NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = I.Grant Found 76 matches. 2018EK01 At.Data Nucl.Data Tables 120, 152 (2018) J.Ekman, P.Jonsson, L.Radziute, G.Gaigalas, G.Del Zanna, I.P.Grant Large-scale calculations of atomic level and transition properties in the aluminum isoelectronic sequence from Ti X through Kr XXIV, Xe XLII, and W LXII ATOMIC PHYSICS Z=22-36, 54, 74; calculated energy levels and uncertainties. Comparison with available data.
doi: 10.1016/j.adt.2017.04.005
2016MA40 Eur.Phys.J. A 52, 172 (2016) H.Mach, A.Lindroth, E.Ruchowska, J.Kvasil, B.Fogelberg, K.Gulda, A.J.Aas, M.J.G.Borge, I.S.Grant, E.Hagebo, W.Kurcewicz, T.Martinez, B.Rubio, J.F.Smith, K.Steffensen, J.L.Tain, O.Tengblad, T.F.Thorsteinsen On the enhanced E1 transitions in the K = 3/2 parity doublet band in 223Ra RADIOACTIVITY 223Fr(β-)[from 223Rn]; measured β-decay of (3/2)- and (5/2)- states (50 and 80 keV) Eγ, Iγ(t) using BaF2 crystal for timing and two Ge, Eβ, Iβ(t) using ΔE NE111A, βγ-coin; deduced time-delayed βγ(t) spectrum, T1/2, B(E1), B(E2), B(M1) for K=3/2 band states below 250 keV, intrinsic electric dipole moment D0; calculated T1/2, γ transition probabilities, B(E1), B(E2), B(M1), average electric dipole moment for 223,224Ra (and compared with available data for Ra isotopes), quadrupole and octupole vibration energies in 222,224Ra, structure of intrinsic states.
doi: 10.1140/epja/i2016-16172-4
2016PH01 J.Phys.(London) B49, 035601 (2016) T.LH.Pham, T.VB.Nguyen, J.A.Lowe, I.P.Grant, C.T.Chantler Characterization of the copper K β x-ray emission profile: an ab initio multi-configuration Dirac-Hartree-Fock approach with Bayesian constraints ATOMIC PHYSICS Cu; calculated K β x-ray transition energies and intensities, gf ratios. Ab initio multi-configuration Dirac-Hartree-Fock (MCDHF).
doi: 10.1088/0953-4075/49/3/035601
2002GU15 Nucl.Phys. A703, 45 (2002) K.Gulda, W.Kurcewicz, A.J.Aas, M.J.G.Borge, D.G.Burke, B.Fogelberg, I.S.Grant, E.Hagebo, N.Kaffrell, J.Kvasil, G.Lovhoiden, H.Mach, A.Mackova, T.Martinez, G.Nyman, B.Rubio, J.L.Tain, O.Tengblad, T.F.Thorsteinsen, and the ISOLDE Collaboration The Nuclear Structure of 229Th RADIOACTIVITY 229Ac(β-) [from 232Th(p, 4p) and 238U(p, 6p4n) and subsequent decay]; measured Eγ, Iγ, E(ce), I(ce), T1/2, βγ(t), (ce)γ-, γγ-coin. 229Th deduced levels, J, π, ICC, multipolarities, rotational bands, B(E1), B(E2), B(M1), dipole moments. Mini-orange spectrometer, advanced fast-timing techniques. Comparison with quasiparticle-phonon model predictions.
doi: 10.1016/S0375-9474(01)01456-7
2001FR05 Nucl.Phys. A686, 71 (2001) L.M.Fraile, M.J.G.Borge, H.Mach, R.Boutami, A.J.Aas, B.Fogelberg, L.M.Garcia-Raffi, I.S.Grant, K.Gulda, E.Hagebo, W.Kurcewicz, J.Kvasil, M.J.Lopez, G.Lovhoiden, T.Martinez, B.Rubio, J.L.Tain, O.Tengblad, and the ISOLDE Collaboration Persistence of Octupole Correlations in 231Ra RADIOACTIVITY 231Fr(β-) [from 238U(p, 2n6p)]; measured Eγ, Iγ, E(ce), I(ce), γγ-, (ce)γ-coin, T1/2. 231Ra deduced levels, J, π, ICC, multipolarities, rotational bands, B(E1), B(E2). Quasiparticle-plus-phonon model, BaF2 detectors, mini-orange spectrometer.
doi: 10.1016/S0375-9474(00)00572-8
2000PE30 J.Phys.(London) G26, 1829 (2000) M.R.Pearson, P.Campbell, K.Leerungnavarat, J.Billowes, I.S.Grant, M.Keim, J.Kilgallon, I.D.Moore, R.Neugart, M.Neuroth, S.Wilbert, and the ISOLDE Collaboration Nuclear Moments and Charge Radii of Bismuth Isotopes NUCLEAR MOMENTS 205,206,207,208,209,210,212,213Bi; measure hfs, isotope shifts; deduced μ, quadrupole moment. Comparison with Hg, Tl, Pb and Po isotopes and with Shell model calculations.
doi: 10.1088/0954-3899/26/12/307
1999AA03 Nucl.Phys. A654, 499 (1999) A.J.Aas, H.Mach, J.Kvasil, M.J.G.Borge, B.Fogelberg, I.S.Grant, K.Gulda, E.Hagebo, P.Hoff, W.Kurcewicz, A.Lindroth, G.Lovhoiden, A.Machova, T.Martinez, B.Rubio, M.Sanchez-Vega, J.F.Smith, J.L.Tain, R.B.E.Taylor, O.Tengblad, T.F.Thorsteinsen, and the ISOLDE Collaboration Quenched E1 Transition Rates in 231Th RADIOACTIVITY 231Ac(β-); measured Eγ, Iγ, βγ-, γγ-coin, T1/2. 231Th deduced levels T1/2, B(λ), rotational bands. Fast-timing βγγ(t) method, quasiparticle-plus-phonon model.
doi: 10.1016/S0375-9474(99)00307-3
1999BI11 Phys.Rev. A59, 4295 (1999) J.Bieron, C.F.Fischer, I.P.Grant Large-Scale Multiconfigurational Dirac-Fock Calculations of the Hyperfine-Structure Constants and Determination of the Nuclear Quadrupole Moment of 49Ti NUCLEAR MOMENTS 49Ti; calculated hyperfine interaction constants, quadrupole moments. Multiconfiguration Dirac-Fock model.
doi: 10.1103/PhysRevA.59.4295
1999FR33 Nucl.Phys. A657, 355 (1999) L.M.Fraile, A.J.Aas, M.J.G.Borge, B.Fogelberg, L.M.Garcia-Raffi, I.S.Grant, K.Gulda, E.Hagebo, W.Kurcewicz, J.Kvasil, G.Lovhoiden, H.Mach, A.Mackova, T.Martinez, B.Rubio, J.L.Tain, A.G.Teijeiro, O.Tengblad, T.F.Thorsteinsen, and the ISOLDE Collaboration Octupole Correlations in 229Ra RADIOACTIVITY 229Fr(β-) [from 238U(p, 4n6p)]; measured Eγ, Iγ, I(ce), γγ-coin, T1/2. 229Ra deduced levels, J, π, ICC, multipolarities, rotational bands, B(λ). Ge, Si(Li) detectors, mini-orange spectrometer, quasiparticle-plus-phonon model.
doi: 10.1016/S0375-9474(99)00330-9
1999LE11 Phys.Rev.Lett. 82, 2476 (1999) J.M.G.Levins, D.M.Benton, J.Billowes, P.Campbell, T.G.Cooper, P.Dendooven, D.E.Evans, D.H.Forest, I.S.Grant, J.A.R.Griffith, J.Huikari, A.Jokinen, K.Perajarvi, G.Tungate, G.Yeandle, J.Aysto First On-Line Laser Spectroscopy of Radioisotopes of a Refractory Element NUCLEAR MOMENTS 170,172,173,174,176,177,179,180Hf; measured isotope shifts, mean-square charge radii; deduced deformation. On-line laser spectroscopy.
doi: 10.1103/PhysRevLett.82.2476
1998BI20 Phys.Rev. A 58, 4401 (1998) J.Bieron, I.P.Grant, C.F.Fischer Multiconfiguration Dirac-Fock calculations of the hyperfine structure constants and determination of the nuclear quadrupole moment of yttrium 90 NUCLEAR STRUCTURE 90Y; calculated electric quadrupole hyperfine constants; deduced quadrupole moment as a function of different configurations. Multiconfiguration Dirac-Fock model.
doi: 10.1103/PhysRevA.58.4401
1997BI13 Phys.Rev. A56, 316 (1997) J.Bieron, I.P.Grant, C.F.Fischer Nuclear Quadrupole Moment of Scandium NUCLEAR MOMENTS 45Sc; calculated hyperfine constants, electric quadrupole moment. Mulitconfiguration Dirac-Fock model.
doi: 10.1103/PhysRevA.56.316
1997CA39 J.Phys.(London) G23, 1141 (1997) P.Campbell, J.Billowes, E.C.A.Cochrane, J.L.Cooke, T.G.Cooper, P.Dendooven, D.E.Evans, I.S.Grant, J.A.R.Griffith, A.Honkanen, M.Huhta, M.Oinonen, M.R.Pearson, H.Penttila, J.R.Persson, D.S.Richardson, G.Tungate, P.D.Wheeler, L.Zybert, J.Aysto A Thirty Second Isomer in 171Hf NUCLEAR REACTIONS 170Yb(α, 3n), E=50 MeV; measured Iγ(t). 171mHf deduced T1/2. Ion guide online isotope seperator. RADIOACTIVITY 171mHf(IT) [from 170Yb(α, 3n), E=50 MeV]; measured Iγ(t); deduced T1/2. Ion guide online isotope seperator.
doi: 10.1088/0954-3899/23/9/014
1997CA53 J.Phys.(London) B30, 2351 (1997) P.Campbell, J.Billowes, I.S.Grant The Specific Mass Shift of the Zinc Atomic Ground State NUCLEAR MOMENTS Zn; measured resonance lines isotope shifts; deduced core-valence correlations. ATOMIC PHYSICS Zn; measured resonance lines isotope shifts; deduced core-valence correlations.
doi: 10.1088/0953-4075/30/10/010
1997CO26 J.Phys.(London) G23, L97 (1997) J.L.Cooke, J.Billowes, P.Campbell, E.C.A.Cochrane, T.G.Cooper, P.Dendooven, D.E.Evans, J.A.R.Griffith, I.S.Grant, A.Honkanen, M.Huhta, J.M.G.Levins, M.Oinonen, M.R.Pearson, H.Penttila, J.A.Persson, D.S.Richardson, G.Tungate, P.D.Wheeler, L.Zybert, J.Aysto First Measurement of Radioisotopes by Collinear Laser Spectroscopy at an Ion-Guide Separator NUCLEAR REACTIONS 238U(p, F), E=25 MeV; measured 112Rh yield vs electrode voltage, beam current. Molecular beam, ion-guide isotope separator, ion-photon coincidence. RADIOACTIVITY 140,142,144Ba [from 238U(p, F), E=25 MeV]; measured optical isotope shifts. Ion-guide isotope separator, collinear laser spectroscopy, ion-photon coincidence.
doi: 10.1088/0954-3899/23/11/002
1997KU20 Nucl.Phys. A621, 827 (1997) W.Kurcewicz, I.S.Grant, K.Gulda, A.J.Aas, J.Billowes, M.J.G.Borge, D.G.Burke, P.A.Butler, J.F.C.Cocks, B.Fogelberg, S.J.Freeman, G.D.Jones, E.Hagebo, P.Hoff, J.Honsi, A.Lindroth, G.Lovhoiden, H.Mach, T.Martinez, R.A.Naumann, K.Nybo, G.Nyman, H.Ravn, B.Rubio, J.Simpson, A.G.Smith, J.F.Smith, K.Steffensen, J.L.Tain, O.Tengblad, T.F.Thorsteinsen, and the ISOLDE Collaboration The Nuclear Structure of 227Fr RADIOACTIVITY 227Rn(β-) [from 232Th(p, n5p), E=1 GeV]; measured Eγ, Iγ, I(ce), T1/2, βγγ(t), γγ-coin. 227Fr deduced levels, J, π, ICC, γ-multipolarity, rotational bands, B(λ). Ge, Si(Li), BGO, plastic, BaF2 detectors, mini-orange spectrometer.
doi: 10.1016/S0375-9474(97)00190-5
1996AA01 Nucl.Phys. A611, 281 (1996) A.J.Aas, H.Mach, M.J.G.Borge, B.Fogelberg, I.S.Grant, K.Gulda, E.Hagebo, W.Kurcewicz, J.Kvasil, A.Lindroth, T.Martinez, D.Nosek, B.Rubio, J.F.Smith, K.Steffensen, J.L.Tain, O.Tengblad, T.F.Thorsteinsen, and the ISOLDE Collaboration Enhanced and Quenched B(E1) Transition Rates between Parity Doublet Bands in 227Ra RADIOACTIVITY 227Fr(β-); measured βγγ(t). 227Ra deduced levels, J, π, T1/2, K, B(λ), band structure. Quasiparticle-plus-phonon model, Coriolis coupling.
doi: 10.1016/S0375-9474(96)00312-0
1996RA23 J.Phys.(London) G22, 1037 (1996) S.Rastikerdar, W.Gelletly, B.J.Varley, I.S.Grant New Results on 102Cd NUCLEAR REACTIONS 50Cr(56Fe, 2n2p), E=195 MeV; measured Eγ, Iγ, γγ-coin. 102Cd deduced levels, J, π, band structure. Pure γ-spectrum from mass gated γ yields distributions.
doi: 10.1088/0954-3899/22/7/009
1996ST14 Phys.Rev.Lett. 77, 36 (1996) T.L.Stewart, M.W.Kermode, D.J.Beachey, N.Rowley, I.S.Grant, A.T.Kruppa α Decay of Deformed Actinide Nuclei RADIOACTIVITY 221Fr, 227Pa, 241Am, 253Es(α); calculated α-decay associated anisotropies. Branching ratios data input.
doi: 10.1103/PhysRevLett.77.36
1996ST28 Nucl.Phys. A611, 332 (1996) T.L.Stewart, M.W.Kermode, D.J.Beachey, N.Rowley, I.S.Grant, A.T.Kruppa α-Particle Decay Through a Deformed Barrier RADIOACTIVITY A=220-248; Z=88-96; calculated α-decay associated amplitudes vs phases. 233,229U, 247,257Es, 237Np, 241Pu, 243,245Cm, 249Bk, 249Cf(α); calculated α-decay associated anisotropies, branching ratios in some cases. Eigenchannel formalism, sub-barrier fusion.
doi: 10.1016/S0375-9474(96)00404-6
1992BA68 Hyperfine Interactions 75, 433 (1992) C.G.Barham, S.S.Al-Ghamdi, A.Bhagwat, M.Booth, I.S.Grant, M.Lindroos, J.Rikovska, B.D.D.Singleton, N.J.Stone, P.M.Walker On-Line Orientation of Bromine Isotope RADIOACTIVITY 74mBr(β+), (EC); 72Br(β+); measured γ-anisotropy. 72Br level deduced μ limits. 75Br(β+), (EC); measured β-asymmetry; deduced level configuration. On-line orientation.
1992BH02 J.Phys.(London) G18, 977 (1992) A.Bhagwat, S.S.Al-Ghamdi, P.M.Walker, B.D.D.Singleton, C.G.Barham, I.S.Grant Lifetime Measurements of Intruder States in 120Xe and the Shape Coexistence Picture RADIOACTIVITY 120,120mCs(β+), (EC) [from 93Nb(32S, xnyp), E=165 MeV]; measured I(ce), (β)(ce)-coin, centroid shifts. 120Xe deduced levels, γ-multipolarity, K-electron branching ratio, T1/2, B(λ).
doi: 10.1088/0954-3899/18/5/025
1992DA06 J.Phys.(London) G18, L67 (1992) M.P.Dancey, M.A.Skelton, J.Billowes, D.A.Eastham, D.E.Evans, I.S.Grant, J.A.R.Griffith, P.M.Walker, D.D.Warner, S.A.Wells Properties of a Two-Second Isomer in 127Ba Measured with a New Technique of Laser Spectroscopy RADIOACTIVITY 127mBa [from 97Mo(34S, 2p2n)]; measured isotope shift, hfs; deduced Q, μ, radius differences. Particle plus triaxial rotor model comparison. New laser spectroscopy technique.
doi: 10.1088/0954-3899/18/3/002
1992GR20 Phys.Rev. C46, 2228 (1992) A.G.Griffiths, C.J.Ashworth, J.Rikovska, N.J.Stone, J.P.White, I.S.Grant, P.M.Walker, W.B.Walters Magnetic Moments and Shape Coexistence in the Light Br Isotopes RADIOACTIVITY 72g,72m,73,74m,75,76g,77Br; measured γ(θ, H, T), oriented nuclei implanted into Fe. 73Br level deduced J. 72,74,75,76,77Br levels deduced μ. Model comparison.
doi: 10.1103/PhysRevC.46.2228
1992PL01 Z.Phys. A342, 43 (1992) A.Plochocki, K.Rykaczewski, T.Batsch, J.Szerypo, J.Zylicz, R.Barden, O.Klepper, E.Roeckl, D.Schardt, H.Gabelmann, P.Hill, H.Ravn, T.Thorsteinsen, I.S.Grant, H.Grawe, P.Manakos, L.D.Skouras, and the ISOLDE Collaboration Gamow-Teller Beta Decay of the Very Neutron-Deficient N = 50 Nuclide 98Cd RADIOACTIVITY 98Cd(EC), (β+) [from Sn(p, X), E=600 MeV]; measured Eγ, Iγ, γγ-, γ(X-ray)-coin; deduced Q(EC). 98Ag deduced levels, relative Iγ, ICC, J, π, Gamow-Teller transition strength, γ-multipolarity. Shell model.
1992RO21 Hyperfine Interactions 75, 457 (1992) I.Romanski, I.Berkes, D.E.Brown, M.De Jesus, R.Eder, I.S.Grant, E.Hagn, P.Harding, P.Herzog, B.Hinfurtner, B.Kastelein, H.Postma, J.Prinz, P.Richards, K.Schlosser, N.J.Stone, L.Vanneste, E.Zech, and the NICOLE and ISOLDE Collaborations Time-Resolved and Time-Integral On-Line Nuclear Orientation Measurements of Neutron-Deficient Hg-Au-Pt-Ir Nuclei RADIOACTIVITY 182,183,184,186Hg(β+), (EC) [from Pb(3He, X), E=600, 910 MeV]; measured γ-anisotropy vs temperature. 183Ir level deduced μ for two possible J. 183Pt deduced isomer μ. 184Au levels deduced g-factors. Time resolved, time integral on-line nuclear orientation techniques, Fe host.
doi: 10.1007/BF02399003
1992SI22 Hyperfine Interactions 75, 471 (1992) B.D.D.Singleton, P.M.Walker, A.Bhagwat, S.S.Al-Ghamdi, C.G.Barham, I.S.Grant, A.G.Griffiths, J.Rikovska, N.J.Stone On-Line Nuclear Orientation of the Deformed Neutron-Deficient Eu, Sm and Pm Isotopes RADIOACTIVITY 142m,139Eu(β+), (EC); 138Eu(β+); 141m,139mSm(β+), (EC); 141,138Pm(β+), (EC) [from 98,96Mo(48Ti, X), E=220 MeV]; measured γ-anisotropy vs temperature, time. 139,138Eu, 139Sm, 138Pm levels deduced μ. Oriented nuclei.
doi: 10.1007/BF02399004
1991KE08 Z.Phys. A339, 355 (1991) H.Keller, R.Barden, R.Kirchner, O.Klepper, E.Roeckl, D.Schardt, I.S.Grant, A.Plochocki, K.Rykaczewski, J.Szerypo, J.Zylicz, and the ISOLDE Collaboration Q(EC) Value and Gamow-Teller Strength of the 102Cd EC/β+ Decay RADIOACTIVITY 102Cd [from 92Mo(16O, X), 50Cr(58Ni, X), E=9.2, 5.3 MeV/nucleon, respectively; Sn(p, X), E=600 MeV]; measured Eγ, Iγ, I(ce), γ(X-ray)-coin, γγ-coin; deduced T1/2, Q(EC). 102Ag deduced levels, J, π, ICC, Gamow-Teller transition strength.
doi: 10.1007/BF01560637
1990DA13 Hyperfine Interactions 59, 193 (1990) M.P.Dancey, J.Billowes, I.S.Grant, D.E.Evans, J.A.R.Griffith, S.A.Wells, D.A.Eastham, J.Groves, J.R.H.Smith, D.W.L.Tolfree, P.M.Walker Laser Fluorescence on Radio-Active Isotopes Produced in Very Low Yield RADIOACTIVITY 120,121,122,123,124,127mBa [from 92,96,98Mo(32S, xn2p)]; measured hfs; deduced rms radii changes. 127mBa deduced μ, quadrupole moment. Fast ion-photon coincidence, ultra-sensitive laser fluorescence spectroscopy.
1990ED01 Hyperfine Interactions 59, 83 (1990) R.Eder, I.Berkes, D.E.Brown, I.S.Grant, E.Hagn, P.Harding, R.Hassani, P.Herzog, B.Kastelein, A.Knipper, G.Marguier, M.Massaq, S.Ohya, H.Postma, J.Prinz, C.Richard-Serre, I.Romanski, K.Schlosser, N.J.Stone, W.Vanderpoorten, J.Vanhaverbeke, L.Vanneste, T.Woelfle, E.Zech, and the ISOLDE Collaboration NICOLE: New on-line orientation facility at ISOLDE/CERN RADIOACTIVITY 187,185,189Pt, 186mIr; measured NMR, on-line orientation. 187,185,189Pt levels deduced μ, electric quadrupole moments, ratio. 186Ir deduced isomer μ, J. 184Hg; measured γ(θ), anisotropy vs temperature, I(ce). 184Au levels deduced T1/2, decay scheme. Off-line, on-line orientation techniques.
doi: 10.1007/BF02401196
1990EN01 J.Phys.(London) G16, 105 (1990) J.G.England, I.S.Grant, J.A.R.Griffith, D.E.Evans, D.A.Eastham, G.W.A.Newton, P.M.Walker Isotope Shifts and Hyperfine Splittings in 144-154Sm I RADIOACTIVITY 145,151,153,146Sm; measured isotope shifts, hfs; deduced hfs constants, rms radii differences, μ, Q. Other data input. NUCLEAR MOMENTS 144,147,148,149,150,152,154Sm; measured isotope shifts, hfs; deduced hfs constants, rms radii differences, μ, Q. Other data input. NUCLEAR STRUCTURE 145,147,149,151,153Sm; calculated μ, quadrupole moment.
doi: 10.1088/0954-3899/16/1/014
1989RY02 Z.Phys. A332, 275 (1989) K.Rykaczewski, A.Plochocki, I.S.Grant, H.Gabelmann, R.Barden, D.Schardt, J.Zylicz, G.Nyman, and the ISOLDE Collaboration The Gamow-Teller Beta Decay of 100Cd RADIOACTIVITY 100Cd(EC), (β+) [from Sn(p, X), E=600 MeV]; measured E(γ), I(γ), γγ-coin, I(ce); deduced Q(EC). 100Ag deduced levels, possible J, π, Gamow-Teller transition strength.
1988AS06 Hyperfine Interactions 43, 489 (1988) C.J.Ashworth, T.L.Shaw, J.Rikovska, N.J.Stone, V.R.Green, P.M.Walker, B.D.D.Singleton, I.S.Grant The Sign of the Magnetic Dipole Moment of the Ground State of 122I RADIOACTIVITY 122I [from 93Nb(32S, X), E=150-170 MeV]; measured annhilation radiation γ(θ), oriented nuclei. 122I deduced μ sign.
doi: 10.1007/BF02398330
1988BR38 Hyperfine Interactions 43, 353 (1988) D.E.Brown, L.Goettig, I.S.Grant, V.R.Green, K.S.Krane, J.Rikovska, T.L.Shaw, N.J.Stone, P.M.Walker On-Line Nuclear Orientation of Odd - Odd 120I RADIOACTIVITY 120I(β+) [from 93Nb(32S, X), (34S, X)]; measured γγ-, (ce)γ-coin, γ(θ), oriented nuclei. 120Te deduced levels, J, π, δ(M1/E2).
doi: 10.1007/BF02398315
1988ED02 Hyperfine Interactions 43, 469 (1988) R.Eder, C.J.Ashworth, I.Berkes, D.E.Brown, U.Daemmrich, I.S.Grant, A.G.Griffiths, E.Hagn, R.Hassani, P.Herzog, S.Ohya, M.Massaq, C.Richard-Serre, J.Rikovska, K.Schloesser, N.Severijns, N.J.Stone, W.Vanderpoorten, J.Vanhaverbeke, L.Vanneste, T.Woelfle, E.Zech, and the ISOLDE Collaboration Shape Transition in Light Pt Isotopes: Magnetic moments and electric quadrupole moment ratios for 185,187,189Pt RADIOACTIVITY 185,187,189Pt; measured NMR, oriented nuclei. 187,185Pt deduced level g, spectroscopic quadrupole moment.
doi: 10.1007/BF02398326
1988GR26 Hyperfine Interactions 43, 481 (1988) A.G.Griffiths, C.J.Ashworth, I.S.Grant, J.Rikovska, N.J.Stone, P.M.Walker, W.B.Walters, J.P.White Deformation in the Light Br Isotopes RADIOACTIVITY 72,74m,75,76,77Br [from 54Fe(28Si, X), E=150 MeV]; measured γ(θ), oriented nuclei. 72,72m,74m,75,77Br deduced μ. 73Br deduced μ, J.
doi: 10.1007/BF02398329
1988WA33 Hyperfine Interactions 43, 343 (1988) W.B.Walters, J.Rikovska, N.J.Stone, T.L.Shaw, P.Walker, I.S.Grant E0 Transitions in the Mid-Shell Even-Even Xe Nuclides: Decay of 31-s 124Cs to levels of 124Xe RADIOACTIVITY 124Cs(EC), (β+) [from 92Mo(32S, X)]; measured E(γ), I(γ), I(ce), γγ-, γ(ce)-, (ce)(ce)-coin. 124Xe deduced levels, ICC, γ-multipolarity, B(E0)/B(E2).
doi: 10.1007/BF02398314
1988WE14 Phys.Lett. 211B, 272 (1988) S.A.Wells, D.E.Evans, J.A.R.Griffith, D.A.Eastham, J.Groves, J.R.H.Smith, D.W.L.Tolfree, D.D.Warner, J.Billowes, I.S.Grant, P.M.Walker Fluorescent Atom Coincidence Spectroscopy of Extremely Neutron-Deficient Barium Isotopes RADIOACTIVITY 120,121,122,123,124Ba [from 92,96Mo(32S, xn2p)]; measured hfs, isotope shifts; deduced quadrupole deformation parameter. 120,121,122,123Ba deduced rms charge radii relative to 124Ba. Fluorescent atom coincidence spectroscopy.
doi: 10.1016/0370-2693(88)90902-1
1987EA01 Phys.Rev. C36, 1583 (1987) D.A.Eastham, P.M.Walker, J.R.H.Smith, D.D.Warner, J.A.R.Griffith, D.E.Evans, S.A.Wells, M.J.Fawcett, I.S.Grant Nuclear Charge Radii of Proton-Rich Strontium Isotopes RADIOACTIVITY 78,79,80,81,82,83Sr; measured hfs, isotope shift; deduced μ, rms radii. Atom-photon coincidence laser spectroscopy. NUCLEAR MOMENTS 88,86,87Sr; measured hyperfine structure, isotope shifts; deduced μ, rms radii. Atom-photon coincidence laser spectroscopy.
doi: 10.1103/PhysRevC.36.1583
1987GR15 Nucl.Instrum.Methods Phys.Res. B26, 482 (1987) V.R.Green, C.J.Ashworth, J.Rikovska, T.L.Shaw, N.J.Stone, P.M.Walker, C.Leyland, I.S.Grant On-Line Low-Temperature Nuclear Orientation at DOLIS-COLD RADIOACTIVITY 117I, 118m,121mCs, 116Sb; measured NMR, γ-ray anisotropy vs inverse temperature. 117I, 118m,121mCs, 116Sb deduced μ. On-line isotope separator, cryogenic on-line device.
doi: 10.1016/0168-583X(87)90798-1
1987SH12 Phys.Rev. C36, 413 (1987) T.L.Shaw, V.R.Green, C.J.Ashworth, J.Rikovska, N.J.Stone, P.M.Walker, I.S.Grant On-Line Nuclear Orientation of Cesium Isotopes and the Magnetic Moment of 118mCs RADIOACTIVITY 118m,119mCs; 120Cs(β+), (EC); 121mCs; measured γ(θ), oriented nuclei; deduced hyperfine field for Cs in Fe, relaxation Korringa constant. 118mCs deduced μ, configuration.
doi: 10.1103/PhysRevC.36.413
1987SH18 Hyperfine Interactions 35, 821 (1987) T.L.Shaw, V.R.Green, C.J.Ashworth, J.Rikovska, N.J.Stone, P.M.Walker, I.S.Grant On-Line Nuclear Orientation and Relaxation Studies of Cs Isotopes RADIOACTIVITY 119m,120,121mCs(EC), (β+) [from 93Nb(32S, X), (34S, X)]; measured γ(θ), anisotropy, oriented nuclei; deduced Cs hyperfine field in Fe. 118mCs deduced μ. On-line low temperature nuclear orientation technique.
doi: 10.1007/BF02394500
1987ST19 Hyperfine Interactions 34, 111 (1987) N.J.Stone, V.R.Green, T.L.Shaw, J.Rikovska, C.Ashworth, P.M.Walker, I.S.Grant On-Line Resonance of 116gSb Cryogenically Oriented at the DOLIS-COLD Facility RADIOACTIVITY 119Sb(EC) [from 93Nb(28Si, xnyp), E=145 MeV]; measured NMR, oriented nuclei. 119Sb level deduced μ.
doi: 10.1007/BF02072688
1987ST20 Hyperfine Interactions 34, 115 (1987) N.J.Stone, J.Rikovska, V.R.Green, T.L.Shaw, K.S.Krane, P.M.Walker, I.S.Grant Iodine Magnetic Moments Measured by On-Line Nuclear Orientation RADIOACTIVITY 117,118,118m,119,120,120m,121,122I [from 93Nb, 100Mo(24Mg, X), (32S, X), (34S, X)]; measured γ(θ), oriented nuclei. 117,118,119,120,121,122I level deduced μ, shape characteristics.
doi: 10.1007/BF02072689
1987WA17 J.Phys.(London) G13, L195 (1987) P.M.Walker, C.J.Ashworth, I.S.Grant, V.R.Green, J.Rikovska, T.L.Shaw, N.J.Stone E0 Transitions in the Light Tellurium Isotopes: Evidence for intruder states RADIOACTIVITY 118,120,122I(β+), (EC) [from 93Nb(32S, X), (34S, X), E=160-175 MeV]; measured I(ce), γγ-coin, γ linear polarization. 118,120,122Te deduced levels, J, π, γ-branching, ICC, transition strength ratios.
doi: 10.1088/0305-4616/13/9/005
1986DA02 J.Phys.(London) B19, L7 (1986) Multiconfiguration Dirac-Fock Approach to the Fine-Structure Splitting in the 3s3p Configuration of the Magnesium Sequence ATOMIC PHYSICS Z=13-50; calculated Mg sequence fine structure intervals. Multi-configuration Dirac-Fock approach.
doi: 10.1088/0022-3700/19/1/002
1986EA01 J.Phys.(London) G12, L205 (1986) D.A.Eastham, P.M.Walker, J.R.H.Smith, J.A.R.Griffith, D.E.Evans, S.A.Wells, M.J.Fawcett, I.S.Grant Optical Isotope Shifts of 80,82Sr from Coincidence Laser Spectroscopy NUCLEAR MOMENTS 80,82Sr; measured isotope shifts. 84,82,80Sr deduced rms charge radii differences. Ultra sensitive laser fluorescence technique.
doi: 10.1088/0305-4616/12/9/003
1986GR06 Phys.Lett. 173B, 115 (1986) V.R.Green, N.J.Stone, T.L.Shaw, J.Rikovska, K.S.Krane, P.M.Walker, I.S.Grant Iodine Magnetic Moments: Shape coexistence and N = 64 subshell closure RADIOACTIVITY 117,118,119,120,120m,121I(β-); 118mI(β-), (IT); 122I(EC); measured γ(θ), low temperature nuclear orientation; deduced μ.
doi: 10.1016/0370-2693(86)90229-7
1986GR16 Phys.Lett. 177B, 159 (1986) V.R.Green, C.J.Ashworth, J.Rikovska, T.L.Shaw, N.J.Stone, P.M.Walker, I.S.Grant The NMR of 116gSb Cryogenically Oriented On-Line in Iron RADIOACTIVITY 116Sb(EC), (β+) [from 93Nb(28Si, X), E=145 MeV]; measured NMR, oriented nuclei; deduced μ.
doi: 10.1016/0370-2693(86)91046-4
1985RA19 Z.Phys. A321, 599 (1985) G.-E.Rathke, K.Rykaczewski, R.Kirchner, O.Klepper, V.T.Koslowsky, E.Roeckl, D.Schardt, I.S.Grant, P.O.Larsson, A.Plochocki, J.Zylicz, P.Tidemand-Petersson Decay Properties of the New Proton-Rich Nucleus 104Sn: Mass determinations beyond the proton drip line RADIOACTIVITY 104Sn(β+), (EC) [from 50Cr(58Ni, 2n2p), E=4.68 MeV/nucleon]; measured Eγ, Iγ, γγ-, γ(X-ray)-coin; deduced Q(EC), T1/2. 104In deduced levels, (β+/(β++EC)) ratios. 108Te, 109I, 112Xe, 113Cs deduced mass excess. Other data input. NUCLEAR REACTIONS 50Cr(58Ni, 2n2p), E=4.68 MeV/nucleon; measured Eγ, Iγ, γγ-, γ(X-ray)-coin.
doi: 10.1007/BF01432436
1985RY02 Z.Phys. A322, 263 (1985) K.Rykaczewski, I.S.Grant, R.Kirchner, O.Klepper, V.T.Koslowsky, P.O.Larson, E.Nolte, G.Nyman, E.Roeckl, D.Schardt, L.Spanier, P.Tidemand-Petersson, E.F.Zganjar, J.Zylicz The Gamow-Teller Transitions in the 96Pd → 96Rh Decay RADIOACTIVITY 96Pd(EC), (β+) [from 60Ni(40Ca, xnyp), E=167 MeV]; measured Eγ, Iγ, γγ-coin; deduced Q(EC), mass excess, (β+/(EC+β+)) branching ratios. 96Rh deduced levels, J, π, γ-multipolarity, Gamow-Teller transition strengths.
doi: 10.1007/BF01411890
1985SH04 Phys.Lett. 153B, 221 (1985) T.L.Shaw, V.R.Green, N.J.Stone, J.Rikovska, P.M.Walker, S.Collins, S.A.Hamada, W.D.Hamilton, I.S.Grant On-Line Nuclear Orientation of 118I and the Identification of the g9/2 Intruder Orbital RADIOACTIVITY 118,118mI(β+), (EC) [from 93Nb(32S, xnyp), E=175 MeV]; measured γγ-coin, γγ(θ), γ(θ), oriented nuclei; deduced μ. 118Te deduced level, J, π, K, γ-multipolarity, possible shape coexistence role.
doi: 10.1016/0370-2693(85)90535-0
1985SH16 Hyperfine Interactions 22, 539 (1985) T.L.Shaw, V.R.Green, N.J.Stone, P.M.Walker, W.D.Hamilton, S.Collins, I.Grant, J.Rikovska Nuclear Orientation and Coincidence Studies of 118I and 118Cs Isotopes RADIOACTIVITY 118,118mI(β-), 118,118mCs(β+), (EC) [from 93Nb(32S, X), (34S, X), E=175 MeV]; measured γγ(θ), γ(θ), oriented nuclei in Fe. 118I deduced isomer μ. 118Te deduced levels, γ-branching, J, π. 118Xe deduced transition energy.
doi: 10.1007/BF02064022
1984EA01 Z.Phys. A318, 243 (1984) D.A.Eastham, P.M.Walker, J.A.R.Griffith, D.E.Evans, J.G.England, I.S.Grant Optical Isotope Shifts of 146Sm and 151Sm NUCLEAR MOMENTS 146,151Sm; measured optical isotope shifts; deduced rms nuclear radii. Resonance fluorescence spectrum.
doi: 10.1007/BF01413476
1984EA02 J.Phys.(London) G10, L271 (1984) D.A.Eastham, J.G.England, D.E.Evans, M.J.Fawcett, I.S.Grant, J.A.R.Griffith, G.W.A.Newton, P.M.Walker Optical Isotope Shift and Hyperfine Structure of 153Sm RADIOACTIVITY 153Sm(β-) [from 152Sm neutron irradiation]; measured optical isotope shift, hfs. 146,147,148,149,150,151,152,153,154Sm deduced rms charge radii relative to 144Sm.
doi: 10.1088/0305-4616/10/12/002
1982JO03 J.Phys.(London) G8, 1405 (1982) M.G.Johnston, I.S.Grant, P.Misaelides, P.J.Nolan, P.Peuser, R.Kirchner, O.Klepper, E.Roeckl, P.Tidemand-Petersson The Decay Scheme of 109Sb RADIOACTIVITY 109Sb(β+), (EC) [from 92Mo(20Ne, xnyp), E=190 MeV; 58Ni(58Ni, xnyp), E=290 MeV]; measured Eγ, Iγ, T1/2, γγ-, γ(X-ray)-, γβ-coin, Q(EC); deduced log ft. 109Sn deduced levels. 112Sb(β+), (EC) [from 92Mo(20Ne, xnyp), E=190 MeV; 58Ni(58Ni, xnyp), E=290 MeV]; measured β+-endpoint energies, Q(EC). Helium jet transport.
doi: 10.1088/0305-4616/8/10/011
1982PL05 Nucl.Phys. A388, 93 (1982) A.Plochocki, J.Zylicz, R.Kirchner, O.Klepper, E.Roeckl, P.Tidemand-Petersson, I.S.Grant, P.Misaelides Masses of very Neutron-Deficient Isotopes in the Cadmium-to-Cesium Region RADIOACTIVITY 104Cd(β+), (EC), 104In(β+), (EC), 105Sn(EC), (β+), 106Sn(EC), (β+), 106Sb(EC), (β+), 109Sb(EC), (β+), 109Te(EC), (β+p), (α), (β+), 110Te(β+), (EC), (α), 112Te(β+), (EC), 110I(β+), (β+p), (α), 113I(β+), (α), 113Xe(β+), (β+p), (EC), (α), 114Cs(β+), (α), (β+p) [from 58Ni(58Ni, xnyp)]; measured Eα, β-delayed Ep, βγ-, βp-coin; deduced Qα, Q(EC), (Q(EC)-Sp), mass excess. On-line mass separation, enriched targets, surface barrier Si, plastic scintillator, Ge(Li) detectors.
doi: 10.1016/0375-9474(82)90510-3
1982SH24 Nucl.Phys. A390, 351 (1982) J.H.Shea, J.L.Durell, G.S.Foote, I.S.Grant The Interaction of 605 MeV 63Cu with 197Au NUCLEAR REACTIONS 197Au(63Cu, X), E=605 MeV; measured fragment kinetic energies, masses, σ(fragment θ), deep inelastic events; deduced σ(total), fission yields following fusion.
doi: 10.1016/0375-9474(82)90165-8
1981MI12 Z.Phys. A301, 199 (1981) P.Misaelides, P.Tidemand-Petersson, U.J.Schrewe, I.S.Grant, R.Kirchner, O.Klepper, I.C.Malcolm, P.J.Nolan, E.Roeckl, W.-D.Schmidt-Ott, J.L.Wood The α- and β-Decay of 187Pb RADIOACTIVITY 187Pb [from 142Nd(48Ti, 3n), E=235 MeV; 107Ag(84Kr, 3np)]; measured Eγ, Iγ, γγ-, αγ-, γ(X-ray)-coin, Eα, Iα, T1/2(α). 187Tl deduced levels, T1/2, J, π. 183Hg deduced levels, J, π, γ-multipolarity.
doi: 10.1007/BF01416294
1981PL05 Phys.Lett. 106B, 285 (1981) A.Plochocki, J.Zylicz, R.Kirchner, O.Klepper, E.Roeckl, P.Tidemand-Petersson, I.S.Grant, P.Misaelides, W.-D.Schmidt-Ott Measurements of Proton Separation-Energies close to the Proton Drip Line in the Antimony-Cesium Region RADIOACTIVITY 114Cs [from 58Ni(58Ni, np), E=290 MeV]; measured Ip, Ep, β+p-coin; deduced Q(EC)-S(p), mass excess. 110I, 106Sb; deduced mass excess, S(p). Analysis of Qα data.
doi: 10.1016/0370-2693(81)90537-2
1980CU02 J.Phys.(London) G6, 127 (1980) J.G.Cuninghame, J.A.B.Goodall, J.E.Freeman, G.W.A.Newton, V.J.Robinson, J.L.Durell, G.S.Foote, I.S.Grant, M.Rathle Isomer Ratios in Fission Fragments at High Excitation NUCLEAR REACTIONS 209Bi(12C, X), E=75-112 MeV; 196Pt(12C, X), E=79-105 MeV; 204Pb(α, X), E=49-79 MeV; measured isomer yield ratios for 120,124,126,128Sb, 84Br. Evaporation model.
doi: 10.1088/0305-4616/6/1/018
1980NI08 Phys.Rev. C22, 617 (1980) L.Nikkinen, B.P.Pathak, L.Lessard, I.S.Grant Independent Yields of Rb, In, Cs Isotopes in the Proton-Induced Fission of 232Th NUCLEAR REACTIONS 232Th(p, F), E=29, 59, 75, 97 MeV; measured independent σ(E) for 116,117,118,119,120,121,122,123,124,125,96,97Rb, 131,132,133,134,135,136,137,138,139,140,141,142,143,144Cs; deduced total neutron number per fission event.
doi: 10.1103/PhysRevC.22.617
1979BR11 J.Inorg.Nucl.Chem. 41, 617 (1979) C.L.Branquinho, S.M.A.Hoffmann, G.W.A.Newton, V.J.Robinson, H.-Y.Wang, I.S.Grant, J.A.B.Goodall Excitation Functions and Isomer Ratios in the Reactions 93Nb(α, xn)(X = 1-4) NUCLEAR REACTIONS 93Nb(α, n), E=15-25 MeV; 93Nb(α, 2n), E=15-50 MeV; 93Nb(α, 3n), E=40-70 MeV; measured σ(E), isomeric ratio; deduced reaction mechanisms.
doi: 10.1016/0022-1902(79)80343-7
1979BR16 J.Inorg.Nucl.Chem. 41, 791 (1979) C.L.Branquinho, S.M.A.Hoffmann, G.W.A.Newton, V.J.Robinson, I.S.Grant, J.A.B.Goodall Spallation Cross Sections in the System 93Nb + 4He NUCLEAR REACTIONS 92Nb(α, 5n), (α, 3np), (α, 2p), (α, α'n), (α, α'xn), E=15-72 MeV; measured production σ(E) for 92Tc, 93mMo, 95m,95Nb, 90m,90Nb, 89m,89Nb. Compound nucleus model with pre-equilibrium nucleon emission.
doi: 10.1016/0022-1902(79)80267-5
1979GR21 J.Phys.(London) G5, 1741 (1979) Isomer Ratios in Antimony and Tellurium Isotopes NUCLEAR REACTIONS 115In(α, n), (α, 3n), 118,120,122,124Sn(α, np), 118,120Sn(α, 3n), E=16.6-38.4 MeV; measured σ. 116,118,120,122,124,126Sb, 119,121Te deduced isomeric yield ratio. Sharp cutoff model.
doi: 10.1088/0305-4616/5/12/013
1979SH15 Nucl.Phys. A327, 207 (1979) J.H.Shea, J.L.Durell, G.S.Foote, I.S.Grant The Interaction of 538 MeV 56Fe with 238U NUCLEAR REACTIONS 238U(56Fe, X), E=538 MeV; measured masses, kinetic energies, σ(θ), deep inelastic events; deduced reaction mechanism.
doi: 10.1016/0375-9474(79)90325-7
1978DU22 S.Afr.J.Phys. 1, 153 (1978) J.L.Durell, G.S.Foote, I.S.Grant, J.H.Shea The Interaction of 9.6 MeV/A 63Cu and 84Kr with 197Au NUCLEAR REACTIONS 197Au(84Kr, X), (63Cu, X), E=9.6 MeV/nucleon; measured σ(θ) for quasi-elastic, deep-inelastic, fission-like events; deduced L(max), L(critical).
1977CH24 J.Inorg.Nucl.Chem. 39, 1915 (1977) K.C.Chan, B.P.Pathak, L.Nikkinen, L.Lessard, I.S.Grant Independent Yields of Indium and Gallium in the Proton Induced Fission Of Natural Uranium NUCLEAR REACTIONS 238U(p, F), E=30-98.6 MeV; measured σ(E, A, Z).
doi: 10.1016/0022-1902(77)80516-2
1977ES01 Phys.Rev. C15, 319 (1977) R.A.Esterlund, D.Molzahn, R.Brandt, P.Patzelt, P.Vater, A.H.Boos, M.R.Chandratillake, I.S.Grant, J.D.Hemingway, G.W.A.Newton Search for Long-Lived Superheavy Elements in the Reaction System 238U + 9.6-MeV/Nucleon 63,65Cu NUCLEAR REACTIONS 238U(63Cu, X), (65Cu, X), E=9.6 MeV/nucleon; measured σ for production of superheavy elements, 254Cf.
doi: 10.1103/PhysRevC.15.319
1977RE09 Phys.Rev.Lett. 39, 171 (1977) U.Reus, A.M.H.Watzig, R.A.Esterlund, P.Patzelt, I.S.Grant Mass-Yield Distributions in the Reaction of 56Fe Ions with 238U NUCLEAR REACTIONS 238U(56Fe, X), E=538 MeV; measured σ(A), quasielastic transfer, quasifission, fusion-fission σ.
doi: 10.1103/PhysRevLett.39.171
1976FR06 J.Inorg.Nucl.Chem. 38, 941 (1976) J.E.Freeman, A.K.A.R.Ahmed, G.W.A.Newton, V.J.Robinson, K.Gregory, I.S.Grant Radiochemical Studies of Charge Distribution and Dispersion in the 12C-Induced Fission of 209Bi NUCLEAR REACTIONS 209Bi(12C, F), E ≤ 115 MeV; measured radiochemical yields of Sb, Y, Cd, Nb.
doi: 10.1016/0022-1902(76)80002-4
1973EA01 Nucl.Phys. A208, 119 (1973) Alpha Decay of Neutron-Deficient Isotopes of Tungsten RADIOACTIVITY 163,164W [from 144,147Sm(24Mg, xn)], measured Eα, T1/2; 162W [from 144Sm(24Mg, 6n)], measured Eα. NUCLEAR REACTIONS 144Sm(24Mg, xn), 147Sm(24Mg, xn), E=110-204 MeV; measured σ(E). Enriched target.
doi: 10.1016/0375-9474(73)90738-0
1970CO03 Nucl.Phys. A141, 532 (1970) P.M.Cockburn, L.J.B.Goldfarb, I.S.Grant, H.E.Reed The Dynamics of Three α-Particle Decay from an Unpolarized Source NUCLEAR REACTIONS 11B(p, 3α), E=0.68 MeV; measured αα-coin. 8Be deduced resonance parameters.
doi: 10.1016/0375-9474(70)90985-1
1967CO19 Phys.Letters 25B, 111 (1967) A Detailed Study of the First Excited State of 8Be NUCLEAR STRUCTURE 7Li, 8Be; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90194-3
1967CO29 Nucl.Sci.Appl. 3, No.2, 10 (1967) The First Excited State of Be8 NUCLEAR STRUCTURE 8Be, 7Li, 11B; measured not abstracted; deduced nuclear properties.
1960GR21 Proc.Phys.Soc.(London) 76, 737 (1960) NUCLEAR STRUCTURE 8Be; measured not abstracted; deduced nuclear properties.
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