The Predicted and Observed Properties of Eka
Transcription
The Predicted and Observed Properties of Eka
Nuclear Structure of Actinide and Transactinide Elements Irshad Ahmad Argonne National Laboratory September 11, 2011 Superheavy Elements • Lanthanides (Rare Earths): La (Z = 57) to Lu (Z = 71) Filling of 4f shell …. 14 elements • Actinides: Ac (Z = 89) to Lr (Z = 103) Filling of 5f shell …. 14 elements • Transactinide Elements: Elements Rf (Z = 104) and beyond • Superheavy Elements: Definition not as definite Elements around Z = 114 Discovery of Transuranium Elements 1940-1955 Berkeley Np (Z = 93) – Md (Z = 101) Actinide targets + d or alpha 60-inch cyclotron Identification: Chemical separation 1960’s Dubna/Berkeley No (Z = 102) – Sg (Z = 106) Heavy-ion beams on actinide targets Identification; Decay chain 1980-1990 GSI, Germany Bh(Z = 107) – Cn (Z = 102) Cold fusion, 208Pb/209Bi targets + HI beams Identification: Decay chain to known isotope 2004 Riken, Japan Z=113 , 209Bi+HI beam Identification: Decay chain 2000’s Dubna, Russia Z = 114 – Z = 118 Hot fusion, actinide targets + 48Ca beam Identification: Decay chain; end product unknown isotope Half lives of the longest-lived isotopes of actinides Atomic Radii Atomic Radii Atomic ionization energy Nuclear energy levels Total Energy E(β) = ELDM(β) + u(β) + P(β) p,n Shell Correction u(β) = u – ũ u = 2 – single-particle energy – pair occupation probability ũ = 2 g()d g() – uniform distribution of nuclear states – chemical potential N = 2 g()d N = total number of particles GSI, Germany Linac + Ship Discovered element 107-112 Example: Hassium (Z = 108), 1995 208Pb 265Hs + 58Fe 265Hs + n separated from the beam and other reaction products Using recoil separator SHIP Alpha counted 265Hs and its daughter Dubna, Russia, Cyclotron Discovered element Z = 114-118 48Ca beam plus actinide targets Example: Element 117 249Bk + 48Ca 294 X 117 +3n Measured alpha decay energy and fission followed the decay chain Final isotope not known Phys. Rev. Lett. 104, 142502 (2010) 255Fm nucleus R j Symmetry Axis Wp[NnzLS] e.g. 7/2+[613] W odd-mass K+3 6+ K+2 K+1 K 4+ for j=9/2 W=1/2, 3/2, 5/2, 7/2 and 9/2 2+ 0+ even-even protons neutrons Differential Cross Sections in (d,p) reactions on deformed nuclei dσ/dΩ = 2N u2KCjK2ΘDW with u2K= 1 - v2K; v2K= pair occupation probability; CjK= the expansion coefficient of the wavefunction ψK= ΣjCjKΦjK ΘDW = DWBA cross section N=normalization constant ΣCjK2 = 1 and CjK2 = dσ/dΩ /(k ΘDW) Cjk2 for Neutron Single-Particle States above N=152 Chasman (1990) State K j 1/2 3/2 5/2 7/2 9/2 11/2 13/2 0.041 0.209 0.216 0.238 0.133 0.030 0.003 0.843 0.102 0.049 0.358 0.161 0.196 0.024 9/ 2+[615] 0.069 0.914 0.016 9/ 2+[604] 0.910 0.076 0.009 1/ 2+[620] 0.131 7/ 2+[613] 3/ 2+[622] 0.168 0.091 October Issue T1/2=0.9 ms 294118 T1/2=1.0 ms Summary Use of decay data and one-nucleon transfer reaction data have enabled us to determine the single-particle energies and wavefunctions in very heavy actinide nuclei. – Neutron orbitals up to N=162 identified – Proton orbitals up to Z=101 identified The single-particle energies and wavefunctions are reproduced by a singleparticle model calculation using a deformed Woods-Saxon potential. Acknowledgement This work was supported by the U.S. Department of Energy, Office of Nuclear Physics, under contract No. DE-AC-02-06CH11357. Participants I. Ahmad, F.G. Kondev, M. P. Carpenter, R. R. Chasman, J. P. Greene, E.F. Moore, R. V. F. Janssens, T. Lauritsen, C. J. Lister, and D. Seweryniak Discovery of the First Transuranium Element - Neptunium Irshad Ahmad Argonne National Laboratory September 12, 2011 Mendeleeff’s Table I.-1871 Series Group I. R2 O Group II RO Group III R2O3 Group IV RH4 RO2 Group V RH3 R2O6 Group VI RH2 RO3 Group VII RH R2O7 1….. H=1 2….. Li=7 Be=9.4 B=11 C=12 N=14 O=16 F=19 3….. Na=23 Mg=24 Al=27.3 Si=28 P=31 S=32 Cl=35.5 4….. K=39 Ca=40 -=44 Ti=48 V=51 Cr=52 Mn=55 5….. (Cu=63) Zn=65 -=68 -=72 As=75 Se=78 Br=80 6….. Rb=85 Sr=87 Y=88 Zr=90 Nb=94 Mo=96 -=100 7….. (Ag=108) Cd=112 In=113 Sn=118 Sb=122 Te=125 I=127 8….. Cs=133 Ba=137 Di=138 Ce=140 …. …. …. …. 9….. …. …. …. …. …. …. …. …. 10….. …. …. Er=178 La=180 Ta=182 W=184 …. Hg=200 Tl=204 Pb=207 Bi=208 …. …. ….. …. Th=231 …. U=240 …. 11….. 12….. (Au=199) …. Group VIII RO4 Fe=56,Ce=59, Ni=59, Cu=63 Ru=194, Rh=104, Pd=106, Ag=108 Os=195, In=197, Pt, 198, Au=199 ….. 33 The Predicted and Observed Properties of Eka-silicon (Germanium) Property Relative atomic mass Eka-silicon 1871 prediction Germanium discovered 1886 72 72.32 Specific gravity Specific heat 5.5 0.073 Atomic volume Color 13 cm3 Dark gray 5.47 0.076 13.22 cm3 Grayish white • • • 1932 Neutron discovered by Chadwick 1934 Artificial radioactivity discovered by I. Curie and F. Joliet 1934/35 Fermi irradiated more than 50 elements with neutrons Ra + Be ~107 n/s For each element, n capture made beta unstable isotope which decayed to the next element with one more proton For example: 197Au + n 198Au (2.7 d) 198Hg So U + n should produce element with Z = 93 238U + n 239U 239Np In the irradiation of U Fermi observed activities with 239Np half-life = 2.3 days Half-life = 40 s, 1 min, 15 min, 90 min Performed chemical separation with the 15-min activity. It was carried with Mn. So it was Re-like as expected for Np. Now we know that what Fermi saw was 14.3-min 101Tc. So Fermi saw no Np at all!! Lawrence at Berkeley 1931 4.5 inch cyclotron 80 keV 11 inch cyclotron 1.2 MeV 1936 27 inch cyclotron 6 MeV d 1937 37 inch cyclotron 8 MeV d 1939 60 inch cyclotron 22 MeV d 8 MeV d + Be • 16 MeV d + Be gives 1011 n/s/microampere • This is 10,000 times neutron production with Ra + Be Medical Use: 131I gives 1010 neutrons/s/microampere • (8 d) , 59Fe (45 d), 99Tc (6 hr), 60Co (5.3 yr) History of the discovery of Neptunium • 1939 Fission discovered. This showed Fermi’s discovery of element 93 was wrong • 1939 McMillan: thin U + neutrons from 37-inch cyclotron. Fission fragments recoiled out of the target. Two activities remained in the target. Half-life = 23 min; Hahn showed it to be 239U in 1937. So, 2.3-d activity, most likely Z = 93 • 1939 Segre performed chemical separation. Chemistry not like Re so, no element 93 Chemistry more like Rare earths • 1940 McMillan and Abelson: chemistry Chemistry like U, different from any known element. Showed 2.3-d activity grew with the half-life of 239U (23 min) So, it is Z = 93, named neptunium Discovery of Neptunium Chemical separation by McMillan and Abelson showed that: • Element 93 (Np) is not like Re • It is like U and Rare earth • Thus Np should be part of actinide series (5f) • This concept was further developed by Seaborg • So, now they had predictions of chemical properties of elements beyond neptunium (Np) Discovery of Element with Z = 101, Md • Chemistry of Lanthanides showed what the chemistry of Md would be like • On a cation-exchange resin column it would elute before Fm. • Experiment: only 109 atoms of 253Es available (1 picogram) 253Es • + 4He 256Md + n Collect the recoils, dissolved in acid and loaded on a But column Md separated Only 5 atoms identified Chemistry behaved perfect! Phys. Rev. 98, 115 (1955) Acknowledgement This work was supported by the U.S. Department of Energy, Office of Nuclear Physics, under contract No. DE-AC02-06CH11357.