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NSR database version of May 1, 2024.

Search: Author = A.Bockisch

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1984BR24      Nucl.Instrum.Methods 224, 112 (1984)

G.Braun, A.Bockisch, W.Neuwirth

Lifetime of the 0₂⁺ State of ⁷²Ge Determined by Delayed Auto-Coincidence of a Ge(Li) Detector

NUCLEAR REACTIONS ⁷²Ge(n, n'γ), E=fast; measured Eγ, Iγ, delayed autocoincidence spectra. ⁷²Ge level deduced T_1/2. Ge(Li) detector irradiation technique, (d, t) neutron generator, ²⁴¹Am/Be sources.

doi: 10.1016/0167-5087(84)90454-X
Citations: PlumX Metrics

1982KE01      Nucl.Phys. A376, 246 (1982)

J.Keinonen, K.P.Lieb, H.P.Hellmeister, A.Bockisch, H.Emling

Coulomb Excitation and Lifetime Measurements of the 2₁⁺ States in ^76,82,84Kr

NUCLEAR REACTIONS ⁶³Cu(¹⁹F, 2nα), E=58 MeV; measured recoil. ²⁷Al, ^64,66Zn, ^70,72,74,76Ge(⁸²Kr, ⁸²Kr'), (⁸⁴Kr, ⁸⁴Kr'), E=115, 118 MeV; measured Coulomb excitation, σ(E), DSA; deduced stopping power for Kr in Al, Zn, Ge, Ge in Ge, Zn in Zn. ^76,82,84Kr level deduced B(E2), T_1/2.

doi: 10.1016/0375-9474(82)90063-X
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1981MI08      Z.Phys. A300, 97 (1981)

M.Miller, A.M.Kleinfeld, A.Bockisch, K.Bharuth-Ram

The Analysis of Elastic and Inelastic Scattering of Alpha Particles using a Folding Potential

NUCLEAR REACTIONS ^{110,112,114,116}Cd, ¹²⁴Te(α, α), (α, α'), E=10-17 MeV; measured σ(Eα, θ); deduced folding potential parameters. ^{110,112,114,116}Cd deduced rms radius. Effective α-nucleon interaction.

doi: 10.1007/BF01412620
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1980BO05      Phys.Lett. 90B, 61 (1980)

A.Bockisch, M.Miller, K.P.Lieb, K.Heyde

Identification of the Missing f₅/₂ State in ²⁰¹Hg by Coulomb Excitation

NUCLEAR REACTIONS ²⁰¹Hg(α, α'), E=15 MeV; ²⁰¹Hg(¹⁶O, ¹⁶O'), E=35-64 MeV; measured σ(Eγ), Coulomb excitation. ²⁰¹Hg deduced level, γ-branching, J, π, B(E2). One quasiparticle core-coupling model.

doi: 10.1016/0370-2693(80)90051-9
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1979BO02      Z.Phys. A289, 231 (1979)

A.Bockisch, K.Bharuth-Ram, A.M.Kleinfeld, K.P.Lieb

Oblate Shapes of ^200,202,204Hg

NUCLEAR REACTIONS Hg(¹⁶O, ¹⁶O'), E=56-64 MeV; measured relative γ-yield following Coulomb excitation. ^200,202,204Hg deduced quadrupole moment, oblate shapes. ^{196,198,200,202,204}Hg levels deduced B(E2). Natural target.

doi: 10.1007/BF01435944
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1979BO16      Z.Phys. A291, 245 (1979)

A.Bockisch, K.Bharuth-Ram, A.M.Kleinfeld, K.P.Lieb

Reorientation Effect Measurements of Even Mercury Isotopes

NUCLEAR REACTIONS ¹⁹⁸Hg(α, α'), E=13, 15, 16 MeV; ¹⁹⁸Hg(¹⁶O, ¹⁶O'), E=56, 58, 60 MeV; Hg(α, α'), E=15 MeV; Hg(¹⁶O, ¹⁶O'), E=56-64 MeV; measured Eγ, Iγ, multiple Coulomb excitation, reorientation effects, particle spectra. ¹⁹⁸Hg deduced quadrupole moment. ^198,200,202Hg deduced B(E2), oblate shapes. Triaxial rotation, anharmonic vibration interpretation.

doi: 10.1007/BF01409190
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1979BO28      Z.Phys. A292, 265 (1979)

A.Bockisch, M.Miller, A.M.Kleinfeld, A.Gelberg, U.Kaup

Reorientation Effect Measurements and Multiple Coulomb Excitation in ¹⁰²Ru

NUCLEAR REACTIONS ¹⁰²Ru(α, α'), E=8.5, 9.0 MeV; ¹⁰²Ru(¹⁶O, ¹⁶O'), E=38-42 MeV; measured σ(E, θ), reorientation effect, multiple Coulomb excitation. ¹⁰²Ru levels deduced quadrupole moment, B(E2). Interacting boson model interpretation. Enriched target.

doi: 10.1007/BF01547471
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1979HA16      Phys.Lett. 83B, 169 (1979)

L.Hasselgren, C.Fahlander, J.E.Thun, A.Bockisch, F.J.Bergmeister

A Determination of the Sign of P₃ = M₀+_{1 2}+₁ M₂+_{1 2}+₂ M₂+_{2 0}+₁ for ¹⁹⁴Pt

NUCLEAR REACTIONS ¹⁹⁴Pt(¹⁶O, ¹⁶O'γ), E=70 MeV; measured Eγ, Iγ, ¹⁶Oγ-coin, ¹⁶Oγ(θ) following Coulomb excitation. ¹⁹⁴Pt deduced Coulomb interference term to be negative.

doi: 10.1016/0370-2693(79)90677-4
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1977KL05      Nucl.Phys. A283, 526 (1977)

A.M.Kleinfeld, A.Bockisch, K.P.Lieb

Reorientation Effect and Multiple Coulomb Excitation Measurements of ¹³⁴Ba

NUCLEAR REACTIONS ¹³⁴Ba(α, α'), E=11.3 MeV; ¹³⁴Ba(¹²C, ¹²C'), E=35 MeV; ¹³⁴Ba(¹⁸O, ¹⁸O'), E=52.5 MeV; ¹³⁴Ba(¹⁶O, ¹⁶O'), E=48, 49.5, 52.5 MeV; measured Coulomb excitation. ¹³⁴Ba levels deduced quadrupole moment, B(E2).

doi: 10.1016/0375-9474(77)90556-5
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1977LA16      Nucl.Phys. A292, 301 (1977)

J.Lange, A.T.Kandil, J.Neuber, C.D.Uhlhorn, H.Von Buttlar, A.Bockisch

Properties of Excited States in ¹⁰²Pd

NUCLEAR REACTIONS ¹⁰²Pd(p, p'γ), E=8 MeV; measured Ep, Eγ, p'γ(θ). ¹⁰²Pd deduced levels, J, δ, B(E2) ratios. ¹⁰²Pd(¹⁶O, ¹⁶O'), E=37 MeV; measured Coulomb excitation. ¹⁰²Pd deduced B(E2), quadrupole moment. Enriched targets.

doi: 10.1016/0375-9474(77)90376-1
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1976BO12      Nucl.Phys. A261, 498 (1976)

A.Bockisch, A.M.Kleinfeld

Reorientation Effect Measurements of ¹²²Te and ¹³⁰Te

NUCLEAR REACTIONS ^122,130Te(α, α'), E=10-11 MeV; ^122,130Te(¹⁶O, ¹⁶O'), E=30-54 MeV; measured σ(E(¹⁶O), E(¹⁶O')), σ(Eα, Eα'). ^122,130Te deduced quadrupole moment, B(E2). Enriched targets.

doi: 10.1016/0375-9474(76)90163-9
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1976FA02      Phys.Lett. 60B, 347 (1976)

C.Fahlander, L.Hasselgren, J.E.Thun, A.Bockisch, A.M.Kleinfeld, A.Gelberg, K.P.Lieb

A Direct Determination of the Sign of the Interference Term in the Coulomb Excitation of ¹⁰²Ru

NUCLEAR REACTIONS ¹⁰²Ru(¹⁶O, ¹⁶O'γ), E=45 MeV; measured ¹⁶O'γ-coin, γγ(θ). ¹⁰²Ru level deduced quadrupole moment.

doi: 10.1016/0370-2693(76)90747-4
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