References quoted in the ENSDF dataset: 91ZR ADOPTED LEVELS, GAMMAS
45 references found.
Clicking on a keynumber will list datasets that reference the given article.
Phys.Rev. 105, 1929 (1957); See Also 57Br89
E.Brun, J.Oeser, H.H.Staub
Magnetic Moment and Spin of Zr91
Nucl.Phys. 64, 458 (1965)
N.Auerbach, I.Talmi
Energy Levels, Configuration Mixing and Proton Neutron Interaction in the Zr Region
doi: 10.1016/0029-5582(65)90571-7
Nucl.Phys. 75, 17 (1966)
J.Vervier
Effective Nucleon-Nucleon Interactions in the Y, Zr, Nb, Mo and Tc Isotopes
NUCLEAR STRUCTURE 96Zr, 95Tc, 95Zr, 95Mo, 95Nb, 94Tc, 94Zr, 94Mo, 94Nb, 96Nb, 97Mo, 96Mo, 97Tc, 96Tc, 97Nb, 98Mo, 99Tc, 89Y, 90Y, 90Zr, 91Nb, 91Zr, 93Nb, 93Tc, 93Y, 93Zr, 93Mo, 92Nb, 92Mo, 92Y, 92Zr, 91Y; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(66)90746-2
Phys.Lett. 37B, 363 (1971)
L.A.Fajardo, J.R.Ficenec, W.P.Trower, I.Sick
Elastic Electron-Zirconium Scattering
NUCLEAR REACTIONS 90,91,92,94,96Zr(e, e), E=300 MeV; measured σ(θ). 90,91,92,94,96Zr deduced nuclear charge distribution parameters.
doi: 10.1016/0370-2693(71)90203-6
Nucl.Phys. A165, 533 (1971)
J.E.Glenn, H.W.Baer, J.J.Kraushaar
Spectroscopy of States in 91Zr from γ-Ray Transitions Observed in the 88Sr(α, nγ)91Zr Reaction
NUCLEAR REACTIONS 87,88Sr(α, nγ), Eα=10.3-13.5 MeV; measured Eγ, σ(Eα;Eγ), γγ-coin. 90,91Zr deduced levels, J. Natural, enriched targets; Ge(Li) detector.
doi: 10.1016/0375-9474(71)90468-4
Nucl.Phys. A168, 539 (1971)
T.Paradellis, S.Hontzeas, H.Blok
Unified-Model Calculations in Some Zr Isotopes
NUCLEAR STRUCTURE 91,92,93,94,95Zr; calculated level, S for (d, p). Unified model.
doi: 10.1016/0375-9474(71)90546-X
Z.Phys. 259, 37 (1973)
G.Vanden Berghe, K.Heyde, M.Waroquier
Core Polarization Corrections to Magnetic Dipole Moments and Transitions
NUCLEAR STRUCTURE 87Rb, 87Sr, 89Y, 91Zr, 113In, 115Sn, 123Sb, 139,141Ce; calculated μ, B(M1).
Phys.Rev. C10, 173 (1974)
S.S.Glickstein, G.Tessler
Neutron Inelastic Scattering from 91Zr
NUCLEAR REACTIONS 91Zr(n, n'γ), E=1.27-6.19 MeV; measured σ(E, Eγ). 91Zr deduced levels, J, π.
Nucl.Phys. A224, 411 (1974)
V.G.Soloviev, C.Stoyanov, A.I.Vdovin
Semi-Microscopic Calculation of the Level Density in Spherical Nuclei
NUCLEAR STRUCTURE 50,51Ti, 53,54,55Cr, 55,57,58Fe, 59,61,62,63,65Ni, 65,67,68,69Zn, 71,73,74,75,77Ge, 75,77,78,79,81,83Se, 85,87,88,89Sr, 91,92,93,95,97Zr, 96,97,98,99,101Mo, 100,102Ru, 106Pd, 112,113,114Cd, 113,115,116,117,118,119,120,121,123,125Sn, 123,124,126,129,131Te, 132,136Xe, 131,135,136,137,138,139Ba, 137,139,141,143Ce, 143,144,145,146,147,149Nd, 145,148,149Sm, 195,196,197,199Pt, 199,200,201,202,203Hg, 205,207Pb; calculated density of states.
doi: 10.1016/0375-9474(74)90696-4
Nucl.Phys. A253, 301 (1975)
D.H.Gloeckner
Shell-Model Systematics of the Zirconium and Niobium Isotopes
NUCLEAR STRUCTURE 92,93,94,95,96,97Nb, 90,91Y, 91,92,93,94,95,96Zr; calculated levels, systematics, parentage.
doi: 10.1016/0375-9474(75)90484-4
Nucl.Phys. A253, 189 (1975)
S.S.Ipson, K.C.McLean, W.Booth, J.G.B.Haigh, R.N.Glover
Experimental and Shell-Model Studies of the Reactions 91Zr(d, p)92Zr and 90Zr(t, p)92Zr
NUCLEAR REACTIONS 91Zr(d, p), E=12 MeV; 90Zr(t, p), E=11.85 MeV; measured σ(Ep, θ). 92Zr deduced levels, L, (2j+1)S, L, J, π. Enriched targets. 91,92Zr shell-model calculations.
doi: 10.1016/0375-9474(75)90127-X
Nucl.Phys. A257, 135 (1976)
C.V.K.Baba, D.B.Fossan, T.Faestermann, F.Feilitzsch, M.R.Maier, P.Raghavan, R.S.Raghavan, C.Signorini
Lifetime and g-Factor Results for the 13/2- 1985 keV Level in 91Nb And the 15/2- 2288 keV Level in 91Zr
NUCLEAR REACTIONS 89Y(α, 2nγ), E=21 MeV; 88Sr(α, nγ), E=16 MeV; measured αγ(θ), αγ(t). 91Nb, 91Zr levels deduced g, T1/2. Natural target. NaI(Tl), Ge(Li) detectors.
doi: 10.1016/0375-9474(76)90479-6
Phys.Rev. C13, 1900 (1976)
B.A.Brown, P.M.S.Lesser, D.B.Fossan
Properties of High-Spin States in 91Nb and 91Zr via 6Li-Induced Reactions
NUCLEAR REACTIONS 88Sr(6Li, 3n), (6Li, 2np), E=34 MeV; measured γγ-coin, σ(Eγ, θ, t). 91Nb, 91Zr deduced levels, J, π, T1/2, δ, B(E2), γ-branching, effective charges. Natural target, Ge(Li), Si(Li) detectors.
Z.Phys. A286, 125 (1978)
S.Buttgenbach, R.Dicke, H.Gebauer, R.Kuhnen, F.Traber
Hyperfine Structure of Seven Atomic Levels of 91Zr and the 91Zr Nuclear Electric Quadrupole Moment
NUCLEAR MOMENTS 91Zr; measured hfs; deduced quadrupole moment.
Nucl.Phys. A321, 415 (1979)
D.S.Chuu, M.M.King Yen, Y.Shan, S.T.Hsieh
Shell-Model Studies of the 90Y, 91Zr, 92Nb and 93Mo Nuclei
NUCLEAR STRUCTURE 90Y, 91Zr, 92Nb, 93Mo; calculated energy levels, S, E2 reduced width. Shell model, surface δ-interaction.
doi: 10.1016/0375-9474(79)90134-9
Nucl.Phys. A371, 393 (1981)
J.Nag, M.K.Pal
Core Polarization and Magnetic Moment of some Odd-Mass Nuclei Around N = 50
NUCLEAR STRUCTURE 85,87Kr, 87,89Sr, 91Zr, 89Y; calculated μ. Core polarization, modified TDA.
doi: 10.1016/0375-9474(81)90054-3
Bull.Am.Phys.Soc. 27, No.7, 727, EC3 (1982)
P.Raghavan, Z.Z.Ding, R.S.Raghavan
g-Factor of the 21/2+ Isomeric Level of 91Zr
NUCLEAR REACTIONS 82Se(13C, 4n), E=40 MeV; measured γ(θ, H, t). 91Zr deduced isomer g.
Nucl.Phys. A404, 106 (1983)
J.Nag, M.K.Pal
Exchange Magnetic Moments of some Odd-Mass Nuclei
NUCLEAR STRUCTURE 91Zr, 89Sr, 87Kr; calculated μ. Core polarization.
doi: 10.1016/0375-9474(83)90417-7
Phys.Rev.Lett. 54, 2592 (1985)
P.Raghavan, M.Senba, Z.Z.Ding, A.Lopez-Garcia, B.A.Brown, R.S.Raghavan
E2 Effective Charges of g9/2 Nucleons Derived from Quadrupole Moments of High-Spin Isomers in 88,90,91Zr and 90,92,94Mo
NUCLEAR REACTIONS 74,76,77,78,80,82Se(12C, xn), (13C, xn), E=48 MeV; 74,76,77,78,80,82Se(16O, xn), E=56 MeV; measured γ(θ, H, t). 88,90,91Zr deduced isomer static quadrupole moment. 90,92,94Mo deduced isomer static quadrupole moments, ratios.
doi: 10.1103/PhysRevLett.54.2592
J.Phys.(London) G13, 1037 (1987)
H.Stanczyk
Average Partial Radiation Widths of Neutron Resonances Calculated by Semi Classical Description
NUCLEAR STRUCTURE 26Mg, 40Ar, 53Cr, 56,57Fe, 60,61Ni, 91Zr, 93,99,101Mo, 102Ru, 104Rh, 116In, 136Ba, 169Er, 170Tm, 174Yb, 178Hf, 182Ta, 196Pt, 207,208Pb; calculated average electric, magnetic dipole partial radiation widths. Semi-classical method.
doi: 10.1088/0305-4616/13/8/011
Zh.Eksp.Teor.Fiz. 94, 9 (1988); Sov.Phys.JETP 67, 1089 (1988)
Yu.P.Gangrsky, S.G.Zemlyanoi, B.K.Kuldzhanov, K.P.Marinova, B.N.Markov, Hoang Thi Kim Hue, Chan Kong Tam
Determination of the Differences between the Charge Radii of Zirconium Nuclei Using Laser-Excited Resonance Fluorescence
NUCLEAR MOMENTS 90,91,92,94,96Zr; measured optical isotope shifts. 90,92,94,96Zr deduced rms charge radii differences, deformation parameters.
Program and Theses, Proc.38th Ann.Conf.Nucl.Spectrosc.Struct.At.Nuclei, Baku, p.74 (1988)
Yu.P.Gangrsky, S.G.Zemlyanoy, B.K.Kuldzhanov, K.P.Marinova, B.N.Markov, Khoang Tkhi Kim Khueh, Chan Kong Tam
Measurements of Charge Radius Differences of Zirconium Nuclei using Resonance Laser Fluorescence Method
NUCLEAR MOMENTS 90,91,92,94Zr; measured isotope shifts; deduced charge radius differences. Resonance laser fluorescence method.
Phys.Rev. C40, 1398 (1989)
R.J.Furnstahl, C.E.Price
Relativistic Hartree Calculations of Odd-A Nuclei
NUCLEAR STRUCTURE 15N, 15,17O, 17F, 39K, 39,41Ca, 41Sc, 89Y, 91Zr, 207Pb, 209Bi; calculated magnetic moments. Relativistic Hartree approach.
NUCLEAR REACTIONS 15N, 17O, 209Bi(e, e), E not given; calculated magnetic form factor. Relativistic Hartree approach.
At.Data Nucl.Data Tables 42, 189 (1989)
P.Raghavan
Table of Nuclear Moments
COMPILATION Z=1-99; compiled μ, electric quadrupole moments.
doi: 10.1016/0092-640X(89)90008-9
Phys.Rev. A48, 173 (1993)
L.Young, C.A.Kurtz, D.R.Beck, D.Datta
Hyperfine-Structure Studies of Zr II: Experimental and relativistic configuration-interaction results
NUCLEAR MOMENTS 91Zr; measured hfs; deduced parameters. Laser-rf double resonance method.
Eur.Phys.J. D 4, 39 (1998)
S.Bouazza, J.Dembczynski, E.Stachowska, G.Szawiola, J.Ruczkowski
Reanalysis and Semi-Empirical Predictions of the Hyperfine Structure of 91ZrI in the Model Space (4d + 5s)4
NUCLEAR MOMENTS 91Zr; analyzed previous hfs data; deduced quadrupole moment.
Eur.Phys.J. A 3, 237 (1998)
I.P.Johnstone, I.S.Towner
Effective Magnetic Dipole Operators for 88Sr and 90Zr Closed-Shell Cores
NUCLEAR STRUCTURE 88Sr, 90Zr; calculated effective g-factors, magnetic dipole operators. 90,91Zr, 91,92Nb, 92,93Mo, 93,94Tc, 94,95Ru, 96Pd; calculated magnetic moments; deduced two-body core polarization, meson exchange current effects.
J.Chem.Phys. 110, 10715 (1999)
S.A.Beaton, M.C.L.Gerry
Rotational Spectra and Hyperfine Constants of ZrO and ZrS
NUCLEAR MOMENTS 91Zr; measured hfs; deduced parameters. 90,91,92,94,96Zr; measured molecular spectra.
Program and Thesis, Proc.49th Ann.Conf.Nucl.Spectrosc.Struct.At.Nuclei, Dubna, p.98 (1999)
Yu.P.Gangrsky, S.G.Zemlyanoy, B.N.Markov, K.P.Marinova
Charge Radii of Nuclei Near the Neutron Closed Shells
NUCLEAR MOMENTS 39,40,41,42,46,47,48Ca, 48,49,50Ti, 84,85,86,87,88Kr, 86,87,88,89,90Sr, 90,91,92Zr, 136,137,138,139,140Ba, 138,140,142Ce, 140,141,142,143,144Nd, 142,143,144,145,146Sm, 204,205,206Hg, 206,207,208,209,210Pb; measured mean square radii difference. Laser resonance fluorescence method.
J.Phys.(London) B33, 2355 (2000)
S.Bouazza, D.S.Gough, P.Hannaford, M.Wilson
Hyperfine Structure of Odd-Parity Levels in 91Zr I
NUCLEAR MOMENTS 91Zr; measured hfs; deduced parameters.
doi: 10.1088/0953-4075/33/12/316
Phys.Rev. C62, 064605 (2000)
A.A.Cowley, G.F.Steyn, S.S.Dimitrova, P.E.Hodgson, G.J.Arendse, S.V.Fortsch, G.C.Hillhouse, J.J.Lawrie, R.Neveling, W.A.Richter, J.A.Stander, S.M.Wyngaardt
Multistep Direct Mechanism in the (p(pol), 3He) Inclusive Reaction on 59Co and 93Nb at an Incident Energy of 100 MeV
NUCLEAR REACTIONS 59Co, 93Nb(polarized p, 3He), E=100 MeV; measured σ(E, θ), Ay(θ); deduced one-step, multistep process contributions, other reaction mechanism features. Comparison with model predictions.
doi: 10.1103/PhysRevC.62.064605
Phys.Rev. C62, 054608 (2000)
P.E.Garrett, L.A.Bernstein, J.A.Becker, K.Hauschild, C.A.McGrath, D.P.McNabb, W.Younes, M.B.Chadwick, G.D.Johns, R.O.Nelson, W.S.Wilburn, E.Tavukcu, S.W.Yates
92Mo(n, xnypzαγ) Reactions for Neutron Energies up to 250 MeV
NUCLEAR REACTIONS 92Mo(n, xnypzα)92Mo/91Mo/90Mo/89Mo/88Mo/92Nb/91Nb/90Nb/89Nb/88Nb/91Zr/90Zr/89Zr/88Zr/87Zr/86Zr/88Y/86Y/85Y/84Y/86Sr/85Sr/84Sr/83Sr/82Sr/80Sr, E=2-250 MeV; measured Eγ, Iγ(t), γγ-coin; deduced excitation functions, isomer yields. Comparison with model predictions.
doi: 10.1103/PhysRevC.62.054608
Phys.Rev. C61, 064318 (2000)
A.Holt, T.Engeland, M.Hjorth-Jensen, E.Osnes
Application of Realistic Effective Interactions to the Structure of the Zr Isotopes
NUCLEAR STRUCTURE 90,91,92,93,94,95,96,97,98Zr; calculated levels, J, π, configurations, B(E2). Shell model, realistic effective interactions, comparisons with data.
doi: 10.1103/PhysRevC.61.064318
Chem.Phys.Lett. 318, 222 (2000)
V.Kello, P.Pyykko, A.J.Sadlej, P.Schwerdtfeger, J.Thyssen
The Nuclear Quadrupole Moment of 91Zr from Molecular Data for ZrO and ZrS
NUCLEAR MOMENTS 91Zr; analyzed molecular quadrupole coupling constants; deduced quadrupole moment. Comparison with theory.
doi: 10.1016/S0009-2614(00)00031-2
Nucl.Sci.Eng. 134, 50 (2000)
G.Leinweber, J.Burke, C.R.Lubitz, H.D.Knox, N.J.Drindak, R.C.Block, R.E.Slovacek, C.J.Werner, N.C.Francis, Y.Danon, B.E.Moretti
Neutron Capture and Total Cross-Section Measurements and Resonance Parameter Analysis of Zirconium up to 2.5 keV
NUCLEAR REACTIONS Zr(n, X), (n, γ), E < 2.5 keV; measured capture and transmission σ. 91,96Zr deduced resonance parameters.
J.Phys.(London) G29, 2247 (2003)
H.L.Thayer, J.Billowes, P.Campbell, P.Dendooven, K.T.Flanagan, D.H.Forest, J.A.R.Griffith, J.Huikari, A.Jokinen, R.Moore, A.Nieminen, G.Tungate, S.Zemlyanoi, J.Aysto
Collinear laser spectroscopy of radioisotopes of zirconium
NUCLEAR MOMENTS 87,87m,88,89,89m,91,92,94,96,97,98,99,100,101,102Zr; measured hfs, isotope shifts; deduced μ, quadrupole moments, radii. Collinear laser spectroscopy.
doi: 10.1088/0954-3899/29/9/318
At.Data Nucl.Data Tables 87, 185 (2004)
I.Angeli
A consistent set of nuclear rms charge radii: properties of the radius surface R(N, Z)
COMPILATION A=1-248; compiled, analyzed charge radii.
doi: 10.1016/j.adt.2004.04.002
Eur.Phys.J. A 25, Supplement 1, 187 (2005)
J.Billowes
Developments in laser spectroscopy at the Jyvaskyla IGISOL
NUCLEAR MOMENTS 86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102Zr; measured charge radii. 176Yb; measured isomer shift. Ion-beam cooler, laser spectroscopy.
doi: 10.1140/epjad/i2005-06-099-7
Nucl.Phys. A758, 126c (2005)
J.A.Church, L.Ahle, L.A.Bernstein, J.Cooper, F.S.Dietrich, J.Escher, C.Forssen, H.Ai, H.Amro, M.Babilon, C.Beausang, J.Caggiano, A.Heinz, R.Hughes, E.McCutchan, D.Meyer, C.Plettner, J.Ressler, V.Zamfir
Determining neutron capture cross sections with the Surrogate Reaction Technique: Measuring decay probabilities with STARS
NUCLEAR REACTIONS 92Zr(α, α'), (α, 3HeX), (α, tX), (α, dX), (α, pX), E=51 MeV; measured particle spectra. 92Zr(α, α'), (α, xnα), E=51 MeV; measured Eγ, Iγ, αγ-coin. 90,91,92Zr deduced transitions. Surrogate reaction technique.
doi: 10.1016/j.nuclphysa.2005.05.169
Atlas of Neutron Resonances, 5ed., Resonance Parameters and Thermal Cross Sections, Z = 1-100, Elsevier, Amsterdam (2006)
S.F.Mughabghab
COMPILATION Z=1-100; compiled, evaluated thermal neutron induced σ, resonance parameter data.
Nucl.Instrum.Methods Phys.Res. B261, 938 (2007)
J.A.Cizewski, R.Hatarik, K.L.Jones, S.D.Pain, J.S.Thomas, M.S.Johnson, D.W.Bardayan, J.C.Blackmon, M.S.Smith, R.L.Kozub
(d, pγ) Reactions and the surrogate reaction technique
NUCLEAR REACTIONS 2H(90Zr, pγ), (80Se, pγ), E=4 MeV/nucleon; measured Eγ, Ep, pγ-coinc.
doi: 10.1016/j.nimb.2007.03.028
Phys.Rev. C 77, 035802 (2008)
G.Tagliente, for the n_TOF Collaboration
Neutron capture cross section of 90Zr: Bottleneck in the s-process reaction flow
NUCLEAR REACTIONS 90Zr(n, γ), E<250 MeV; measured σ, neutron resonances. Eγ, Iγ, n-TOF spallation source. R-matrix analysis.
doi: 10.1103/PhysRevC.77.035802
INDC(NDS)-0594 (2011)
N.J.Stone
Table of nuclear magnetic dipole and electric quadrupole moments
COMPILATION Z=1-99, N=1-254; compiled experimental data on nuclear magnetic and electrical quadrupole moments.
Chin.Phys.C 36, 1603 (2012)
M.Wang, G.Audi, A.H.Wapstra, F.G.Kondev, M.MacCormick, X.Xu, B.Pfeiffer
The AME2012 atomic mass evaluation (II). Tables, graphs and references
COMPILATION A=1-295; compiled, evaluated atomic mass data.
Phys.Rev. C 87, 041303 (2013)
D.Lonardoni, S.Gandolfi, F.Pederiva
Effects of the two-body and three-body hyperon-nucleon interactions in Λ hypernuclei
NUCLEAR STRUCTURE A=5-91; 5He, 17O, 41Ca, 91Zr; calculated hyperon separation energies for closed-shell hypernuclei, binding energies using auxiliary field diffusion Monte Carlo (AFDMC) method. Necessity of inclusion of the three-body hyperon-NN interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.041303