References quoted in the ENSDF dataset: 191IR COULOMB EXCITATION

18 references found.

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1956DA40

Phys.Rev. 103, 1801 (1956)

R.H.Davis, A.S.Divatia, D.A.Lind, R.D.Moffat

Coulomb Excitation of Elements of Medium and Heavy Mass

doi: 10.1103/PhysRev.103.1801

1956HU49

Kgl.Danske Videnskab.Selskab, Mat.-Fys.Medd. 30, No.17 (1956)

T.Huus, J.H.Bjerregaard, B.Elbek

Measurement of Conversion Electrons from Coulomb Excitation of the Elements in the Rare Earth Region

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

1957MC34

Phys.Rev. 107, 1674 (1957)

F.K.McGowan, P.H.Stelson

Internal Conversion Coefficients for Pure E2 and Mixed E2 + M1 Transitions

doi: 10.1103/PhysRev.107.1674

1958MC02

Phys.Rev. 109, 901 (1958)

F.K.McGowan, P.H.Stelson

Yields, Angular Distributions, and Polarization of Gamma Rays from Coulomb Excitation

doi: 10.1103/PhysRev.109.901

1969AV03

Nucl.Phys. A135, 678 (1969)

R.Avida, M.B.Goldberg, G.Goldring, A.Sprinzak

Electromagnetic Moments of Transitions in ¹⁹¹Ir, ¹⁹³Ir Following Coulomb Excitation

NUCLEAR REACTIONS ^191,193Ir(¹⁶O, ¹⁶O'γ), E = 9-30 MeV; measured σ(E;Eγ). ^191,193Ir levels deduced transition probabilities, branching ratios. Enriched, natural targets. Ge(Li) detector.

doi: 10.1016/0375-9474(69)90012-8

1970AV02

Nucl.Phys. A147, 200 (1970)

R.Avida, I.Ben Zvi, P.Gilad, M.B.Goldberg, G.Goldring, K.H.Speidel, A.Sprinzak

Angular Correlation Measurements on ^191,193Ir Following Coulomb Excitation

NUCLEAR REACTIONS ^191,193Ir(¹⁶O, ¹⁶O'γ), E = 40 MeV; measured σ(Eγ, θ(γ)). ^191,193Ir levels deduced g, γ-mixing. Natural targets, Ge(Li) detectors.

doi: 10.1016/0375-9474(70)90522-1

1971NO01

Nucl.Phys. A162, 449 (1971)

P.Norgaard, K.M.Bisgard, K.Gregersen, P.Morgen

Inelastic Scattering of Deuterons and α-Particles on ¹⁹¹Ir and ¹⁹³Ir

NUCLEAR REACTIONS ^191,193Ir(d, d'), Ed=7.0 MeV, 12.1 MeV; ^191,193Ir(α, α'), Eα=16.6 MeV; measured σ(E'd, θ)σ(E'α, 90°). ^191,193Ir deduced levels, Q₀, J, π, B(E2). Enriched targets.

doi: 10.1016/0375-9474(71)90247-8

1971PR12

Nucl.Phys. A174, 497 (1971)

R.H.Price, M.W.Johns

Energy Levels in ¹⁹¹Ir

NUCLEAR REACTIONS ¹⁹¹Ir(¹⁶O, ¹⁶O'γ), E=25, 40, 65 MeV; measured Eγ, Iγ. ¹⁹¹Ir levels deduced B(E2).

RADIOACTIVITY ¹⁹¹Pt[from ¹⁹⁰Pt(n, γ)]; measured Eγ, Iγ, I(ce), K X-ray, γ-, γγ-coin; deduced log ft, Q. ¹⁹¹Ir deduced levels, J, π, ICC, γ-branching, γ-mixing.

doi: 10.1016/0375-9474(71)90399-X

1978BA38

Phys.Rev. C18, 131 (1978)

C.Baktash, J.X.Saladin, J.J.O'Brien, J.G.Alessi

Electromagnetic Properties of ¹⁹⁴Pt and the Question of its Triaxiality

NUCLEAR REACTIONS ¹⁹⁴Pt(α, α'), E=7-17.5 MeV; measured σ(E). ¹⁹⁵Pt(α, α'γ), E=16 MeV; ¹⁹⁴Pt(¹⁶O, ¹⁶O'γ), E=46, 54 MeV; measured particle γ-coin. ¹⁹⁴Pt deduced B(E2), B(E4), B(E3), quadrupole, hexadecapole moment. Enriched targets, Ge(Li) detector.

doi: 10.1103/PhysRevC.18.131

1981HUZU

Thesis, Univ.Pittsburgh (1981)

A.A.E.Hussein

The Electromagnetic Properties of ^191,193Ir

1984MU19

Nucl.Phys. A426, 144 (1984)

S.J.Mundy, J.Lukasiak, W.R.Phillips

The Spin(6) Scheme and Electromagnetic Transitions in ¹⁹¹Ir and ¹⁹³Ir

NUCLEAR STRUCTURE ^191,193Ir, ^{192,194,196,198}Pt; calculated levels, B(λ). Interacting boson-fermion model, Spin(6) scheme.

NUCLEAR REACTIONS Ir, Pt(p, p'), (α, α'), E=5-6 MeV; measured σ(Eγ, θ), Eγ, Iγ, Coulomb excitation. ^191,193Ir, ^{192,194,196,198}Pt deduced levels, B(λ), δ. Natural targets.

doi: 10.1016/0375-9474(84)90070-8

1986KO20

Nucl.Phys. A456, 349 (1986)

W.R.Kolbl, J.Billowes, J.Burde, J.A.G.De Raedt, M.A.Grace, A.Pakou

g-Factor and Lifetime Measurements in ^191,193Ir

NUCLEAR REACTIONS ^191,193Ir(³²S, ³²S'), E=89, 118 MeV; measured Coulomb excitation, γ(θ, H), γ(θ, t), recoil. ^191,193Ir levels deduced g, T_1/2. Transient field method, IMPAC technique.

doi: 10.1016/0375-9474(86)90398-2

1986MC01

Phys.Rev. C33, 855 (1986)

F.K.McGowan, N.R.Johnson, I.Y.Lee, W.T.Milner, C.Roulet, J.Hattula, M.P.Fewell, Y.A.Ellis-Akovali, R.M.Diamond, F.S.Stephens, M.W.Guidry

Test of the Triaxial Rotor Model and the Interacting Boson Fermion Approximation Model Description of Collective States in ¹⁹¹Ir

NUCLEAR REACTIONS ¹⁹¹Ir(⁴⁰Ar, ⁴⁰Ar'), E=160 MeV; ¹⁹¹Ir(¹³⁶Xe, ¹³⁶Xe'), E=617 MeV; measured Eγ, Iγ(θ) following Coulomb excitation. ¹⁹¹Ir deduced levels, J, π, B(λ).

doi: 10.1103/PhysRevC.33.855

1996ST22

Hyperfine Interactions 97/98, 479 (1996)

A.E.Stuchbery, S.S.Anderssen, E.Bezakova

IMPAC In-Beam and Out-of-Beam; g-Factors and pre-equilibrium effects following ion-implantation

NUCLEAR REACTIONS ^188,190,192Os, ^194,196,198Pt(¹⁶O, ¹⁶O'), E=36 MeV; ^194,196,198Pt(²⁸Si, ²⁸Si'), E=60 MeV; ^194,196,198Pt(³⁴S, ³⁴S'), E=80 MeV; ^188,190,192Os(³²S, ³²S'), E=80 MeV; ^191,193Ir(⁵⁸Ni, ⁵⁸Ni'), E=155, 180 MeV; measured γγ(θ, H), implanted recoil nuclei. ^191,193Ir, ^188,190,192Os levels deduced g factors.

2000BE07

Nucl.Phys. A669, 241 (2000)

E.Bezakova, A.E.Stuchbery, H.H.Bolotin, W.A.Seale, S.Kuyucak, P.Van Isacker

Electromagnetic Properties of Low-Excitation States in ¹⁹¹Ir and ¹⁹³Ir and Supersymmetry Schemes

NUCLEAR REACTIONS ^191,193Ir(⁵⁸Ni, ⁵⁸Ni'), E=155, 180 MeV; ^191,193Ir(⁶⁵Cu, ⁶⁵Cu'), E=130 MeV; ^191,193Ir(³²S, ³²S'), E=100 MeV; ^191,193Ir(¹⁶O, ¹⁶O'), E=40 MeV; measured Eγ, Iγ(θ, H, T) in polarized Gd, Fe following Coulomb excitation, (recoil)γ-, (particle)γ-coin. ^191,193Ir levels deduced g-factors, δ, T_1/2. Thin-foil transient-field IMPAC technique, recoil-distance lifetime measurement.

NUCLEAR STRUCTURE ^191,193Ir; calculated g-factors, B(M1), B(E2). Particle-triaxial-rotor model, supersymmetry models.

doi: 10.1016/S0375-9474(99)00565-5

2004STZZ

Priv.Comm. (2004)

A.Stuchbery

2006SI17

Nucl.Data Sheets 107, 1531 (2006)

B.Singh

Nuclear Data Sheets for A = 194

COMPILATION ¹⁹⁴Re, ¹⁹⁴Os, ¹⁹⁴Ir, ¹⁹⁴Pt, ¹⁹⁴Au, ¹⁹⁴Hg, ¹⁹⁴Tl, ¹⁹⁴Pb, ¹⁹⁴Bi, ¹⁹⁴Po, ¹⁹⁴At; compiled, evaluated structure data.

doi: 10.1016/j.nds.2006.05.004