References quoted in the ENSDF dataset: 54FE ADOPTED LEVELS, GAMMAS
35 references found.
Clicking on a keynumber will list datasets that reference the given article.
Nucl.Phys. 62, 385 (1965)
J.J.Simpson, J.A.Cookson, D.Eccleshall, M.J.L.Yates
Coulomb Excitation of Ti50, Cr52 and Fe54 First Excited States
NUCLEAR REACTIONS 50Ti, 52Cr, 54Fe(16O, 16O'), E=31-41 MeV; measured σ(E;E(16O')). 50Ti, 52Cr, 54Fe deduced B(E2).
doi: 10.1016/0029-5582(65)90486-4
Yadern.Fiz. 6, 219 (1967); Soviet J.Nucl.Phys. 6, 160 (1968)
O.F.Afonin, A.P.Grinberg, I.K.Lemberg, I.N.Chugunov
Coulomb Excitation of Light and Medium Nuclei at Supra-Barrier Energies
NUCLEAR STRUCTURE 23Na, 27Al, 29Si, 35Cl, 31P, 37Cl, 53Cr, 54Fe, 52Cr, 51V, 45Sc, 50Ti, 49Ti, 48Ti, 47Ti; measured not abstracted; deduced nuclear properties.
Phys.Rev. C2, 2241 (1970)
S.Cochavi, D.B.Fossan, S.H.Henson, D.E.Alburger, E.K.Warburton
E2 Transition Strengths between (1f7/2)+,-2 States of Ca42, Ti50, and Fe54
NUCLEAR REACTIONS 39K(α, pγ), E=8.3 MeV; measured recoil distance, σ(Eγ). 42Ca level deduced T1/2, B(E2).
RADIOACTIVITY 50Sc, 54Co; measured βγ-delay. 50Ti, 54Fe levels deduced T1/2, B(E2).
Z.Phys. 230, 337 (1970)
W.Kreische, W.Lampert, G.Loos, D.Weltle
Untersuchung der Niedrigliegenden Niveaus des 54Fe durch die (p, p'γγ)-Reaktion
NUCLEAR REACTIONS 54Fe(p, p'γγ), E=6.6 MeV; measured σ(Eγ, θ(γ)), γγ-triple correlation. 54Fe deduced levels, J, π.
AECL-3996, p.16 (1971)
W.G.Davies, J.S.Forster, I.M.Szoghy, D.Ward
Coulomb Excitation of N = 28 Nuclei
NUCLEAR REACTIONS 50Ti, 51V, 52Cr, 54Fe(16O, 16O'γ), E=21, 24, 27, 30 MeV, (35Cl, 35Cl'γ), E=60, 70, 79 MeV; measured B(E2). 50Ti, 51V, 50,52Cr, 54,56Fe deduced B(E2).
Phys.Rev.Lett. 27, 1587 (1971)
R.Hensler, J.W.Tape, N.Benczer-Koller, J.R.MacDonald
Mean Lifetime and Magnetic Moment of the 2.95-MeV (6+) State of 54Fe
NUCLEAR REACTIONS 54Fe(p, p'γ), E=8.187 MeV; measured p'γ-delay, p'γ(θ, H, t). 54Fe level deduced T1/2, g, B(E2).
doi: 10.1103/PhysRevLett.27.1587
J.Phys.Soc.Jap. 30, 1252 (1971)
H.Saito, T.Nomura, T.Yamazaki
The Lifetime of the Lowest 6+ State in 54Fe and E2 Effective Charge
RADIOACTIVITY 54mCo; measured βγ-delay. 54Fe level deduced T1/2, B(E2), E2 effective charge.
Phys.Rev.Lett. 29, 504 (1972)
M.S.Moore, L.G.Miller, G.E.Stokes
Correlation between Fission-Channel Effects and Fragment Kinetic Energies
NUCLEAR REACTIONS, Fission 235U(n, F), E < 60 eV; measured relative yield of high-energy fission fragments.
doi: 10.1103/PhysRevLett.29.504
Phys.Rev. C6, 1224 (1972)
E.K.Warburton, D.E.Alburger
E0 Decay of the 2561-keV 0+ Level of 54Fe
NUCLEAR REACTIONS 54Fe(p, p'γ), E=7 MeV; measured Eγ, Iγ, β+β-(θ), I(β+β-). 54Fe deduced levels, γ-branching, J, π.
Nucl.Sci.Eng. 50, 311 (1973)
J.K.Dickens, G.L.Morgan, F.G.Perey
Neutron-Induced Gamma-Ray Production in Iron for the Energy Range 0.8 < E < 20 MeV
NUCLEAR REACTIONS 54,56Fe(n, Xγ), E=0.8-20 MeV; measured σ(E, Eγ, θ).
Nucl.Phys. A257, 29 (1976)
H.Lancman, R.J.Sparks, C.Van der Leun
Nuclear Resonance Fluorescence in 54Fe
NUCLEAR REACTIONS 54Fe(γ, γ), E=6.13 MeV; measured σ(Eγ), σ(θ), σ. 54Fe deduced level, J, Γ, decay scheme. Natural Fe scatterer.
doi: 10.1016/0375-9474(76)90472-3
J.Phys.(London) G2, L39 (1976)
J.R.Leigh, E.C.Pollacco, N.Shikazono, D.C.Weisser, C.Garrett
Differences in the Coulomb-Nuclear Interference Patterns Produced with 12C and 13C Ions
NUCLEAR REACTIONS 52Cr, 54Fe(12C, 12C), (12C, 12C'), (13C, 13C), (13C, 13C'), E=18-26 MeV; measured σ(E); deduced differences in Coulomb-nuclear interference patterns.
doi: 10.1088/0305-4616/2/3/005
Phys.Rev. C16, 899 (1977)
J.M.Brennan, N.Benczer-Koller, M.Hass, H.T.King
Magnetic Moments of the 2+ First Excited States of Even Iron Isotopes
NUCLEAR REACTIONS 54,56,58Fe(32S, 32S'), E=72 MeV; measured γ(θ, H). 54,58Fe levels deduced g.
Nucl.Phys. A291, 241 (1977)
C.Fahlander, K.Johansson, E.Karlsson, G.Possnert
The g-Factors of the First 2+ States in 50,54Cr, 54Fe and 70Ge
NUCLEAR REACTIONS 50,54Cr, 54Fe, 70Ge(16O, 16O'γ), E=36 MeV; measured 16O'γ(θ, B) in polarized Gd at 80° K. 50,54Cr, 54Fe, 70Ge deduced g for first 2+ states. 70,72,74Ge; reevaluated data; deduced g. IMPAC.
doi: 10.1016/0375-9474(77)90209-3
Phys.Lett. 76B, 51 (1978)
E.Dafni, J.W.Noe, M.H.Rafailovich, G.D.Sprouse
Static Moments of 54mFe and Perturbed Angular Distributions with Combined Dipole and Quadrupole Interactions
NUCLEAR REACTIONS 40Ca(16O, 2p), E=40 MeV; measured γ(θ, H, t). 54Fe level deduced g, quadrupole moment. TDPAD method.
doi: 10.1016/0370-2693(78)90097-7
Proc.Int.Conf. on Medium-Light Nuclei, Florence, Italy, 1977, P.Blasi, R.A.Ricci, Eds., p.458 (1978)
J.W.Noe, D.F.Geesaman, P.Gural, G.D.Sprouse
High-Spin 1p-3h States in 54Fe
NUCLEAR REACTIONS 40Ca(16O, 2p), E≈40 MeV; measured γγ(θ), oriented nuclei, γ(θ, H, t). 54Fe deduced high-spin states, T1/2, g. Shell model.
J.Phys.(Paris), Lett. 40, L-93 (1979)
G.Guillaume, P.Fintz
Vie Moyenne de Petat 8+ a 6, 38 MeV dans 54Fe
NUCLEAR REACTIONS 50Cr(6Li, pn), E=20 MeV; measured DSA, γn-coin. 54Fe levels deduced T1/2. E2 strengths discussed. Shell model.
Phys.Rev. C19, 2073 (1979)
E.C.Pollacco, C.Garrett, D.C.Weisser
Differences in 16O and 18O Induced Inelastic Scattering
NUCLEAR REACTIONS 52Cr, 54Fe(16O, 16O), (18O, 18O), E=30-42 MeV; measured σ(E). 52Cr, 54Fe level deduced optical model parameters, Coulomb, nuclear deformation parameters. DWBA analysis.
Nucl.Phys. A330, 173 (1979)
E.C.Pollacco, D.M.Parkinson, J.R.Leigh, D.C.Weisser, N.Shikazono, G.S.Foote, D.Branford
12C and 13C Induced Reactions on N = 28 Nuclei at Energies Near the Coulomb Barrier
NUCLEAR REACTIONS 48Ca, 50Ti, 52Cr, 54Fe(13C, 13C); 48Ca, 50Ti, 52Cr, 53Cr, 54Fe(12C, 12C); 52Cr, 54Fe(12C, 12C'); 52Cr, 54Fe(13C, 13C'); 48Ca, 50Ti, 52Cr, 54Fe(13C, 12C); 53Cr(12C, 13C); measured σ(E). 52Cr, 54Fe deduced B(E2), β of ion-ion potential. 49Ca, 51Ti, 53Cr, 55Fe levels deduced S. Enriched targets. DWBA analysis.
doi: 10.1016/0375-9474(79)90543-8
Nucl.Phys. A327, 295 (1979)
J.Styczen, E.Bozek, T.Pawlat, Zb.Stachura, F.A.Beck, C.Gehringer, B.Haas, J.C.Merdinger, N.Schulz, P.Taras, M. Toulemonde, J.P.Vivien, A.Muller-Arnke
High-Spin States in 50Ti, 52Cr and 54Fe
NUCLEAR REACTIONS 48Ca, 50Ti, 52Cr(α, 2nγ), E=24-33 MeV; measured Eγ, σ(E, θγ), linear polarization, γγ-coin, σ(θγ, t). 50Ti, 52Cr, 54Fe deduced levels, J, π, δ, T1/2. Enriched targets.
doi: 10.1016/0375-9474(79)90261-6
JYFL Ann.Rept., 1980, p.31 (1980)
A.Passoja, R.Julin, J.Kantele, J.Kumpulainen, M.Luontama, T.Salonen
E0-Decay Branches of Excited 0+ States in the f-p Shell
NUCLEAR REACTIONS 54Fe, 64,68Zn(p, p'), E=6.9 MeV; measured Eγ, Iγ, I(ce), T1/2, internal pair sum coincidence. 54Fe, 64,68Zn levels deduced B(E0)/B(E2), E0 decay branching.
Phys.Rev. C23, 244 (1981)
M.J.LeVine, E.K.Warburton, D.Schwalm
Static Quadrupole Moments for the 2+ States of 54,56,58Fe
NUCLEAR REACTIONS 56,58Fe(12C, 12C'), E=22 MeV; 56,58Fe(52Cr, 56Fe), (52Cr, 58Fe), E=110-120 MeV; 54Fe(16O, 16O'), E=28 MeV; 54Fe(40Ca, 40Ca'), E=86 MeV; measured σ(E(12C)), σ(E(16O)), target recoil, reorientation in Coulomb excitation. 54,56,58Fe levels deduced B(E2), quadrupole moment. Enriched targets, Q3D spectrometer.
Nucl.Phys. A410, 399 (1983); Erratum Nucl.Phys. A417, 564 (1984)
C.Djalali, N.Marty, M.Morlet, A.Willis, J.C.Jourdain, N.Anantaraman, G.M.Crawley, A.Galonsky, J.Duffy
Excitation of ΔL = 0 Spin-Flip Transitions in the N = 28 Isotones by 201 MeV Proton Inelastic Scattering
NUCLEAR REACTIONS 50Ti, 52Cr, 54Fe(p, p'), E=201 MeV; measured σ(θ). 50Ti, 52Cr, 54Fe deduced 1+ states. DWIA calculations.
doi: 10.1016/0375-9474(83)90633-4
Phys.Rev. C27, 602 (1983)
M.H.Rafailovich, E.Dafni, J.M.Brennan, G.D.Sprouse
Magnetic Moment of the 54Fe (10+) Level
NUCLEAR REACTIONS 45Sc(12C, 2np), E=40 MeV; measured γ(θ, H, t). 54Fe level deduced g, quadrupole moment, configuration.
Nucl.Phys. A414, 316 (1984)
M.Hass, E.Dafni, H.H.Bertschat, C.Broude, F.Davidovsky, G.Goldring, P.M.S.Lesser
Nuclear Polarization of High-Spin Levels and the Sign of the Quadrupole Moment of 54Fe(10+)
NUCLEAR REACTIONS 45Sc(12C, 2np), E=40 MeV; measured Iγ(θ, t), oriented nuclei. 54Fe deduced isomer quadrupole moment sign, magnitude. Multifoil array induced nuclear polarization, pulsed beam, recoil implantation into Zn, Cd.
doi: 10.1016/0375-9474(84)90648-1
Phys.Rev. C31, 2054 (1985)
D.I.Sober, B.C.Metsch, W.Knupfer, G.Eulenberg, G.Kuchler, A.Richter, E.Spamer, W.Steffen
Magnetic Dipole Excitations in the N = 28 Isotones 50Ti, 52Cr, and 54Fe
NUCLEAR REACTIONS 50Ti, 52Cr, 54Fe(e, e'), E=30-57 MeV; measured σ(θ), σ(E(e')). 50Ti, 52Cr, 54Fe levels deduced B(λ), transition radius, M1 total strength, fragmentation. Shell model calculations.
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
Z.Phys. A342, 17 (1992)
K.H.Speidel, J.Cub, U.Reuter-Knopp, W.Karle, H.Busch, S.Kremeyer, J.Gerber, F.Hagelberg
New Determination of the Magnetic Moment of the 54Fe(2+1) State
NUCLEAR REACTIONS 28Si(56Fe, 56Fe'), (54Fe, 54Fe'), E=150 MeV; measured (particle)γ-coin, (particle)γ(θ), γ-anisotropy following Coulomb excitation. 54Fe level deduced g-factor 2+. Transient magnetic fields, ferromagnetic Gd host.
Phys.Rev. C58, 2566 (1998)
I.Bikit, M.Krmar, J.Slivka, M.Veskovic, Lj.Conkic, I.Anicin
New Results on the Double β Decay of Iron
RADIOACTIVITY 54Fe(2EC); measured Eγ, Iγ(t); deduced 0ν accompanied two-EC decay T1/2 limits.
Phys.Rev. C62, 031301 (2000)
K.-H.Speidel, R.Ernst, O.Kenn, J.Gerber, P.Maier-Komor, N.Benczer-Koller, G.Kumbartzki, L.Zamick, M.S.Fayache, Y.Y.Sharon
Core Polarization in the Light of New Experimental g Factors of fp Shell, N = 28, Isotones
NUCLEAR REACTIONS C(50Ti, 50Ti'), E=110 MeV; C(54Fe, 54Fe'), E=130 MeV; measured Eγ, Iγ(θ, H, t) in magnetized Gd following projectile Coulomb excitation. 50Ti, 54Fe levels deduced g factors, T1/2. Transient field technique. Comparison with shell model predictions.
NUCLEAR STRUCTURE 49Sc, 50Ti, 51V, 52Cr, 53Mn, 54Fe, 55Co; calculated g factors. Shell model, several interactions compared. Comparisons with data.
doi: 10.1103/PhysRevC.62.031301
At.Data Nucl.Data Tables 78, 1 (2001)
S.Raman, C.W.Nestor, P.Tikkanen
Transition Probability from the Ground to the First-Excited 2+ State of Even-Even Nuclides
COMPILATION Z=4-100; compiled, evaluated B(E2) for transition from ground to first-excited 2+ states in even-even nuclides.
Bull.Rus.Acad.Sci.Phys. 70, 1805 (2006)
V.M.Khvastunov, V.V.Denyak, Yu.N.Ranyuk
Scattering of electrons by 54Fe and 56Fe nuclei in energy range of giant resonance
NUCLEAR REACTIONS 54,56Fe(e, e'), E=225 MeV; measured energy and angular distributions. Deduced reduced transition probabilities B(E1), B(E2), B(E3), B(E4), B(E5).
Phys.Rev. C 79, 024304 (2009); Publishers note Phys.Rev. C 80, 019908 (2009)
M.C.East, A.E.Stuchbery, S.K.Chamoli, J.S.Pinter, H.L.Crawford, A.N.Wilson, T.Kibedi, P.F.Mantica
Relative g-factor measurements in 54Fe, 56Fe, and 58Fe
NUCLEAR REACTIONS C(54Fe, 54Fe'), (56Fe, 56Fe'), (58Fe, 58Fe), E=110 MeV/nucleon; measured Eγ, Iγ(θ), γγ-, 12C-γ coin, precession angles. 54,56,58Fe; deduced g factors.
NUCLEAR MOMENTS 54,56,58Fe; measured g factors of first 2+ states of 54Fe and 58Fe relative to that of the first 2+ state in 56Fe using transient-field technique in Coulomb excitation in inverse kinematics. Comparison with shell-model calculations in fp model space.
doi: 10.1103/PhysRevC.79.024304
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.