References quoted in the ENSDF dataset: 191AU ADOPTED LEVELS, GAMMAS
41 references found.
Clicking on a keynumber will list datasets that reference the given article.
Phys.Rev. 93, 124 (1954)
L.P.Gillon, K.Gopalakrishnan, A.deShalit, J.W.Mihelich
Nuclear Spectroscopy of Neutron Deficient Hg Isotopes
Phys.Rev. 98, 1258 (1955)
W.G.Smith, J.M.Hollander
Radiochemical Study of Neutron-Deficient Chains in the Noble Metal Region
Phys.Rev. 120, 1406 (1960)
W.B.Ewbank, L.L.Marino, W.A.Nierenberg, H.A.Shugart, H.B.Silsbee
Nuclear Spins of Six Neutron-Deficient Gold Isotopes
NUCLEAR STRUCTURE 194Au, 195Au, 192Au, 193Au, 191Au, 196Au; measured not abstracted; deduced nuclear properties.
J.Inorg.Nuclear Chem. 17, 15 (1961)
G.Andersson, I.B.Haller, R.Ringh
Thallium Isotopes 192 and 193
NUCLEAR STRUCTURE 193Tl, 192Tl; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(61)80180-2
Arkiv Fysik 23, 57 (1963)
M.Karras, G.Andersson, M.Nurmia
Search for Alpha Activity in Neutron Deficient Isotopes of Pb, Tl, Hg, Pt, and Te
NUCLEAR STRUCTURE 119Te, 117Te, 116Te, 118Te, 198Bi, 198Tl, 198Pb, 197Pb, 196Bi, 196Pb, 194Tl, 195Tl, 193Hg, 193Au, 192Hg, 193Tl, 192Au, 190Hg, 191Hg, 191Au, 189Hg, 190Au, 189Au; measured not abstracted; deduced nuclear properties.
Phys.Rev. 135, A358 (1964)
W.B.Ewbank, H.A.Shugart
Hyperfine-Structure Separations of Au191 and Au193
NUCLEAR STRUCTURE 193Au, 191Au; measured not abstracted; deduced nuclear properties.
Nucl.Phys. A98, 278 (1967)
A.Johansson, B.Nyman, G.Malmsten, S.-E.Karlsson
The Decay of 191Au and the Level Scheme of 191Pt
RADIOACTIVITY 191Au [from pt(p, xn)]; measured T1/2, Eγ, I(ce), (ce)(ce)- coin. 191Pt deduced levels, J, π. Natural target.
doi: 10.1016/0375-9474(67)90140-6
Z.Phys. 247, 383 (1971)
H.Beuscher, P.Jahn, R.M.Lieder, C.Mayer-Boricke
Electron Capture Decay of 51 min 191Hg
RADIOACTIVITY 191mHg; measured Eγ, Iγ, I(ce), T1/2, γγ-coin, ceγ-coin, ceγ-delay. 191Au deduced levels, J, π, ICC, γ-multipolarity, T1/2.
Nucl.Phys. A231, 397 (1974)
P.O.Tjom, M.R.Maier, D.Benson, Jr., F.S.Stephens, R.M.Diamond
High-Spin States in 191,193,195Au
NUCLEAR REACTIONS 190,192Os(7Li, xnγ), E=50, 58 MeV; 191,193Ir(α, xnγ), E=26, 29, 42 MeV; measured Eγ, Iγ, γγ-coin, γγ(t), γ(θ). 191,193,195Au deduced levels, J, π. Enriched targets; Ge(Li) detectors.
doi: 10.1016/0375-9474(74)90504-1
Phys.Lett. 58B, 159 (1975)
E.F.Zganjar, J.L.Wood, R.W.Fink, L.L.Riedinger, C.R.Bingham, B.D.Kern, J.L.Weil, J.H.Hamilton, A.V.Ramayya, E.H.Spejewski, R.L.Mlekodaj, H.K.Carter, W.D.Schmidt-Ott
Rotation-Aligned Coupling and Axial Asymmetry in 189-195Au
RADIOACTIVITY 189,189m,191,191m,193Hg; measured γγ(t), γ X-ray(t), Eγ, Iγ, I(ce); deduced ICC. 189,191,193Au deduced levels. 189,191,193,195Au deduced systematics.
doi: 10.1016/0370-2693(75)90627-9
Phys.Rev.Lett. 37, 1123 (1976)
Y.Gono, R.M.Lieder, M.Muller-Veggian, A.Neskakis, C.Mayer-Boricke
Blocking Effect in the Transitional Nuclei 189,191,193Au
NUCLEAR REACTIONS 191,193Ir(α, 4nγ), (α, 6nγ), E=51, 77 MeV; measured in-beamγ. 189,191,193Au deduced levels, K, T1/2, λ, J, π.
doi: 10.1103/PhysRevLett.37.1123
Phys.Lett. 70B, 159 (1977)
Y.Gono, R.M.Lieder, M.Muller-Veggian, A.Neskakis, C.Mayer-Boricke
Particle-Hole Symmetry Observed in the Angular Distributions of γ-Rays in 189,191,193Au
NUCLEAR REACTIONS 193,191Ir(α, 4nγ), (α, 6nγ), E=51, 77 MeV; measured Eγ, Iγ, γ(θ). 189,191,193Au transitions deduced δ.
doi: 10.1016/0370-2693(77)90510-X
Nucl.Phys. A327, 269 (1979)
Y.Gono, R.M.Lieder, M.Muller-Veggian, A.Neskakis, C.Mayer-Boricke
In-Beam γ-Ray Study of 189,191,193Au
NUCLEAR REACTIONS 191,193Ir(α, 4nγ), E=51 MeV; 191Ir(α, 6nγ), E=77 MeV; measured Eγ, Iγ, σ(Eγ, θ), γγ-, αγ(t). 189,191,193Au deduced levels, J, π, T1/2, γ-branching, ICC. Enriched targets. Ge(Li), intrinsic Ge detectors.
doi: 10.1016/0375-9474(79)90259-8
Nucl.Phys. A348, 25 (1980)
C.Ekstrom, L.Robertsson, S.Ingelman, G.Wannberg, I.Ragnarsson, and the ISOLDE Collaboration
Nuclear Ground-State Spin of 185Au and Magnetic Moments of 187,188Au: Further evidence for coexisting nuclear shapes in this mass region
NUCLEAR MOMENTS 185Au; measured hfs, J. 187Au measured hfs, a, μ. 188Au; measured a; deduced μ. ABMR technique.
doi: 10.1016/0375-9474(80)90543-6
KVI Ann.Rept., 1981, p.61 (1982)
H.J.Ligthart, J.de Jong, H.Postma
Magnetic Moments of Odd-Mass Au-Nuclei
RADIOACTIVITY 197,195,193,191Hg [from 194Pt(α, xn)]; measured NMR on oriented nuclei. 197,195,193,191Au level deduced μ. Recoil implantation in Fe.
ORNL-6004, p.180 (1983)
C.D.Papanicolopulos, J.L.Wood, J.D.Cole, J.H.Hamilton, K.S.Krane, R.L.Mlekodaj, A.V.Ramayya, M.Huyse, L.Vanneste, E.F.Zganjar
Dynamical Supersymmetries and the Positive Parity States in 191Au
RADIOACTIVITY 191,191mHg(EC), (β+) [from Ta, Hf(16O, X)]; measured γγ(t), γ(θ), oriented nuclei. 191Au deduced γ transitions, δ(M1/E2), evidence for dynamical supersymmetry. Other data input.
Nucl.Phys. A439, 189 (1985)
V.Kolschbach, P.Schuler, K.Hardt, D.Rosendaal, C.Gunther, K.Euler, R.Tolle, M.Marten-Tolle, P.Zeyen
On the Rotation-Aligned Coupling of the h11/2 Proton-Hole States in 191,193Au
NUCLEAR REACTIONS 191,193Ir, 194,196,198Pt(α, 4n), E=50 MeV; measured Eγ, Iγ, γ(θ, H), I(ce), (ce)γ-coin. 191Au deduced levels, J, π. 191,193Au deduced levels, T1/2, B(λ), g. 194,196,198Hg deduced levels T1/2, B(λ).
doi: 10.1016/0375-9474(85)90427-0
Z.Phys. A321, 537 (1985)
J.Streib, H.-J.Kluge, H.Kremmling, R.B.Moore, H.W.Schaaf, K.Wallmeroth, and the ISOLDE Collaboration
Isotope Shifts of Neutron-Deficient Gold Isotopes with 193 ≥ A ≥ 190
RADIOACTIVITY 190,191,192,193Au [from Hg isotope decay]; measured isotope shifts relative to 197Au; deduced rms charge radii. Resonance fluorescence spectroscopy.
Hyperfine Interactions 22, 507 (1985)
E.Van Walle, J.Wouters, D.Vandeplassche, N.Severijns, L.Vanneste
On-Line Nuclear Orientation of Au Isotopes at KOOL
RADIOACTIVITY 185,186,189mAu, 191mHg(β+), (EC); 185Ir(β+), (EC) [from 185Pt decay following 185Au decay]; 191mAu(IT) [from 191Hg decay]; measured γ(θ), oriented nuclei in Fe. 191m,189mAu deduced μ. 185,186,189Pt deduced levels, γ-branching, J, π. 191Au levels deduced J, π, γ-branching, γ-multipolarity, δ.
Nucl.Phys. A453, 93 (1986)
V.Berg, J.Oms, K.Fransson, Z.Hu, and the ISOCELE Collaboration
Half-Life and Electromagentic Deexcitation Rate Measurements for (1/2)+ and (3/2)+ States in Odd-Proton Nuclei around Z = 82
RADIOACTIVITY 201Po(EC), (β+), 203,205,207Po(EC), (β+), (α), 191Hg(EC), (β+) [from Bi(p, xn) and Au(p, xn), E=200 MeV, mass separation]; measured (ce)(ce)(t), ceγ(t). 201,203,205,207Bi, 187,191Au deduced T1/2, δ, B(λ). Plastic scintillators, double magnetic spectrometer.
doi: 10.1016/0375-9474(86)90031-X
Bull.Am.Phys.Soc. 33, No.5, 1190, BJ8 (1988)
J.K.P.Lee, G.Savard, J.E.Crawford, G.Thekkadath, H.T.Duong, J.Pinard, S.Liberman, F.Le Blanc, P.Kilcher, J.Obert, J.Oms, J.C.Putaux, B.Roussiere, J.Sauvage
Nuclear Charge Radius Variations of Gold Isotopes from A = 186 to 199
RADIOACTIVITY 186,187,188,189,190,191,192,193,194,195,196,197,198,199Au; measured hfs, isotope shifts; deduced rms nuclear charge radii differences.
ORNL-6508, p.141 (1989)
I.C.Girit, E.F.Zganjar, C.R.Bingham, H.K.Carter, J.D.Cole, W.L.Croft, J.H.Hamilton, P.M.Gore, E.F.Jones, B.D.Kern, H.Xie, M.O.Kortelahti, J.Kormicki, P.M.Mantica, K.S.Krane, W.B.Newbolt, W.G.Nettles, Y.S.Xu, M.L.Simpson, B.E.Zimmerman
The On-Line Orientation of 191Hg and 193Hg
RADIOACTIVITY 191m,193mHg [from W(12C, X), E=110 MeV]; measured not given. 191,193Au deduced levels.
Nucl.Phys. A493, 224 (1989)
K.Wallmeroth, G.Bollen, A.Dohn, P.Egelhof, U.Kronert, M.J.G.Borge, J.Campos, A.Rodriguez Yunta, K.Heyde, C.de Coster, J.L.Wood, H.-J.Kluge
Nuclear Shape Transition in Light Gold Isotopes
RADIOACTIVITY 185,186,187,188,189m,189,190,191,192,193,195Au; measured hfs, isotope shifts; deduced μ, rms charge radii, deformation parameters β2. Resonance ionization mass spectroscopy, on-line isotope separator.
NUCLEAR MOMENTS 197Au; measured hfs; deduced μ, rms charge radius, deformation parameter. Resonance ionization mass spectroscopy, on-line isotope separator.
doi: 10.1016/0375-9474(89)90396-5
Phys.Rev. C42, R1791 (1990)
J.E.Draper, F.S.Stephens, M.A.Deleplanque, W.Korten, R.M.Diamond, W.H.Kelly, F.Azaiez, A.O.Macchiavelli, C.W.Beausang, E.C.Rubel, J.A.Becker, N.Roy, E.A.Henry, M.J.Brinkman, A.Kuhnert, S.W.Yates
Spins in Superdeformed Bands in the Mass 190 Region
NUCLEAR STRUCTURE 192,194Hf, 233U; analyzed superdeformed band structure; deduced level J. Pseudospin formalism.
doi: 10.1103/PhysRevC.42.R1791
Phys.Rev. C46, 889 (1992)
J.A.Becker, E.A.Henry, A.Kuhnert, T.F.Wang, S.W.Yates, R.M.Diamond, F.S.Stephens, J.E.Draper, W.Korten, M.A.Deleplanque, A.O.Macchiavelli, F.Azaiez, W.H.Kelly, J.A.Cizewski, M.J.Brinkman
Level Spin for Superdeformed Nuclei Near A = 194
NUCLEAR STRUCTURE 189,190,191,192,193,194Hg, 192,194,196,198Pb, 193,194,195Tl; analyzed superdeformed band transition Eγ; deduced J, π. Power series expansion approach.
Nucl.Instrum.Methods Phys.Res. B70, 537 (1992)
P.Kilcher, J.C.Putaux, J.E.Crawford, H.Dautet, H.T.Duong, F.Le Blanc, J.K.P.Lee, J.Obert, J.Oms, J.Pinard, B.Roussiere, J.Sauvage, G.Savard, G.Thekkadath, and the ISOCELE Collaboration
PILIS: Post -ISOCELE laser isobar separation; a high efficiency apparatus for laser spectroscopy
NUCLEAR MOMENTS 197Au; measured hfs; deduced μ, quadrupole moment. 190,192,194,195,196Pt; measured not given; deduced rms charge radius variation. Laser isobar separation.
RADIOACTIVITY 185,186Au(β+), (EC); 191Au(EC); measured hfs; deduced μ, quadrupole moment, rms charge radius variation. 185,186,187,188,189,191,193Pt; measured not given; deduced rms charge radius variation. Laser isobar separation.
doi: 10.1016/0168-583X(92)95978-Z
Nucl.Instrum.Methods Phys.Res. B72, 111 (1992)
F.Le Blanc, J.Pinard, J.Arianer, J.E.Crawford, H.Dautet, H.T.Duong, P.Kilcher, J.K.P.Lee, J.Obert, J.Oms, J.C.Putaux, B.Roussiere, J.Sauvage, G.Thekkadath, and the ISOCELE Collaboration
PILIS: Post-ISOCELE Laser Isobar Separation - a high efficiency apparatus for laser spectroscopy
NUCLEAR MOMENTS 183,184,185,186,191,197Au; measured hfs. 185,186,191Au deduced deformation, μ, quadrupole moments.
Phys.Rev.Lett. 71, 340 (1993)
D.T.Vo, W.H.Kelly, F.K.Wohn, J.C.Hill, M.A.Deleplanque, R.M.Diamond, F.S.Stephens, J.R.B.Oliveira, J.Burde, A.O.Macchiavelli, J.deBoer, B.Cederwall, I.Y.Lee, P.Fallon, J.A.Becker, E.A.Henry, M.J.Brinkman, A.Kuhnert, M.A.Stoyer, J.R.Hughes, J.E.Draper, C.Duyar, E.Rubel
Superdeformation in 191Au
NUCLEAR REACTIONS 186W(11B, 7n), (11B, 6n), (11B, 5n), E=84, 86 MeV; 176Yb(19F, xn), E=100, 105 MeV; measured γγ-coin. 191Au deduced levels, J, π, superdeformed band, dynamic moments of inertia.
doi: 10.1103/PhysRevLett.71.340
Nucl.Phys. A580, 173 (1994)
G.Passler, J.Rikovska, E.Arnold, H.-J.Kluge, L.Monz, R.Neugart, H.Ravn, K.Wendt, and the ISOLDE Collaboration
Quadrupole Moments and Nuclear Shapes of Neutron-Deficient Gold Isotopes
RADIOACTIVITY 193,191Au(EC); 192,194Au(EC), (β+); measured istope shifts, hfs; deduced quadrupole moment, deformation parameter β2, hyperfine constants. Particle-triaxial-rotor model applied to 183-197Au.
doi: 10.1016/0375-9474(94)90769-2
Z.Phys. A359, 373 (1997)
N.Perrin, C.Bourgeois, A.Korichi, M.Pautrat, H.Sergolle, N.Barre, C.Vieu, N.Benouaret, J.Vanhorenbeeck
g Factor Measurements of High Spin Isomeric States in 187,189,191Au
NUCLEAR REACTIONS 181Ta(12C, 4n), E=70 MeV; 172,176Yb(19F, 4n), E=88 MeV; measured Eγ, Iγ(t, H), γγ-coin. 187,189,191Au deduced high-spin levels, isomeric states T1/2, g-factors, configurations.
Phys.Rev. C56, R1667 (1997)
C.Schuck, E.Gueorguieva, A.Lopez-Martens, F.Hannachi, A.Korichi, Ch.Vieu, J.S.Dionisio, I.Deloncle, M.Kaci, F.S.Stephens, M.A.Deleplanque, W.H.Kelly, B.Kharraja, B.J.P.Gall, U.J.van Severen, W.Pohler, B.Schulze, H.Hubel, R.Wadsworth
Proton Superdeformed Bands below the Z = 80 Gap in 191Au: Possible evidence for pseudospin coupling
NUCLEAR REACTIONS 186W(11B, 6n), E=84, 86 MeV; measured Eγ, Iγ, γγ-coin. 191Au deduced high-spin levels, J, π, superdeformed bands properties, configurations. Psuedospin coupling scheme interpretation.
doi: 10.1103/PhysRevC.56.R1667
Hyperfine Interactions 129, 303 (2000)
J.Sauvage, N.Boos, L.Cabaret, J.E.Crawford, H.T.Duong, J.Genevey, M.Girod, G.Huber, F.Ibrahim, M.Krieg, F.Le Blanc, J.K.P.Lee, J.Libert, D.Lunney, J.Obert, J.Oms, S.Peru, J.Pinard, J.C.Putaux, B.Roussiere, V.Sebastian, D.Verney, S.Zemlyanoi, J.Arianer, N.Barre, M.Ducourtieux, D.Forkel-Wirth, G.Le Scornet, J.Lettry, C.Richard-Serre, C.Veron, and the ISOLDE Collaboration
COMPLIS experiments: Collaboration for spectroscopy Measurements using a Pulsed Laser Ion Source
NUCLEAR MOMENTS 182,183,184,185,186,187,188,189,191,193Ir, 179,181,183,183m,185,185m,187,189Pt, 184,184m,191,193,195Au; measured hfs, isotope shifts by Resonance Ionization Spectroscopy (RIS); deduced μ, quadrupole moments, and changes in mean square charge radii, deformation parameter. Comparisons with model calculations.
Nucl.Instrum.Methods Phys.Res. A589, 202 (2008)
T.Kibedi, T.W.Burrows, M.B.Trzhaskovskaya, P.M.Davidson, C.W.Nestor, Jr.
Evaluation of theoretical conversion coefficients using BrIcc
COMPILATION Z=5-110; compiled and evaluated ICC data. BrICC database.
doi: 10.1016/j.nima.2008.02.051
At.Data Nucl.Data Tables 99, 69 (2013)
I.Angeli, K.P.Marinova
Table of experimental nuclear ground state charge radii: An update
COMPILATION Z=0-96; compiled nuclear radii, rms nuclear charge radii.
doi: 10.1016/j.adt.2011.12.006
At.Data Nucl.Data Tables 111-112, 1 (2016)
N.J.Stone
Table of nuclear electric quadrupole moments
COMPILATION Z=1-99; compiled experimental values of nuclear electric quadrupole moments.
doi: 10.1016/j.adt.2015.12.002
INDC(NDS)-0794 (2019)
N.J.Stone
Table of Recommended Nuclear Magnetic Dipole Moments: Part I - Long-lived States
COMPILATION Z=0-99; compiled experimental values of nuclear magnetic moments.
Phys.Rev. C 101, 034308 (2020)
A.E.Barzakh, D.Atanasov, A.N.Andreyev, M.Al Monthery, N.A.Althubiti, B.Andel, S.Antalic, K.Blaum, T.E.Cocolios, J.G.Cubiss, P.Van Duppen, T.Day Goodacre, A.de Roubin, Yu.A.Demidov, G.J.Farooq-Smith, D.V.Fedorov, V.N.Fedosseev, D.A.Fink, L.P.Gaffney, L.Ghys, R.D.Harding, D.T.Joss, F.Herfurth, M.Huyse, N.Imai, M.G.Kozlov, S.Kreim, D.Lunney, K.M.Lynch, V.Manea, B.A.Marsh, Y.Martinez Palenzuela, P.L.Molkanov, D.Neidherr, R.D.Page, M.Rosenbusch, R.E.Rossel, S.Rothe, L.Schweikhard, M.D.Seliverstov, S.Sels, C.Van Beveren, E.Verstraelen, A.Welker, F.Wienholtz, R.N.Wolf, K.Zuber
Hyperfine anomaly in gold and magnetic moments of Iπ = 11/2- gold isomers
NUCLEAR MOMENTS 177m,191m,193m,195mAu; measured hyperfine structure spectra (hfs), hyperfine splitting, differential hyperfine anomaly, magnetic dipole moments using in-source laser resonance-ionization spectroscopy (RILIS) at CERN-ISOLDE. Mass separated Au beams were produced in U(p, X), E=1.4 GeV reaction, and delivered to either the ISOLTRAP Multi-Reflection Time-of-Flight Mass Spectrometer (MR-ToF MS) or the Windmill (WM) decay station. Comparison to the previously measured magnetic moments. 185,186,187,189,189m,191,193,194Au; re-evaluated previously measured magnetic dipole moments by properly accounting for the hyperfine anomaly.
doi: 10.1103/PhysRevC.101.034308
INDC(NDS)-0816 (2020)
N.Stone
Table of Recommended Nuclear Magnetic Dipole Moments: Part II, Short-Lived States
COMPILATION Z=5-95; compiled experimental values of nuclear magnetic moments.
Phys.Rev. C 104, 034616 (2021)
M.S.Asnain, M.Shuaib, I.Majeed, M.K.Sharma, V.R.Sharma, A.Yadav, D.P.Singh, P.P.Singh, U.Gupta, R.N.Sahoo, A.Sood, M.Kaushik, S.Kumar, R.Kumar, B.P.Singh, R.Prasad
Effect of non-α-cluster projectile on incomplete-fusion dynamics: Experimental study of the 14N + 181Ta
NUCLEAR REACTIONS 181Ta(14N, 3n)192Hg, (14N, 4n)191Hg/191mHg, (14N, 5n)190Hg, (14N, 6n)189Hg/189mHg, (14N, 3np)191Au, (14N, 4np)190Au, (14N, 5np)189Au/189mAu, (14N, 2nα)189Pt, (14N, 4nα)187Pt, (14N, 5nα)186Pt, (14N, 3npα)187Ir, (14N, 4npα)186Ir/186mIr, (14N, 5npα)185Ir, (14N, 4n2α)183Os, (14N, 5np2α)181Re, E=65.53, 67.50, 69.47, 71.54, 73.65, 75.65, 77.08, 79.51, 81.42, 83.05, 85.17, 87.07 MeV; measured off-line Eγ, Iγ, σ(E) for radio-nuclides populated via complete fusion (CF) and/or incomplete fusion (ICF processes) by activation method at the ion-beam facility of the IUAC-New Delhi; deduced total fusion, total complete fusion, and total incomplete fusion σ(E). Comparison with statistical model calculations using PACE4 code. 190Hg; measured nominal half-life from γ-decay curves as an example for the purpose of correct identification of different radioactive nuclei produced through various reaction channels.
doi: 10.1103/PhysRevC.104.034616
Chin.Phys.C 45, 030003 (2021)
M.Wang, W.J.Huang, F.G.Kondev, G.Audi, S.Naimi
The AME 2020 atomic mass evaluation (II). Tables, graphs and references
ATOMIC MASSES A=1-295; compiled, evaluated atomic masses, mass excess, β-, ββ and ββββ-decay, binding, neutron and proton separation energies, decay and reaction Q-value data.
Phys.Rev.Lett. 131, 202501 (2023)
J.G.Cubiss, A.N.Andreyev, A.E.Barzakh, P.Van Duppen, S.Hilaire, S.Peru, S.Goriely, M.Al Monthery, N.A.Althubiti, B.Andel, S.Antalic, D.Atanasov, K.Blaum, T.E.Cocolios, T.Day Goodacre, A.de Roubin, G.J.Farooq-Smith, D.V.Fedorov, V.N.Fedosseev, D.A.Fink, L.P.Gaffney, L.Ghys, R.D.Harding, M.Huyse, N.Imai, D.T.Joss, S.Kreim, D.Lunney, K.M.Lynch, V.Manea, B.A.Marsh, Y.Martinez Palenzuela, P.L.Molkanov, D.Neidherr, G.G.O'Neill, R.D.Page, S.D.Prosnyak, M.Rosenbusch, R.E.Rossel, S.Rothe, L.Schweikhard, M.D.Seliverstov, S.Sels, L.V.Skripnikov, A.Stott, C.Van Beveren, E.Verstraelen, A.Welker, F.Wienholtz, R.N.Wolf, K.Zuber
Deformation versus Sphericity in the Ground States of the Lightest Gold Isotopes
NUCLEAR MOMENTS 176,177,178,179,180,181,182,183,187,191,193,195Au [from U(p, X), E=1.4 GeV]; measured frequencies; deduced mean-squared charge radii, ground-state deformations, nuclear magnetic moments. Comparison with available data. The in-source, resonance-ionization laser spectroscopy technique, at the ISOLDE facility (CERN).
doi: 10.1103/PhysRevLett.131.202501