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Chemistry of the Heaviest Elements
Yuichiro Nagame1,2
1Advanced Science Research Center, JAEA 2Graduate School of Science & Engineering, Ibaraki Univ.
6th Asian-Pacific Symposium on
Radiochemistry
September 17-22, 2017, Jeju Island, Korea
JAEA Tokai
2
1 18
1 2
2 13 14 15 16 17
3 4 5 6 7 8 9 10
11 12 13 14 15 16 17 18
3 4 5 6 7 8 9 10 11 12
19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36
37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54
55 56 57 72 73 74 75 76 77 78 79 80 81 82 83 84 85 86
87 88 89 104 105 106 107 108 109 110 111 112 113 114 115 116 117 118
57 58 59 60 61 62 63 64 65 66 67 68 69 70 71
89 90 91 92 93 94 95 96 97 98 99 100 101 102 103
Es FmPa U Np MdPu
Sm GdCe Tm
No LrAm BkCm CfAc ThActinides
YbLa Pr Nd PmLanthanides
DsHsDb Sg BhFr Ra Ac Rf
PdRh
Lu
Mt
Tb Dy Ho ErEu
Rg Lv
Os Ir Pt Au
Nh McCn Fl
Re RnHg Tl Pb Bi AtPoCs Ba La
MoNbZrY
Ta WHf
As
Sr
Br Kr
Rb XeITeSbSn
V
Cd
Mn Fe Co Ge
InRuTc Ag
He
Be B NeF
Se
NC
Cl ArP
Cr
H
Li
Na Mg
K Ca Sc Ti
S
O
Ts Og
Al
Ni Cu Zn Ga
Si
Transuranium elements : Z ≥ 93
Transactinide elements: Z ≥ 104
The heaviest elements: The elements with Z ≥ 101 that are produced only
in heavy-ion-induced nuclear reactions.
The heaviest elements
one atom-at-a-time
3
Naming four new elements
nihonium and symbol Nh, for the element 113
moscovium and symbol Mc, for the element 115
tennessine and symbol Ts, for the element 117
oganesson and symbol Og, for the element 118
Talk by S. Dmitriev (IA-508)
4
Searching for and producing new elements and their chemical / physical
(nuclear) characterization are very challenging subjects in recent advanced
nuclear & radiochemistry.
• How many chemical elements may be synthesized on earth?
• How can they be produced?
• How long can they survive?
• Which properties do determine their stability?
• What are their chemical and physical properties?
• How are the orbital electron configurations affected in the strong
electric field of heavy atoms?
These are the most fundamental questions in science.
Impact on science
Yu. Ts. Oganessian & K. P. Rykaczewski,
Phys. Today, August 2015, p. 32
5
Contents
1. Introduction:
Chemical studies of the heaviest elements
▶ Atom-at-a-time chemistry
▶ Relativistic effects on electronic structure
2. Recent highlighted studies of liquid-phase chemistry
2-1. Complex formation of 104Rf
2-2. Electrochemistry of 101Md & 102No
3. Atomic properties of the heaviest actinides
3-1. Ionization energy of 103Lr
4. Summary & perspectives
JAEA Tandem Accelerator
6
1. Introduction
Objectives:
Chemical studies of the heaviest elements provide crucial & challenging
opportunities
▶ to advance our understanding of properties of matter at the limits of
existence
▶ to elucidate the influence of relativistic effects on atomic electrons
▶ to architect the Periodic Table at the farthest reach
The heaviest elements (Z > 100):
▶ available in quantities of only a few atoms or often one atom-at-a-time
Chemical characterization with an atom-at-a-time scale:
⇒ Extreme Chemistry
7
1. Introduction
Chemical properties:
▶ complex formation abilities
▶ oxidation states & redox potentials
▶ valence electronic states, etc.
⇒ role of relativistic effects on valence electronic structure
of heavy atoms
1. Relativistic effects
2. Atom-at-a-time chemistry
8
Relativistic effects (1)
General: relativity - increase of the mass with increasing velocity
At heavy elements: Increasing nuclear charge plays as the “accelerator”
of the velocity of electrons.
Electrons near the nucleus are attracted closer to the nucleus and move
there with high velocity.
mass increase of the inner electrons and the contraction of the inner
electron orbitals (Bohr radius)
1. Direct relativistic effects
9
Electrons further away from the nucleus are better screened from the
nuclear charge by the inner electrons, and consequently the orbitals of
the outer electrons expand.
2. Indirect relativistic effects
3. Spin-orbit (SO) splitting of levels with l > 0 into two levels with
j = l ± 1/2
It is expected that the heaviest elements would show a drastic
rearrangement of electrons in their atomic ground states, and as the
electron configuration is responsible for the chemical behavior of elements,
such relativistic effects can lead to surprising chemical properties.
Increasing deviations from the periodicity of chemical properties
based on extrapolation from lighter homologues in the Periodic Table
are predicted.
Relativistic effects (2)
10
Cracks in the Periodic Table
E. Scerri, Scientific American, June 2013, p. 68
…..table may be losing its power due to relativistic effects.
11
Typical production rates of the heaviest
nuclides used for chemical studies
Z Nuclide T1/2 Reaction σ / nb Production
rate*
101 255Md 27 min 248Cm(11B, 4n) 4000 1380 min-1
102 255No 3.5 min 248Cm(12C, 5n) 580 200 min-1
103 256Lr 27 s 249Cf(11B, 4n) 122 40 min-1
104 261Rf 68 s 248Cm(18O, 5n) 13 4 min-1
105 262Db 35 s 249Bk(18O, 5n) 6 2 min-1
106 265Sg 14 s/9 s 248Cm(22Ne, 5n) 0.38 6 h-1
107 267Bh 17 s 249Bk(22Ne, 4n) 0.07 2 h-1
108 269Hs 10 s 248Cm(26Mg, 5n) 0.007 3 d-1
112 283Cn 4 s 242Pu(48Ca, 3n)287Fl
→283Cn
0.004 2 d-1
* Assuming typical values of 0.8 mg/cm2 for the target thickness and beam intensities
of 3 x 1012 particles per second.
12
Atom-at-a-time chemistry
Because of the short half-lives and the low production rates of
the heaviest nuclides, each atom produced decays before a
new atom is synthesized.
Any chemistry to be performed must be done on an "atom-at-
a-time" basis.
This imposes stringent limits on experimental procedures.
Rapid and very efficient radiochemical procedures must be
devised.
13
Atom-at-a-time experiments
1. Gas-phase chemistry:
▶ Thermochromatography
▶ Isothermal chromatography
Talk by A. Türler (IA-518)
2. Liquid-phase chemistry:
▶ Liquid-liquid extraction
▶ Ion-exchange chromatography
▶ Reversed-phase extraction chromatography
▶ Redox chromatography
14
▶ Chemical properties of element 106 (seaborgium)
M. Schädel et al, Nature 388, 55 (1997).
▶ Chemical characterization of bohrium (element 107)
R. Eichler et al., Nature 407, 63 (2000).
▶ Chemical investigation of hassium (element 108)
Ch. E. Düllmann et al., Nature 418, 859 (2002).
▶ Chemical characterization of element 112
R. Eichler et al., Nature 447, 72 (2007).
▶ Synthesis and detection of a seaborgium
carbonyl complex
J. Even et al., Science 345, 1492 (2014).
▶ Measurement of the first ionization
potential of lawrencium, element 103
T. K. Sato et al., Nature 520, 209 (2015).
▶ Atom-at-a-time laser resonance ionization
spectroscopy of nobelium
M. Laatiaoui et al., Nature 538, 495 (2016).
Highlighted chemical studies
15
Nucl. Phys. A
944, 1-690 (2015)
Special Issue on
Superheavy Elements
Edited by
Christoph E. Düllmann,
Rolf-Dietmar Herzberg,
Witold Nazarewicz and
Yuri Oganessian
Recent review articles
Chem. Rev. 113, 1237-1312 (2013)
(2014)
M. Schädel and D. Shaughnessy. Eds
16
Presentation in APSORC2017
Overview
A. Türler (IA-518): A postcard from the island of stability: what’s new in superheavy
element chemistry
Production & Nuclear reaction mechanism
J. V. Kratz (A-036): Radiochemical investigation of the kinematics of multi-nucleon
transfer reactions in 48Ca + 248Cm collisions 10% above the
Coulomb barrier
H. Haba (A-079): Production and decay studies of 261Rf, 262Db, 265Sg, and 266Bh for
superheavy element chemistry at RIKEN GARIS
17
Presentation in APSORC2017
Liquid-phase chemistry
Y. Komori (A-078): Development of a rapid solvent extraction apparatus coupled to
the GARIS gas-jet transport system to aqueous chemistry of the
heaviest elements
Gas-phase chemistry & atomic properties
T. Tomitsuka (A-209): Adsorption of lawrencium (Z = 103) on a Ta surface
N. M. Chiera (A-160): Unexpected transport to the cryo-on-line-detector COLD)
setup of a volatile At species
K. Shirai (A-035): Influence of surface condition of quartz column for gas
chromatographic behavior of ZrCl4 and HfCl4
Y. Nagame (A-259): First ionization energies of heavy actinides
Development of new innovative apparatuses !
18
2. Recent liquid-phase chemistry
Atom-at-a-time chemistry:
To get statistically significant results with single atoms, it is indispensable to repeat the
same experimental procedure several hundred or even several thousand times with
cycle times of about the lifetime of the nuclide under investigation.
The behavior of the heaviest elements is compared with that of its lighter homologs
under identical conditions.
Extensive series of detailed investigations have been made possible by the
development of computer-controlled automated systems that have greatly
improved the ability
▶ to perform rapidly and reproducibly large numbers of chemical (chromatographic)
separations on miniaturized columns and
▶ to systematically vary ligand concentrations, thus allowing determining the
stoichiometry of the eluted species: Kd vs. [ligand].
The experiments with automated devices have produced detailed and
sometimes surprising results that called for a detailed theoretical modeling of
the chemical properties with improved quantum-chemical calculations.
19
Recent highlighted liquid-phase chemistry
2-1. Complex formation of 104Rf
- Fluoride complex formation of Rf
complex formation abilities
2-2. Electrochemistry of 101Md & 102No
- Redox reactions of Md & No
oxidation states & redox potentials
20
Experiments with Rf in the liquid-phase
1. Production of a specific heaviest nuclide
2. Rapid transport of this nuclide to chemical separation devices
3. Fast chemical characterization that includes dissolution in an aqueous solution
containing inorganic/organic ligands for complex formation
4. Preparation of a sample
suitable for α-spectroscopy
5. Detection of nuclides
through their characteristic
nuclear decay properties
for unambiguous
identification
Automated rapid chemistry apparatuses
ARCA II and AIDA
The automated rapid
chemistry apparatuses
ARCA II and AIDA enable
cyclic column
chromatographic separation.
21 21
Eluent bottles
Ta disk reservoir
Micro-columns
He gas heater Halogen lamp
Sampling table
Air cylinder
Pulse motors Signal out
8 vacuum chambers
600 mm2 PIPS detectors
Preamp.
He/KCl gas-jet
Cyclic discontinuous column chromatographic separation of short-lived nuclides &
automated detection of α-particles within a typical cycle time of 60 s
ARCA II
AIDA: Automated Ion-exchange separation apparatus coupled
with the Detection system for Alpha-spectroscopy
23
2-1. Fluoride complex formation of Rf
248Cm(18O, 5n)261Rf (T1/2 = 68 s) : σ = 13 nb
Experimental approach should involve detailed comparison of the chemical
properties of the heaviest elements with those of their lighter homologues
under identical conditions.
1 18
1 2
2 13 14 15 16 17
3 4 5 6 7 8 9 10
11 12 13 14 15 16 17 18
3 4 5 6 7 8 9 10 11 12
19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36
37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54
55 56 57 72 73 74 75 76 77 78 79 80 81 82 83 84 85 86
87 88 89 104 105 106 107 108 109 110 111 112 113 114 115 116 117 118
57 58 59 60 61 62 63 64 65 66 67 68 69 70 71
89 90 91 92 93 94 95 96 97 98 99 100 101 102 103
Es FmPa U Np MdPu
Sm GdCe Tm
No LrAm BkCm CfAc ThActinides
YbLa Pr Nd PmLanthanides
DsHsDb Sg BhFr Ra Ac Rf
PdRh
Lu
Mt
Tb Dy Ho ErEu
Rg Lv
Os Ir Pt Au
Nh McCn Fl
Re RnHg Tl Pb Bi AtPoCs Ba La
MoNbZrY
Ta WHf
As
Sr
Br Kr
Rb XeITeSbSn
V
Cd
Mn Fe Co Ge
InRuTc Ag
He
Be B NeF
Se
NC
Cl ArP
Cr
H
Li
Na Mg
K Ca Sc Ti
S
O
Ts Og
Al
Ni Cu Zn Ga
Si
24
Fluoride complex formation of Rf
John Emsley,
in NATURE’S BUILDING
BLOCKS, Oxford 2011
Rutherfordium: Element of surprise
▶ Rutherfordium is not like the higher member of group 4 in
its behavior with fluoride ions.
▶ Like hafnium and zirconium, it forms a complex ion with six
fluorides: RfF62- but it does not form RfF7
3- whereas the
other two metals do.
▶ The reason appears to be that relativistic effects are
coming into play and these affect the behavior of its
bonding electrons.
H. Haba et al., J. Am. Chem. Soc.
126, 5219 (2004).
25
2-2. Electrochemistry of Md & No
Redox studies of the heaviest elements are expected to give valuable
information on valence electronic states influenced by strong relativistic
effects, such as oxidation states & redox potentials.
Reduction of 101Md : Md3+ Md2+
Oxidation of 102No : No2+ No3+
248Cm(11B, 4n)255Md (T1/2 = 27 min)
248Cm(12C, 5n)255No (T1/2 = 3.1 min)
• Development of a rapid electrochemical
apparatus
• Redox reactions with an atom-at-a-time
technique
Solution
26
Flow electrolytic column chromatography
26
Working electrode
(Glassy carbon fibers) Reference
electrode
(Ag/AgCl)
Carbon rod
Inlet
Md3+
Md3+
Carbon fiber
Md2+
e- e-
Flow
Counter
electrode
(Pt)
Outlet
Md2+
Rapid & effective redox reactions
Electrolyte solution: 0.1 M HCl
A. Toyoshima et al.,
Radiochim. Acta 96, 323-326 (2008).
▶ Both electrochemical and cation-exchange reactions in the column
▶ Different cation-exchange behavior between the different oxidation
states
Cation-exchanger (Nafion)
27
Redox reactions of Md & No
0
20
40
60
80
100
120
-1.5 -1 -0.5 0 0.5
Reduction p
robabili
ty / %
Applied potential / V
0
20
40
60
80
100
120
-0.5 0 0.5 1 1.5
Oxid
atio
n p
rob
abili
ty /
%
Applied potential / V
▶ Redox reactions based on an atom-at-a-time scale were successfully
conducted with the newly developed flow electrochemical apparatus.
▶ This new technical approach will open up new frontiers of the
chemistry of the transactinide elements.
A. Toyoshima et al.,
Inorg. Chem. 52, 12311-12313 (2013).
A. Toyoshima et al.,
J. Am. Chem. Soc. 131, 9180-9181 (2009).
No2+ ⇄ No3+ + e- Md3+ + e- ⇄ Md2+
Eu3+ +e- ⇄ Eu2+
28
3. Atomic properties of the heaviest actinides
Study of atomic properties of the heaviest elements is indispensable to
understand electronic ground state configurations.
The first ionization potential/energy (IP1) is an atomic property which most
sensitively reflects the outermost electronic configuration.
Precise and accurate determination of IP1 provides significant information on
the binding energy of the valence electrons and, thus, on increasingly strong
relativistic effects.
Inner electron orbital
Expansion
Nucleus
Outer electron orbital
Electron
Contraction
29
3-1. First ionization energy (IP1) of Lr
Cover of Nature:
9 April 2015
EXTREME
CHEMISTRY
Experiments on rare lawrencium
atoms illuminate a relativistic
region of the periodic table
30
Valence electronic structure of Lr
The ground-state electronic configuration of Lr is predicted to be [Rn]5f147s27p1/2, in
contrast to that of its lanthanide homolog Lu, [Xe]4f146s25d, as the7p1/2 orbital is
expected to be stabilized below the 6d orbital in Lr by strong relativistic effects.
The determination of IP1 sheds light on the important role of relativistic effects on the
electronic structure of heavy elements.
Lr: [Rn]5f147s27p1/2
Lu: [Xe]4f146s25d
No IP1 data beyond Es
(Z = 99)
⇒ New “atom-at-a-time”
technique
1 18
1 2
2 13 14 15 16 17
3 4 5 6 7 8 9 10
11 12 13 14 15 16 17 18
3 4 5 6 7 8 9 10 11 12
19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36
37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54
55 56 57 72 73 74 75 76 77 78 79 80 81 82 83 84 85 86
87 88 89 104 105 106 107 108 109 110 111 112 113 114 115 116 117 118
57 58 59 60 61 62 63 64 65 66 67 68 69 70 71
89 90 91 92 93 94 95 96 97 98 99 100 101 102 103
S
O
Ts Og
Al
Ni Cu Zn Ga
Si P
Cr
H
Li
Na Mg
K Ca Sc Ti
He
Be B NeF
Se
NC
Cl Ar
V
Cd
Mn Fe Co Ge
InRuTc Ag
As
Sr
Br Kr
Rb XeITeSbSn
Cs Ba La
MoNbZrY
Ta WHf Re RnHg Tl Pb Bi AtPo
Lv
Os Ir Pt Au
Nh McCn Fl
PdRh
Lu
Mt
Tb Dy Ho ErEu
Rg
Lanthanides
DsHsDb Sg BhFr Ra Ac Rf
Ac ThActinides
YbLa Pr Nd Pm Sm GdCe Tm
No LrAm BkCm Cf Es FmPa U Np MdPu
⇒ the heaviest
element ion beams
31
Valence electronic structure of Lr
The ground-state electronic configuration of Lr is predicted to be [Rn]5f147s27p1/2, in
contrast to that of its lanthanide homolog Lu, [Xe]4f146s25d, as the7p1/2 orbital is
expected to be stabilized below the 6d orbital in Lr by strong relativistic effects.
The determination of IP1 sheds light on the important role of relativistic effects on the
electronic structure of heavy elements.
Lr: [Rn]5f147s27p1/2
Lu: [Xe]4f146s25d
No IP1 data beyond Es
(Z = 99)
⇒ New “atom-at-a-time”
technique
1 18
1 2
2 13 14 15 16 17
3 4 5 6 7 8 9 10
11 12 13 14 15 16 17 18
3 4 5 6 7 8 9 10 11 12
19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36
37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54
55 56 57 72 73 74 75 76 77 78 79 80 81 82 83 84 85 86
87 88 89 104 105 106 107 108 109 110 111 112 113 114 115 116 117 118
57 58 59 60 61 62 63 64 65 66 67 68 69 70 71
89 90 91 92 93 94 95 96 97 98 99 100 101 102 103
S
O
Ts Og
Al
Ni Cu Zn Ga
Si P
Cr
H
Li
Na Mg
K Ca Sc Ti
He
Be B NeF
Se
NC
Cl Ar
V
Cd
Mn Fe Co Ge
InRuTc Ag
As
Sr
Br Kr
Rb XeITeSbSn
Cs Ba La
MoNbZrY
Ta WHf Re RnHg Tl Pb Bi AtPo
Lv
Os Ir Pt Au
Nh McCn Fl
PdRh
Lu
Mt
Tb Dy Ho ErEu
Rg
Lanthanides
DsHsDb Sg BhFr Ra Ac Rf
Ac ThActinides
YbLa Pr Nd Pm Sm GdCe Tm
No LrAm BkCm Cf Es FmPa U Np MdPu
⇒ the heaviest
element beams
Y. Nagame,
Nature Chem. 8, 282 (2016)
32
Experimental set-up
Complex system: surface ionization, mass separation and detection of Lr ions
249Cf target
11B beam
Gas-jet transport
Skimmer
Ionization
cavity Extraction
electrode
Ion source
α-particle
detector
T. K. Sato et al.
Nature 520, 209 (2015)
Mass separation
Lr atoms are ionized to the +1 charge state via the
interaction with a solid metal surface at high temperature
and is selectively mass-separated from nuclear reaction
by-products.
249Cf(11B, 4n)256Lr
33
First ionization energy (IP1) of Lr
IP / eV
Exp. 4.96 ± 0.08
Cal. 4.963*
The good agreement with theoretical prediction
obtained using relativistic calculations, which
favor a 7s27p1/2 configuration in the Lr atom,
supports this ground state configuration.
This quantitatively reflects and confirms the theoretically predicted situation of
closed 5f14 and 7s2 shells with an additional weakly-bound electron in the
valence orbital. ⇒ Lr: last actinide ⇒ actinide series in the Periodic Table
Lanthanides
Actinides
34
5. Summary & Perspectives
Liquid-phase chemistry
▶ Surprising chemical properties of Rf (and 105Db)
▶ Heavier elements:
New technical development: Continuously working system consisting
of a rapid chemical separation device and a flow-through α-particle
detection apparatus, coupled to a recoil pre-separator
Talk by Y. Komori (A-078)
New approach with the heaviest element (ion) beams
▶ IP1 Talk by Y. Nagame (A-259)
▶ Adsorption behavior of Lr Talk by T. Tomitsuka (A-209)
▶ Ion beams, Atomic & Molecular beams New frontier chemistry