Nuclear Science References (NSR)

NUCLEAR REACTIONS ²³²Th(⁵⁶Fe, X), E=362 MeV; ²³²Th(⁸⁶Kr, X), E=511 MeV; ²³²Th(¹³⁶Xe, X), E=830, 833 MeV; measured Eγ, Iγ(θ), γγ-coin; deduced transfer products yields and highest angular momentum value. GAMMASPHERE and other Ge detector arrays.

doi: 10.1088/0954-3899/26/2/102
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1996CO13 Acta Phys.Pol. B27, 213 (1996)

J.F.C.Cocks, D.J.Blumenthal, R.Broda, P.A.Butler, K.J.Cann, B.Crowell, B.Fornal, R.F.Janssens, G.D.Jones, P.M.Jones, R.Julin, S.Juutinen, T.L.Khoo, T.Lauritsen, D.Muller, D.Nisius, M.Piiparinen, A.Savelius, J.F.Smith

Population of Reflection-Asymmetric Nuclei by Multi-Nucleon Transfer Reactions

NUCLEAR REACTIONS ²³²Th(¹³⁶Xe, X), E=830 MeV; ²³²Th(⁵⁶Fe, X), E=362 MeV; measured γγ-coin; deduced fragment production yield vs mass, nucleons transfer mechanism.

1996LH05 Nucl.Instrum.Methods Phys.Res. A373, 415 (1996)

G.Lhersonneau, P.A.Butler, J.F.C.Cocks, A.Honkanen, M.Huhta, P.M.Jones, A.Jokinen, R.Julin, S.Juutinen, A.Lampinen, D.Muller, E.Makela, M.Oinonen, J.M.Parmonen, M.Piiparinen, A.Savelius, J.F.Smith, S.Tormanen, A.Virtanen, J.Aysto

High-Spin Isomers in Neutron-RIch Nuclei Studied with TARDIS-Array at IGISOL

RADIOACTIVITY ⁹⁷Y(β^-) [from ²³²Th(p, X), E=25 MeV]; measured Eγ, Iγ, γγ-coin. ⁹⁷Zr deduced transitions. Compton suppressed detector array TARDIS.

doi: 10.1016/0168-9002(96)00072-1
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1995PI09 Phys.Rev. C52, R1 (1995)

M.Piiparinen, A.Atac, S.J.Freeman, R.Julin, S.Juutinen, A.Lampinen, T.Lonnroth, D.Muller, J.Nyberg, G.Sletten, P.Tikkanen, S.Tormanen, A.Virtanen, C.T.Zhang, R.Wyss

Collectivity in ' Spherical ' ^143,144Eu Nuclei

NUCLEAR REACTIONS ¹¹⁰Pd(³⁷Cl, 3n), (³⁷Cl, 4n), E=140 MeV; measured Eγ, Iγ(θ), γγ-coin, γγ(t). ^143,144Eu deduced high-spin levels, J, π, T_1/2, B(E2) values, band structure, shape features. Enriched targets, array of Compton-suppressed Ge dedtectors, 4π BaF₂ ball, plunger. Total Routhian surface calculations.

doi: 10.1103/PhysRevC.52.R1
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1994JU04 Nucl.Phys. A573, 306 (1994)

S.Juutinen, R.Julin, M.Piiparinen, P.Ahonen, B.Cederwall, C.Fahlander, A.Lampinen, T.Lonnroth, A.Maj, S.Mitarai, D.Muller, J.Nyberg, P.Simecek, M.Sugawara, I.Thorslund, S.Tormanen, A.Virtanen, R.Wyss

Gamma-Ray Spectroscopy of ¹¹⁰Cd

NUCLEAR REACTIONS ⁹⁶Zr(¹⁸O, 4n), E=73 MeV; ¹⁰⁰Mo(¹³C, 3n), E=44 MeV; measured Eγ, Iγ(θ), γγ-coin, γγ(t). ¹¹⁰Cd deduced levels, J, π, T_1/2, γ-branching, B(M1)/B(E2) ratios, experimental Routhians, aligned momenta. Enriched targets, array of Compton-suppressed Ge detectors, BaF₂ ball. TRS and CSM calculations.

doi: 10.1016/0375-9474(94)90173-2
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1994JU05 Nucl.Phys. A577, 727 (1994)

S.Juutinen, P.Simecek, C.Fahlander, R.Julin, J.Kumpulainen, A.Lampinen, T.Lonnroth, A.Maj, S.Mitarai, D.Muller, J.Nyberg, M.Piiparinen, M.Sugawara, I.Thorslund, S.Tormanen, A.Virtanen

High-Spin States in ^109,111Cd and ¹⁰⁷Pd

NUCLEAR REACTIONS ⁹⁶Zr(¹⁸O, 3nα), (¹⁸O, 5n), (¹⁸O, 3n), E=73 MeV; ¹⁰⁰Mo(¹³C, 4n), E=44 MeV; ¹⁰⁹Ag(p, n), E=12-17.4 MeV; measured Eγ, Iγ, Iγ(θ), γγ-coin, γγ(t). ¹⁰⁷Pd, ^109,111Cd deduced high-spin levels, J, π, T_1/2, γ-branching, B(M1)/B(E2) ratios, experimental routhians, aligned angular momenta. Enriched targets, array of Compton-suppressed Ge detectors, BaF₂ ball. Total Routhian surface, cranked shell model calculations.

doi: 10.1016/0375-9474(94)90942-3
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1994MU18 Phys.Lett. 332B, 265 (1994)

D.Muller, A.Virtanen, R.Julin, S.Juutinen, A.Lampinen, M.Piiparinen, S.Tormanen, F.Christancho, A.P.Byrne, G.D.Dracoulis, B.Fabricius, C.Fahlander, A.Johnson, K.P.Lieb, J.Nyberg, I.Thorslund, R.Wyss

Deformation of Intruder Bands in ¹⁷⁹Ir

NUCLEAR REACTIONS ¹⁴⁶Nd(³⁷Cl, 4n), E=169 MeV; measured γγ-coin, DSA, recoil distance. ¹⁷⁹Ir deduced high-spin levels, J, π, T_1/2, intruder bands features, transition quadrupole moments.

doi: 10.1016/0370-2693(94)91252-1
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1994TH01 Nucl.Phys. A568, 306 (1994)

I.Thorslund, C.Fahlander, J.Nyberg, M.Piiparinen, R.Julin, S.Juutinen, A.Virtanen, D.Muller, H.Jensen, M.Sugawara

Transition Probabilities and Quadrupole Deformation Measured in ¹⁰⁸Cd

NUCLEAR REACTIONS ¹⁰⁰Mo(¹²C, 4n), E=54 MeV; measured Eγ, Iγ, γγ-coin. ¹⁰⁸Cd levels deduced B(E2), T_1/2, deformation β₂. Enriched targets, array of Compton-suppressed Ge-detectors, plunger. Total routhian surface calculations.

doi: 10.1016/0375-9474(94)90204-6
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1993PI01 Phys.Rev.Lett. 70, 150 (1993)

M.Piiparinen, P.Kleinheinz, J.Blomqvist, A.Virtanen, A.Atac, D.Muller, J.Nyberg, T.Ramsoy, G.Sletten

Two- to One -Phonon E3 Transition Strength in ¹⁴⁸Gd

NUCLEAR REACTIONS ¹³³Cs(¹⁹F, 4n), E=73.5 MeV; measured Eγ, Iγ, decay time. ¹⁴⁸Gd deduced levels, J, π, mean T_1/2, B(λ), configuration.

doi: 10.1103/PhysRevLett.70.150
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1993PI16 Nucl.Phys. A565, 671 (1993)

M.Piiparinen, R.Julin, S.Juutinen, A.Virtanen, P.Ahonen, C.Fahlander, J.Hattula, A.Lampinen, T.Lonnroth, A.Maj, S.Mitarai, D.Muller, J.Nyberg, A.Pakkanen, M.Sugawara, I.Thorslund, S.Tormanen

Lifetimes of Yrast States in ¹¹⁰Cd

NUCLEAR REACTIONS ¹⁰⁰Mo(¹³C, 3n), E=44 MeV; measured Eγ, Iγ, γγ-coin. ¹¹⁰Cd levels deduced B(E2) values, T_1/2. Enriched targets, array of Compton-suppressed Ge detectors, 4π BaF₂ ball, plunger.

doi: 10.1016/0375-9474(93)90052-Y
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1993SC13 Phys.Lett. 303B, 230 (1993)

W.Schmitz, H.Hubel, C.X.Yang, G.Baldsiefen, U.Birkental, G.Frohlingsdorf, D.Mehta, R.Musseler, M.Neffgen, P.Willsau, J.Gascon, G.B.Hagemann, A.Maj, D.Muller, J.Nyberg, M.Piiparinen, A.Virtanen, R.Wyss

Transition Quadrupole Moments of a Large-Deformation Intruder Band in ¹⁶³Lu

NUCLEAR REACTIONS ¹⁴⁷Sm(¹⁹F, X), E=85 MeV; measured γγ-coin, DSA, recoil distance. ¹⁶³Lu deduced levels, J, π, T_1/2, band structure, transition quadrupole moment. Cranked shell model.

doi: 10.1016/0370-2693(93)91425-M
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1993TH05 Nucl.Phys. A564, 285 (1993)

I.Thorslund, C.Fahlander, J.Nyberg, S.Juutinen, R.Julin, M.Piiparinen, R.Wyss, A.Lampinen, T.Lonnroth, D.Muller, S.Tormanen, A.Virtanen

The Role of the Shape Driving h_11/2 Neutron Orbital in ¹⁰⁸Cd

NUCLEAR REACTIONS ⁹⁶Zr(¹⁶O, 4n), E=74, 75 MeV; measured Eγ, Iγ, Iγ(θ), γγ-coin. ¹⁰⁸Cd deduced levels, J, π, γ-branching, B(M1)/B(E2) ratios, experimental routhians, aligned angular momentum. Enriched targets, array of Compton-suppressed Ge-detectors, total routhian surface calculations.

doi: 10.1016/0375-9474(93)90522-Y
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1991NO05 Z.Phys. A340, 411 (1991)

E.Nolte, T.Faestermann, A.Gillitzer, G.Korschinek, D.Muller, V.M.Novikov, A.A.Pomansky, A.Ljubicic, D.Miljanic

Test of the Pauli Exclusion Principle for Nucleons and Atomic Electrons by Accelerator Mass Spectrometry

doi: 10.1007/BF01290329
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1991NO08 J.Phys.(London) G17, S355 (1991)

E.Nolte, T.Brunner, T.Faestermann, A.Gillitzer, G.Korschinek, D.Muller, B.Schneck, D.Weselka, V.N.Novikov, A.A.Pomansky, A.Ljubicic, D.Miljanic, H.Vonach

Accelerator Mass Spectrometry for Tests of the Pauli Exclusion Principle and for Detection of ββ Decay Products

NUCLEAR REACTIONS ⁶⁰Ni(n, 2n), E=14.8 MeV; measured σ. Accelerator mass spectrometry technique.

RADIOACTIVITY ⁵⁹Ni(EC), (β⁺) [from ⁶⁰Ni(n, 2n), E=14.8 MeV]; measured T_1/2. Accelerator mass spectrometry technique.

doi: 10.1088/0954-3899/17/S/037
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1990JU01 Z.Phys. A336, 475 (1990)

S.Juutinen, R.Julin, P.Ahonen, C.Fahlander, J.Hattula, J.Kumpulainen, A.Lampinen, T.Lonnroth, D.Muller, J.Nyberg, A.Pakkanen, M.Piiparinen, I.Thorslund, S.Tormanen, A.Virtanen

High-Spin States in ¹¹⁰Cd

NUCLEAR REACTIONS ⁹⁶Zr(¹⁸O, 4n), E=65, 73 MeV; measured γγ-coin. ¹¹⁰Cd deduced levels, J, π, band structure.

1984MU20 Chem.Phys. 109, 332 (1984)

D.Muller, E.Jahn, G.Ladwig, U.Haubenreisser

High-Resolution Solid-State ²⁷Al and ³¹P NMR: Correlation between chemical shift and mean Al-O-P angle in AlPO₄ Polymorphs

NUCLEAR MOMENTS ²⁷Al, ³¹P; measured NMR; deduced chemical shift, AL-O-P angle correlation. Magic angle spinning technique, AlPO₄ polymorphs.

1978MU14 Nucl.Phys. A311, 1 (1978)

D.Muller, R.Beckmann, U.Holm

Analyzing Power and Phase-Shift Analysis of ³He(p, p)³He between 19 and 30 MeV

NUCLEAR REACTIONS ³He(p, p), E=25 MeV; measured A(θ) for ³He; deduced phase shifts. polarized target.

doi: 10.1016/0375-9474(78)90497-9
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1973BR24 Z.Phys. 264, 201 (1973)

G.Breuer, D.Muller

A Study of Branching Ratios of Cross Sections in the Charge Symmetric Reactions ¹⁰B(d, p)¹¹B and ¹⁰B(d, n)¹¹C

NUCLEAR REACTIONS ¹⁰B(d, p), (d, n), E=.6-3.0 MeV; calculated σ(E;θ).

doi: 10.1007/BF01396276
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1966KO04 Phys.Letters 21, 199 (1966)

R.Kosiek, D.Muller, R.Pfeiffer, O.Merwitz

Zum Kernphotoeffekt am Tritium

NUCLEAR STRUCTURE ³H; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(66)90314-3
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1952MU45 Phys.Rev. 88, 775 (1952)

D.E.Muller, H.C.Hoyt, D.J.Klein, J.W.M.DuMond

Precision Measurements of Nuclear γ-Ray Wavelengths of Ir¹⁹², Ta¹⁸², Ra, Th, Rn, W¹⁸⁷, Cs¹³⁷, Au¹⁹⁸, and Annihilation Radiation

doi: 10.1103/PhysRev.88.775
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1949LI24 Phys.Rev. 75, 1544 (1949)

D.A.Lind, J.Brown, D.Klein, D.Muller, J.DuMond

Precision Measurements of Gamma-Rays from I¹³¹with the 2-Meter Focusing Curved Crystal Spectrometer

RADIOACTIVITY ¹³¹I(β^-); measured decay products; deduced γ-ray energies and relative intensities, tentative decay scheme. Comparison with available data.

doi: 10.1103/PhysRev.75.1544
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