorem FFT ff gg = FFT(ff)FFT(gg) ff = IFFT FFT ff gg FFT(gg) Cumulative time distributions of radioactivity of 170 Re (T 1/2 = 9.2 s) Net counts per 1 s Net counts per 1 s 300 200 100 Beam irradiation (10 s) Net counts of 170 Re (305.7 kev) Run 1 (Accumulation and decay of radioactivity) Net counts of 170Re (305.7 kev) Fit with Fit with a "LogNormal lognormal function" Time distribution of 170Re Differential time distribution of 170 Re (arb. unit) Aerosol collection apparatus where FFT and IFFT denote fast Fourier transform and its inverse, respectively. 0 0 0 10 20 30 40 50 60 70 80 Time since start of beam irradiation [s] Time since start of beam irradiation [s]

Convolution and deconvolution A convolution of two functions, f and g is written as f g. ff gg tt = ff ττ gg tt ττ ddττ Cumulative time distributions of radioactivity of 170 Re (T 1/2 = 9.2 s) f: (Differential) time distribution of radioactivity g: Decay of radioactivity, exp( ln(2)*t/9.2) To derive the differential time distribution of radioactivity (f), we deconvoluted the fitted experimental data with the response function g. Net counts per 1 s Net counts per 1 s 300 200 100 Beam on (10 s) ΔT Net counts of 170 Re (305.7 kev) Run 1 (Accumulation and decay of radioactivity) Net counts of 170Re (305.7 kev) Fit with Fit with a "LogNormal lognormal function" Time distribution of 170Re Differential time distribution of 170 Re (arb. unit) Aerosol collection apparatus 0 0 0 10 20 30 40 50 60 70 80 Time since start of beam irradiation [s] Time since start of beam irradiation [s]

Extractant: tri-n-octylamine (TOA) Tri-n-octylamine (TOA) An liquid-anion exchanger 26

Appendix 100 1 M HNO 3 100 0.5 M HNO 3 10Slope (Tc) = 1.2 10 Slope = 1.4 D 1 Slope (Re) = 1.4 95m Tc (FSE) 183 Re (FSE) 95m Tc (batch) 183 Re (batch) D 1 174 Re MDG-FSE 176 Re MDG-FSE 181 Re Batch ext. 0.1 10-3 10-2 10-1 10 0 TOA concentration / M 0.1 10-3 10-2 10-1 10 0 TOA concentration / M 27

100 0.5 M HNO 3 10 Slope = 1.4 D 1 174 Re MDG-FSE 176 Re MDG-FSE 181 Re Batch ext. 0.1 10-3 10-2 10-1 10 0 TOA concentration / M 28

Introduction: Aqueous chemistry of SHEs Aqueous chemistry of SHEs (Z 104) Aqueous chemistry of Rf, Db, and Sg has been performed using a batch-wise column chromatography apparatus (ARCA) with Si detectors. Nuclide Half-life (s) Production rate* (atoms/h) 261 Rf a 68 420 262 Db 34 70 265 Sg a,b 8.5/14.4 12 266 Bh 10.0 1.7 * 248 Cm target thickness: 300 μg/cm 2 ; Beam intensity: 2 pμa Pioneering cation-exchange studies of Sg in HNO 3 /HF and HNO 3 Schädel et al., Radiochim. Acta 77, 149 (1997).; Radiochim. Acta 83, 163 (1998). Decay loss during aerosol collection and α-source preparation (~30 s) Low detection efficiency: eff.(α) = ~30% eff.(α-α) = ~9%; eff.(α-α-α) = ~3% A huge amount of background radioactivities of by-products Requirements for the aqueous chemistry of Sg and Bh Continuous, rapid, and efficient aqueous chemistry apparatus Low-background condition for α/sf detection 29

Experimental (1): RIKEN RI Beam Factory D2(10 o ) Q2 Q1 D1(45 o ) GARIS RILAC Chem. Lab. 30

RIKEN GARIS gas-jet system RIKEN GARIS Gas-jet transport system Differential pumping section Evaporation Beam from RILAC Residues (ERs) Beam dump Gas inlet Focal plane Mylar window 50 kpa ERs Rotating target 33 Pa Elastic scattering beam monitor D1 Q1 Q2 Haba et al., Chem. Lett. 38, 426 (2009). 0 D2 1 2 m He/KCl 0 100 mm By-products are removed almost completely. Production and decay studies of 265 Sg a,b and 266 Bh were successfully performed: 248 Cm( 22 Ne,5n) 265 Sg a,b Haba et al., Phys. Rev. C 85, 024611 (2012). 248 Cm( 23 Na,5n) 266 Bh Haba et al., APSORC 17, A-049 Pre-separated 265 Sg a,b and 266 Bh are ready for the chemistry experiments at GARIS. 31

Results and discussion (1): Production of Re isotopes Counts / 0.5 kev 10 5 10 4 10 3 10 2 10 1 Nuclide 109.1 176 Re 113.0 174 Re 123.2 172 Re 130.2 173 W 148? 181.5 173 Re 184.5 175 Re 190.7 173 Re 195? 196.9 177 Re 240.2 176 Re 243.4 174 Re 120 180 240 300 360 Bρ [Tm] γ-ray spectrum 253.9 172 Re Energy / kev Yield@Chem. Lab. [kbq/pμa min ] RUN: F07-1 Aerosol coll.: 60 s Cooling time: 60 s Meas. time: 60 s 349.5 174 Re, 351.2 176 Re 373.6 173 Re Gas-jet eff. [%] 174 Re 1.74±0.01 55±2 70±3 176 Re 1.76±0.01 16±1 76±2 Ref. Firestone and Shirley, Table of Isotopes, 8th ed., Wiley, New York, 1996. Counts per second Counts per second Decay curves of 174,176 Re 10 2 10 1 10 0 0 2 4 6 8 10 12 10 2 174 Re E γ = 243.4 kev T 1/2 = 2.3 ± 0.1 min Ref. 2.40 ± 0.04 min 176 Re E γ = 240.2 kev T 1/2 = 5.4 ± 0.2 min Ref. 5.3 ± 0.3 min 10 1 0 2 4 6 8 10 12 Elapsed time [min] 32

Results and discussion (1): Solvent extraction of Re isotopes D vs. Capillary length 10 0.5 M HNO 3 [TOA] = 0.01 M 174 Re MDG-FSE 176 Re MDG-FSE 181 Re Batch ext. Capillary length [cm] Chemical yield Chamber pressure [kpa] Chemical yield [%] 174 Re 176 Re D 1 0.1 0 20 40 60 80 100 Capillary length / cm 100 160 86 ± 5 97 ± 6 70 150 81 ± 7 91 ± 7 50 76 ± 13 85 ± 17 40 142 59 ± 21 65 ± 25 30 139 52 ± 13 56 ± 11 Extraction equilibrium of 174,176 Re is attained with the 30-cm capillary. Time required for solutions to pass through the capillary: ~1.8 s. Applicable for 10-s 266 Bh Chemical yields of 174,176 Re increase with increasing the capillary length and the pressure of the gas-jet chamber. 33

Experimental (1): Production of Re isotopes RIKEN GARIS Rotating nat Gd 2 O 3 target Elastic scattering beam monitor Differential pumping section 23 Na beam ERs ( 174 Re) from RILAC Beam dump D1 Q1 Q2 nat Gd( 23 Na,xn) 174 Re (T 1/2 = 2.4 min) Beam: 130.6-MeV 23 Na 7+, 0.33 pμa Target: 340 µg/cm 2 nat Gd 2 O 3 on 2-µm Ti GARIS Bρ: 1.58 1.94 Tm Irradiation room Gas inlet D2 0 Focal plane ERs 1 2 m 33 Pa Gas-jet transport system Mylar window: 0.7 µm 78 kpa He/KCl 0 100 mm 10 m He: 5 L/min Chem. Lab. Glass fiber filter (ADVANTEC GB-100R) γ-ray spectrometry nat Gd 2 O 3 target Gas-jet chamber 20-μm Al catcher γ-ray spectrometry 34

Experimental (1): Solvent extraction of Re isotopes GARIS gas-jet system Gas out H + + [ReO 4 ] + TOA [HReO 4 TOA] org. 174 Re He/KCl aerosols Membrane filter Organic phase () Teflon capillary (i.d. = 0.5 mm) Membrane filter γ-ray spectrometry Mylar window: 2.5 µm Irradiation room Aqueous solution () He: 1.5 L/min Chemistry laboratory Collection on glass fiber filter γ-ray spectrometry Distribution ratio, D = [A] org. /[A] aq. (A: radioactivities) Chemical yield, C.Y. = ([A] org. + [A] aq. ) 100/[A] glass fiber filter D vs. Capillary length D vs. [TOA] phase 0.5 M HNO 3 0.5 M HNO 3 phase 0.01, 0.1 M TOA / toluene 0.005 0.1 M TOA / toluene Capillary length (30), 40, (50), 70, 100 cm 40 cm Extraction equilibrium time, applicable D range 35

Results and discussion (2): Measurement of gas-jet transport, dissolution, and extraction times GARIS gas-jet system 170 Re He/KCl aerosols Membrane filter Gas out Chemistry laboratory Mylar window Irradiation room Extraction capillary (EC) i.d. = 0.5 mm L = 100 cm Phase separator (PS) He: 1.5 L/min 114 kpa 154 kpa 114 kpa 145 kpa 3.1 s 5.1 s 13.2 s 18.6 s 10.1 s (Calc. 4.4 s) 6.3 s (Calc. 5.9 s) 3.6 s (Calc. 3.1 s) 154 kpa 22.7 s Gas-jet chamber Aerosol collection apparatus Outlet of MDG Outlet of EC Outlet of PS 15

Results and discussion (2): Measurement of gas-jet transport, dissolution, and extraction times Net counts per 1 s Net counts per 1 s 300 200 100 Cumulative and differential time distribution of 170 Re Beam on (10 s) GARIS Aerosol Beam on (10 s) collection apparatus ΔT Net counts of 170 Re (305.7 kev) Run 1 (Accumulation and decay of radioactivity) Net counts of 170Re (305.7 kev) Fit with Fit with a "LogNormal lognormal function" Time distribution of 170Re Differential time distribution of 170 Re (arb. unit) Aerosol collection apparatus Net counts per 1 s Net counts per 1 s 200 150 100 50 ΔT GARIS Outlet of the MDG Run The 3 fitted experimental data were deconvoluted with Net counts of 170Re (305.7 kev) a response Fit with "LogNormal function function" Time distribution of 170Re exp( ln(2)*t/9.2) MDG + (5 + 20) cm capillary 0 0 0 10 20 30 40 50 60 70 80 Time since start of beam irradiation [s] Time since start of beam irradiation [s] 0 0 0 10 20 30 40 50 60 70 80 0 10 20 30 40 50 60 70 80 Time since start of beam irradiation [s] Time since start of beam irradiation [s] Average transport time (ΔT): time interval from a half of the irradiation time (5 s) to the time that gives 50% of the integral value of the differential time distribution of 170 Re 37

Continuous and rapid solvent extraction apparatus Development of a continuous and rapid solvent extraction apparatus coupled to the GARIS gas-jet system for aqueous chemistry of Sg and Bh GARIS gas-jet system He/KCl aerosols 265 Sg a,b, 266 Bh Membrane DeGasser (MDG) Gas out Flow Solvent Extractor (FSE) Membrane filter Organic phase () Membrane filter Photomultiplier tube Mylar window Irradiation room Aqueous solution () Chemistry laboratory Teflon capillary (i.d. = 0.5 mm) Phase separator Liquid scintillator Liquid scintillation α/sf detectors Continuous dissolution, solvent extraction, and radiation detection Minimization of decay loss of 265 Sg a,b and 266 Bh Efficient α/sf detection with LS: eff.(α-α/sf) = ~100% 38