Reflection asymmetry in the near spherical nucleus, 219Fr
Abstract
Mass separated sources of 223Ac (separated as AcF2+) were used to study the level structure of 219Fr following alpha decay. The levels in 219Fr are interpreted in terms of parity doublet bands which have a natural theoretical explanation in asymmetric models. The highly anomalous structure and other spectroscopic features of bands can be understood both in terms of reflection asymmetry and the collapse of the Nilsson orbitals towards spherical symmetry.
References (5)
- G.A. Leander et al.
Nucl. Phys.
(1984) - C.F. Liang
Cited by (9)
Incipient reflection asymmetry in <sup>127</sup>Xe
2023, Nuclear Physics AExcited states in 126,127,128Xe were populated via 122Sn(9Be, xnγ) fusion-evaporation reaction at a beam energy of 48 MeV. A positive parity rotational-like sequence of -transitions, which is found to decay into the negative parity band via E1 transitions, is observed above state at 2307 keV in 127Xe. Such enhanced E1 γ-transitions are also observed between the antimagnetic rotational (AMR) and longitudinal wobbling (LW) bands in this nucleus. These indicate the presence of simplex symmetry with excitation in 127Xe.
Nuclear Data Sheets for A=219
2021, Nuclear Data SheetsEvaluated experimental structure and decay data are presented for 12 known nuclides of mass 219 (Pb, Bi, Po, At, Rn, Fr, Ra, Ac, Th, Pa, U, Np). Recommended values are given for level parameters, γ and α radiations, and other spectroscopic information. No excited states are known in 219Bi, 219Po, 219Pa, 219U and 219Np. Except for isotopic identification, no information about its half-life or decay characteristics is available for 219Pb. For 219Po, several γ rays have been reported from the decay of 219Bi β− decay, but no level scheme has been proposed. For 219At, only four excited states are known from α decay of 223Fr. For 219Rn and 219Fr, only the low-spin states are known from α decays of 223Ra and 223Ac, respectively. For 219Ra, 219Ac and 219Th, mainly the data for high-spin states are available from in-beam γ-ray studies. For 219Ra, high-spin data are available from 2017He15, 1992Wi02 and 1987Co36, but evaluators find significant differences in relative photon branchings between the three studies. Detailed comments are given in the Adopted dataset for this nuclide. Half-lives of excited states are known only for seven levels in 219Rn, thus there is a general lack of knowledge about γ-ray transition probabilities. This work supersedes data in the previous evaluations of A=219 published by 2001Br31, 1992Br10 and 1977Ma30.
Nuclear data sheets for A = 215, 219, 233, 227, 231
2001, Nuclear Data SheetsThe evaluator presents in this publication spectroscopic data and level schemes from radioactive decay and nuclear reaction studies for all nuclei with mass numbers A=215, 219, 223, 227, and 231. Nuclei with mass number A=215 have spherical shape, and their nuclear structure have been interpreted in terms of the shell model. Nuclei with mass number A=219 belong to a transitional region with spherical, quadrupole, and possibly octupole deformations; those with mass numbers A=223 and 227 belong to a newly studied region of coexisting quadrupole with possible octupole deformations; and nuclei with mass number A=231 essentially have quadrupole deformation. Highlights of this publication are given below: A recent study of the 206Pb(13C,4nγ) reaction (1998St24) has extended up to Jπ=61/2+ the previously known level scheme from 208Pb(13C,6nγ) (1988Fu10,1983Lo16). This study has provided a new interpretation for all the spectroscopic data above the 2247--keV (Jπ=29/2--) level in 215Ra. A new isotope, 219U (42 μs), which was identified with the recoil separator VASSILISSA (1994Ye08,1994AnZY,1993An07), has been included in this evaluation. The first 223Rn β-- decay scheme (1992Ku03) and a significantly improved measurement of 227Ac α decay (1995Sh03) are presented here. A level scheme of 223Fr has been constructed on the basis of these studies, where most of the levels below 600 keV have been assigned to parity doublet bands and interpreted in terms of the reflection--asymmetric rotor model. This evaluation includes the first level structures of 227Fr and 227Th. Levels in 227Fr are from 227Rn β-- decay (1997Ku20); those in 227Th, are from 231U α decay, from 227Pa electron--capture decay, and from 226Ra(α,3nγ) (1997Mu08,1995Li04,1998Ma83). A study of the β-- decay of a mass--separated source of 231Fr has produced the first level scheme of 231Ra (2001Fr05). The only published data (1994Br36,1996Le01) on the electron--capture decay of 231U have provided much information on the level structure of 231Pa. Studies on 232Th(p,2nγ) and Coulomb Excitation of 231Pa (1996Le01,1999Wu05), which have complemented the existing spectroscopic data from these reactions, have suggested the possibility of weak octupole correlations in 231Pa. A new isotope of plutonium, 231Pu (1999La14), has been included in this evaluation.
Status report of the Leuven isotope separator on-line (LISOL)
1992, Nuclear Inst. and Methods in Physics Research, BThe mass separator LISOL, on-line to the CYCLONE cyclotron, is described as it is presently configured. The main development has been in the ion-guide operation in conjunction with light-ion induced fusion and fission. The plans to obtain intense (nA) beams of light (A ≤ 30), short-lived nuclei in the framework of the ARENAS3 project are also described.
Nuclear data sheets for A = 215,219,223,227
1992, Nuclear Data SheetsThis publication presents evaluated spectroscopic data and corresponding level schemes from radioactive decay and nuclear reaction studies for all nuclei with mass numbers A=215, 219, 223, and 227.
Nuclei with mass number A=215 have spherical shape, and their nuclear structure has been interpreted in terms of the shell model. Nuclei with mass number A=219 belong to a transitional region, with spherical, quadrupole, and possibly, octupole deformations, and those with mass numbers A=223 and 227, to newly studied regions of deformations (pure quadrupole coexisting with possible octupole). Because deformations are small in these regions, nuclear states are no longer fully characterized by single Nilsson orbitals. This terminology, however, is used throughout this evaluation to label states rather than to accurately describe their nature.
Highlights of this publication include the emission of 14C by 223Ra, discovered by Rose and Jones (84Ro30), and its fine structure, measured by Brillard et al. (89Br34). This constitutes a new mode of decay and provides additional arguments for configuration assignments. They further include the first set of nuclear levels in 215Fr, 215Ra, and 215Ac, determined from in—beam γ-ray spectroscopic measurements.
Two major publications have been extensively used in this evaluation: the theoretical paper “Reflection—asymmetric Rotor Model of Odd—A ≈219–229 Nuclei” by Leander and Chen (88Le13), which presents a calculation of single—particle state properties by the coupling of shell—model states to a reflection—asymmetric rotor core; and the review paper “Intrinsic States of Deformed Odd—A Nuclei in the Mass Regions (151≤A≤193) and (A≥221)” by Jain et al. (90Ja11), which gives the systematics and assignments of single—particle states in such mass regions.
These evaluations for A=215, 219, 223, and 227 supersede the earlier ones by C. Maples: 77Ma29, Nuclear Data Sheets 22, 207 (1977); 77Ma30, Nuclear Data Sheets 22, 223 (1977); 77Ma31, Nuclear Data Sheets 22, 243 (1977); and 77Ma32, Nuclear Data Sheets 22, 275 (1977).
Single-particle states and parity doublets in odd- Z Ac 221 and Pa 225 from α -decay spectroscopy
2022, Physical Review C