References quoted in the ENSDF dataset: 155GD COULOMB EXCITATION

23 references found.

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1955MA77

Phys.Rev. 100, 813 (1955)

H.Mark, G.T.Paulissen

Electric Excitation of Certain Rare-Earth Nuclei by Protons

doi: 10.1103/PhysRev.100.813

1956BJ41

Z.Naturforsch. 11a, 273 (1956)

J.H.Bjerregaard, U.Meyer-Berkhout

Coulomb-Anregung der Rotationszustande der Kerne Gd¹⁵⁵ und Gd¹⁵⁷

1956HE78

Phys.Rev. 104, 981 (1956)

N.P.Heydenburg, G.M.Temmer

Coulomb Excitation and Cascade Decay of Rotational States in Odd-Mass Nuclei

doi: 10.1103/PhysRev.104.981

1957BE56

Phys.Rev. 105, 1524 (1957)

E.M.Bernstein, H.W.Lewis

Internal Conversion Electrons Following Coulomb Excitation of Highly Deformed Nuclei

doi: 10.1103/PhysRev.105.1524

1958CH36

Phys.Rev. 112, 518 (1958)

E.L.Chupp, J.W.M.DuMond, F.J.Gordon, R.C.Jopson, H.Mark

Precision Determination of Nuclear Energy Levels in Heavy Elements

doi: 10.1103/PhysRev.112.518

1958RA12

Nuclear Phys. 6, 451 (1958)

V.Ramsak, M.C.Olesen, B.Elbek

Coulomb Excitation Cross Sections of Gadolinium Isotopes from Inelastic Scattering Measurements

doi: 10.1016/0029-5582(58)90195-0

1959DE29

Helv.Phys.Acta 32, 377 (1959); Erratum Helv.Phys.Acta 32, 658 (1959)

J.de Boer, M.Martin, P.Marmier

Gammawinkelverteilungen bei elektrischer Anregung deformierter ug-Kerne

1962GO23

Phys.Rev. 127, 2151 (1962)

G.Goldring, H.M.Loebenstein, R.Barloutaud

Branching Ratios and Magnetic Dipole Transition Probabilities in Odd-A Rotational Nuclei

NUCLEAR STRUCTURE ¹⁶⁷Er, ¹⁸¹Ta, ¹⁷³Yb, ¹⁷⁵Lu, ¹⁷⁷Hf, ¹⁵³Eu, ¹⁵⁷Gd, ¹⁵⁵Gd; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.127.2151

1963EL06

Thesis, University of Copenhagen (1963)

B.Elbek

Determination of Nuclear Transition Probabilities by Coulomb Excitation

NUCLEAR STRUCTURE ²³²Th, ²³⁸U, ¹⁵⁹Tb, ¹⁶²Dy, ¹⁶⁹Tm, ¹⁶⁵Ho, ¹⁶⁴Dy; measured not abstracted; deduced nuclear properties.

1966AS02

Nucl.Phys. 76, 336 (1966)

D.Ashery, A.E.Blaugrund, R.Kalish

E2/M1 Mixing Ratios and K Conversion Coefficients in Odd-Mass Rotational Nuclei

NUCLEAR REACTIONS ¹⁵⁵Gd, ¹⁶⁷Er, ¹⁷³Yb, ¹⁷⁵Lu, ¹⁷⁹Hf, ¹⁸¹Ta, ¹⁸⁵Re, ¹⁸⁷Re, ¹⁹⁵Pt(p, p'γ), ¹⁵⁹Tb(α, α'γ); measured Eγ, γγ-, Xγ-coin, pγγ(θ), ICC. ¹⁵⁵Gd, ¹⁶⁷Er, ¹⁷³Yb, ¹⁷⁵Lu, ¹⁷⁹Hf, ¹⁸¹Ta, ^185,187Re, ¹⁹⁵Pt, ¹⁵⁹Tb γ-mixing, ICC. Enriched targets.

doi: 10.1016/0029-5582(66)90027-7

1966BO16

Phys.Letters 22, 627 (1966); Erratum Phys.Lett. 23, 491 (1966)

F.Boehm, G.Goldring, G.B.Hagemann, G.D.Symons, A.Tveter

A Determination of the Gyromagnetic Ratios of Some Odd-A Deformed Nuclei from Branching Ratio Measurements

NUCLEAR STRUCTURE ¹⁸¹Ta, ¹⁶⁵Ho, ¹⁶³Dy, ¹⁶⁷Er, ¹⁶⁹Tm, ¹⁵⁹Tb, ¹⁶¹Dy, ¹⁵⁵Gd, ¹⁵⁷Gd, ¹⁷¹Yb, ¹⁷³Yb, ¹⁷⁵Lu, ¹⁵³Eu; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(66)90683-4

1969TV01

Nucl.Phys. A134, 599 (1969)

A.Tveter, B.Herskind

Coulomb Excitation of Rotational and Vibrational States in ¹⁶⁷Er, ¹⁶³Dy and ¹⁵⁵Gd

NUCLEAR REACTIONS ¹⁶⁷Er, ¹⁶³Dy, ¹⁵⁵Gd(¹⁶O, ¹⁶O'γ), E = 36-52 MeV; measured σ(Eγ). ¹⁶⁷Er, ¹⁶³Dy, ¹⁵⁵Gd deduced levels, B(E2). Enriched targets.

doi: 10.1016/0375-9474(69)90024-4

1978BR20

Phys.Rev. C18, 666 (1978)

P.F.Brown, C.Baktash, J.O'Brien, J.X.Saladin

B(E2) Values in ¹⁵⁵Gd, ¹⁶¹Dy, ¹⁶³Dy, ¹⁶⁷Er, and ¹⁷⁵Lu

NUCLEAR REACTIONS ¹⁵⁵Gd, ¹⁶⁷Er, ^161,163Dy, ¹⁷⁵Lu(α, α), (α, α'), E=9.0-13.5 MeV; measured σ(E)/σ(E, Eα'), Coulomb excitation. ¹⁵⁵Gd, ^161,163Dy, ¹⁶⁷Er, ¹⁷⁵Lu deduced quadrupole moment, B(E2).

doi: 10.1103/PhysRevC.18.666

1986SC25

J.Phys.(London) G12, 411 (1986)

H.H.Schmidt, W.Stoffl, T.von Egidy, P.Hungerford, H.J.Scheerer, K.Schreckenbach, H.G.Borner, D.D.Warner, R.E.Chrien, R.C.Greenwood, C.W.Reich

The Level Structure of ¹⁵⁵Gd from (n, γ), (d, p) and (d, t) Studies

NUCLEAR REACTIONS ¹⁵⁴Gd(n, γ), E ≤ 24 keV; ¹⁵⁴Gd(d, p), ¹⁵⁶Gd(d, t), E=14, 20 MeV; measured Eγ, Iγ, I(ce), σ(Ep), σ(Et). ¹⁵⁵Gd levels deduced J, π, γ-branching, ICC, γ-multipolarity, neutron binding energy, rotational band structure, configuration.

doi: 10.1088/0305-4616/12/5/008

1992KU15

Phys.Rev. C46, 1257 (1992); Erratum Phys.Rev. C63, 029901 (2001)

H.Kusakari, M.Oshima, A.Uchikura, M.Sugawara, A.Tomotani, S.Ichikawa, H.Iimura, T.Morikawa, T.Inamura, M.Matsuzaki

Electromagnetic Transition Probabilities in the Natural-Parity Rotational Bands of ^155,157Gd

NUCLEAR REACTIONS ^155,157Gd(⁵⁸Ni, ⁵⁸Ni'γ), E=240 MeV; ^155,157Gd(⁸¹Br, ⁸¹Br'γ), E=305 MeV; measured Eγ, Iγ, γ(θ), γγ(θ), recoil distance Doppler shift, (particle)γ-coin. ^155,157Gd levels deduced δ, T_1/2, B(M1), B(E2). Enriched target. Cranking model analysis.

doi: 10.1103/PhysRevC.46.1257

1992OSZX

Japan Atomic Energy Res.Inst.Tandem Linac VDG, Ann.Rept., 1991, p.147 (1992)

M.Oshima, H.Kusakari, A.Uchikura, A.Tomotani, M.Sugawara, S.Ichikawa, H.Iimura, T.Morikawa, T.Inamura, M.Matsuzaki

Electromagnetic Transition Probabilities in the Natural-Parity Rotational Bands of ^155,157Gd

NUCLEAR REACTIONS ^155,157Gd(⁷⁴Ge, ⁷⁴Ge'), E not given; measured Eγ, Iγ following Coulomb excitation. ^155,157Gd deduced B(M1), B(E2). Cranking shell model.

1993KUZY

RIKEN-92, p.10 (1993)

H.Kusakari, M.Oshima, A.Uchikura, M.Sugawara, A.Tomotani, S.Ichikawa, H.Iimura, T.Morikawa, T.Inamura, M.Matsuzaki

Electromagnetic Transition Probabilities in the Natural-Parity Rotational Bands of ^155,157Gd

NUCLEAR REACTIONS ^155,157Gd(⁵⁸Ni, ⁵⁸Ni'), E=240 MeV; ^155,157Gd(⁸¹Br, ⁸¹Br'), E=305 MeV; measured Eγ, γ(θ) following Coulomb excitation. ^155,157Gd deduced levels, J, π, δ(E2/M1), γ-branching, T_1/2, B(λ).

1996KIZV

Japan Atomic Energy Res.Inst.Tandem VDG Ann.Rept., 1995, p.18 (1996); JAERI-Review 96-011 (1996)

M.Kidera, M.Oshima, T.Hayakawa, K.Furutaka, Y.Hatsukawa, M.Matsuda, H.Iimura, H.Kusakari, Y.Igari, M.Sugawara

High-Spin States in ^155,157Gd

NUCLEAR REACTIONS ^155,157Gd(⁹⁰Zr, ⁹⁰Zr'), E=390 MeV; measured Eγ, Iγ(θ), γ⁹⁰Zr-coin following Coulomb excitation. ^155,157Gd deduced high-spin levels, J, π, B(E2)/B(M1). Multiple Coulomb excitation.

1997KI16

J.Phys.Soc.Jpn. 66, 285 (1997)

M.Kidera, M.Oshima, Y.Hatsukawa, K.Furutaka, T.Hayakawa, M.Matsuda, H.Iimura, H.Kusakari, Y.Igari, M.Sugawara

Coulomb Excitation of ¹⁵⁵Gd

NUCLEAR REACTIONS ¹⁵⁵Gd(⁹⁰Zr, ⁹⁰Zr'), E=390 MeV; measured Eγ, Iγ, (particle)γ-coin following Coulomb excitation. ¹⁵⁵Gd deduced high-spin levels, J, π, B(λ).

1997KIZS

Kyushu Univ.Tandem Acc.Lab.Rept., 1995-1996, p.100 (1997); KUTL Report-6 (1997)

M.Kidera, M.Oshima, K.Furutaka, T.Hayakawa, Y.Hatsukawa, M.Matsuda, H.Iimura, H.Kusakari, M.Sugawara, Y.Igari

High-Spin States in ^{155, 157}Gd

NUCLEAR REACTIONS ^155,157Gd(⁹⁰Zr, ⁹⁰Zr'), E=390 MeV; measured Eγ, Iγ, (particle)γ-, γγ-coin following Coulomb excitation. ^155,157Gd deduced levels, J, π, B(E2)/B(M1). Si detector, HPGe array with BGO.

1997OSZZ

Japan Atomic Energy Res.Inst.Tandem VDG Ann.Rept., 1996, p.18 (1997); JAERI-Review 97-010 (1997)

M.Oshima, M.Kidera, Y.Hatsukawa, K.Furutaka, T.Hayakawa, M.Matsuda, H.Iimura, H.Kusakari, Y.Igari, M.Sugawara, T.Shizuma

Coulomb Excitation of ¹⁵⁵Gd

NUCLEAR REACTIONS ¹⁵⁵Gd(³²S, ³²S'), E=140 MeV; ¹⁵⁵Gd(⁵⁸Ni, ⁵⁸Ni'), E=240 MeV; ¹⁵⁵Gd(⁹⁰Zr, ⁹⁰Zr'), E=390 MeV; measured Eγ, Iγ, (projectile)γ-, γγ-coin following Coulomb excitation. ¹⁵⁵Gd deduced levels, J, π, band structure.

1998OSZZ

Japan Atomic Energy Res.Inst.Tandem VDG Ann.Rept., 1997, p.31 (1998); JAERI-Review 98-017 (1998)

M.Oshima, T.Hayakawa, Y.Hatsukawa, K.Furutaka, J.Katakura, M.Matsuda, H.Iimura, H.Kusakari, K.Terui, K.Myojin, D.Nishimiya, M.Sugawara, T.Shizuma

Enhanced Side-Band Population in Coulomb Excitation of ¹⁵⁵Gd

NUCLEAR REACTIONS ¹⁵⁵Gd(³²S, ³²S'), (⁵⁸Ni, ⁵⁸Ni'), E not given; measured side-band Coulomb excitation σ; deduced enhancement relative to calculation.

1998ST28

Nucl.Phys. A642, 361 (1998)

A.E.Stuchbery, G.J.Lampard, H.H.Bolotin

Spectroscopy of ¹⁵⁵Gd following Coulomb Excitation: Signature-independent M1 properties and evidence for octupole correlations

NUCLEAR REACTIONS ^155,156Gd(⁵⁸Ni, ⁵⁸Ni'), E=180, 220, 230 MeV; measured Iγ(θ, H, T) in thin polarized Fe, (particle)γ-, γγ-coin, DSA following Coulomb excitation. ¹⁵⁵Gd levels deduced g-factors, δ, T_1/2. Enriched target, thin-foil transient-field IMPAC technique.

NUCLEAR STRUCTURE ¹⁵⁵Gd calculated levels, B(E1), B(E2), B(M1), δ, g, signature-dependent g and B(M1). Particle-rotor model, octupole correlations.

doi: 10.1016/S0375-9474(98)00540-5