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NSR database version of April 11, 2024.

Search: Author = G.Nowicki

Found 15 matches.

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1982AN15      Phys.Rev. C26, 2194 (1982)

A.Andl, K.Bekk, S.Goring, A.Hanser, G.Nowicki, H.Rebel, G.Schatz, R.C.Thompson

Isotope Shifts and Hyperfine Structure of the 4s2 1S0-4s4p 1P1 Transition in Calcium Isotopes

NUCLEAR MOMENTS 40,42,43,44,46,48Ca, 41,45,47Ca [from 40,44,46Ca(n, γ), E=thermal]; measured hfs, isotope shifts. 41,45,47Ca deduced hyperfine constants, rms charge radii differences, μ. 43Ca deduced hyperfine constants, rms charge radii differences. 40,42,44,46,48Ca deduced rms charge radii differences. Laser spectroscopy, resonance fluorescence technique.

doi: 10.1103/PhysRevC.26.2194
Citations: PlumX Metrics


1979BE25      Z.Phys. A291, 219 (1979)

K.Bekk, A.Andl, S.Goring, A.Hanser, G.Nowicki, H.Rebel, G.Schatz

Laserspectroscopic Studies of Collective Properties of Neutron Deficient Ba Nuclei

NUCLEAR MOMENTS 126,129m,129,135mBa; measured optical isotope shift, hfs. 126,129m,129,135mBa deduced differences of rms charge radii, μ, quadrupole moment. Laser spectroscopy. Quasiparticle-plus-triaxial rotor, droplet model.

doi: 10.1007/BF01409187
Citations: PlumX Metrics


1978NO09      Phys.Rev. C18, 2369 (1978)

G.Nowicki, K.Bekk, S.Goring, A.Hanser, H.Rebel, G.Schatz

Nuclear Charge Radii and Nuclear Moments of Neutron Deficient Ba Isotopes from High Resolution Laser Spectroscopy

NUCLEAR MOMENTS 128,131,133Ba; measured isotope shift, hfs, J, nuclear charge radii. Laser spectroscopy.

doi: 10.1103/PhysRevC.18.2369
Citations: PlumX Metrics


1977NO04      Phys.Rev.Lett. 39, 332 (1977)

G.Nowicki, K.Bekk, S.Goring, H.Hanser, H.Rebel, G.Schatz

Nuclear Radii and Magnetic Moments of 128,131Ba from High-Resolution Laser Spectroscopy

NUCLEAR MOMENTS 128,131Ba; measured isotope shift, hfs. 128,130,131Ba deduced differences of mean-square charge radii. 131Ba deduced μ. Doppler-free laser spectroscopy.

doi: 10.1103/PhysRevLett.39.332
Citations: PlumX Metrics


1976GI10      Z.Phys. A279, 55 (1976)

H.J.Gils, H.Rebel, J.Buschmann, H.Klewe-Nebenius, G.P.Nowicki, W.Nowatzke

Nuclear Matter Sizes and Isoscalar Octupole Transition Rates of 204,206,208Pb from 104 MeV α-Particle Scattering

NUCLEAR REACTIONS 204,206,208Pb(α, α), (α, α'), E=104 MeV; measured σ(θ). 204,206,208Pb deduced rms radii, isoscalar octupole transition probabilities. Folding model analysis.

doi: 10.1007/BF01409092
Citations: PlumX Metrics


1975GI04      J.Phys.(London) G1, 344 (1975)

H.J.Gils, H.Rebel, G.Nowicki, A.Ciocanel, D.Hartmann, H.Klewe-Nebenius, K.Wisshak

Deformation of 56Fe from 104 MeV α-Particle Scattering

NUCLEAR REACTIONS 56Fe(α, α'), (α, α), E=104 MeV; analyzed σ(Eα', θ). 56Fe levels deduced β, B(E2), quadrupole moment.

doi: 10.1088/0305-4616/1/3/009
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1098.


1975KL02      Nucl.Phys. A240, 137 (1975)

H.Klewe-Nebenius, D.Habs, K.Wisshak, H.Faust, G.Nowicki, S.Goring, H.Rebel, G.Schatz, M.Schwall

The Level Scheme of 137Pr; Evidence for Prolate Nuclear Shape

RADIOACTIVITY 137Nd[from 141Pr(α, 7np)]; measured Eγ, Iγ, γγ-coin, E(ce), I(ce); deduced ICC. 137Pr deduced levels, J, π. Mass separated sources.

NUCLEAR REACTIONS 139La(α, 6nγ), E=70-104 MeV; measured σ(E, Eγ, θ), E(ce), I(ce), γ(t); deduced ICC. 137Pr deduced levels, J, π, T1/2. Natural target. Ge(Li), Si(Li) detectors with magnetic filter.

doi: 10.1016/0375-9474(75)90442-X
Citations: PlumX Metrics


1975NO08      Nucl.Phys. A249, 76 (1975)

G.P.Nowicki, J.Buschmann, A.Hanser, H.Rebel, H.Faust, D.Habs, H.Klewe-Nebenius, K.Wisshak

The Level Scheme of 137Nd from (α, xn) Reactions and from β-Decay of The 11/2- Isomer of 137Pm

RADIOACTIVITY 137Pm [from 141Pr(α, 8n)]; measured Eγ, Iγ, γγ-coin, E(ce), I(ce); deduced ICC. 137Nd deduced levels, J, π. Natural target, mass-separated sources, Ge(Li) detectors, Si(Li) detector with magnetic filter.

NUCLEAR REACTIONS 140Ce(α, 7n), E=80-104 MeV; measured σ(E, Eγ, θ), γγcoin, E(ce), I(ce)(θ). 137Nd deduced levels, J, π. Natural target, Ge(Li) detectors, Si(Li) detector with magnetic filter.

doi: 10.1016/0375-9474(75)90092-5
Citations: PlumX Metrics


1975WI11      Nucl.Phys. A247, 59 (1975)

K.Wisshak, H.Klewe-Nebenius, D.Habs, H.Faust, G.Nowicki, H.Rebel

The Level Scheme of 135Pr: Prolate Deformation of the 11/2- Isomer

RADIOACTIVITY 135Nd [from 138Ce(α, 7n), 136Ce(α, 5n)]; measured Eγ, Iγ, γγ-coin, I(ce), E(ce); deduced ICC, K/L. 135Pr deduced levels, J, π. Enriched targets, mass separated sources, Ge(Li) detectors, Si(Li) detector with magnetic filter for background suppression.

NUCLEAR REACTIONS 139La(α, 8n), E=80-104 MeV; measured σ(E, Eγ, θ), γγ-coin. 135Pr deduced levels, J, π. Natural target, Ge(Li) detectors.

doi: 10.1016/0375-9474(75)90277-8
Citations: PlumX Metrics


1974BA07      Nucl.Phys. A222, 459 (1974)

M.V.Banaschik, C.Gunther, H.Hubel, A.C.Rester, G.Nowicki, J.J.Pinajian

High Spin Rotational States in 154Dy, 164Er and 162Yb

NUCLEAR REACTIONS 154Gd, 164Dy, 164Er(α, xnγ), Eα=46-97 MeV; measured Eγ, Iγ(Eα, θ), αγ-delay, γγ-coincidences. 154Dy, 164Er, 162Yb deduced rotational levels, moment of inertia. Enriched targets, Ge(Li) detectors.

doi: 10.1016/0375-9474(74)90332-7
Citations: PlumX Metrics


1974HA19      Z.Phys. 267, 149 (1974)

D.Habs, H.Klewe-Nebenius, K.Wisshak, R.Lohken, G.Nowicki, H.Rebel

The Spherical to Asymmetric Shape Transition in the Mass Region with 50 < (N, Z) < 82

NUCLEAR STRUCTURE 120,122,124,126,128,130Te, 126,128,130,132,134Xe, 128,130,132,134,136Ba, 136,138Ce, 138,140Nd, 142Sm; calculated levels, B(E2), quadrupole moment.

doi: 10.1007/BF01668642
Citations: PlumX Metrics


1974RE01      Nucl.Phys. A218, 13 (1974)

H.Rebel, G.Hauser, G.W.Schweimer, G.Nowicki, W.Wiesner, D.Hartmann

The Deformation of 46,48,50Ti from 104 MeV α-Particle Scattering

NUCLEAR REACTIONS 46,48,50Ti(α, α'), E=104 MeV; measured σ(Eα', θ). 46,48,50Ti levels deduced deformation parameters.

doi: 10.1016/0375-9474(74)90017-7
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0714.


1972HA08      Nucl.Phys. A182, 1 (1972)

G.Hauser, R.Lohken, G.Nowicki, H.Rebel, G.Schatz, G.Schweimer, J.Specht

(α, τ) and (α, t) Reactions with 104 MeV α-Particles

NUCLEAR REACTIONS 12C, 40Ca(α, 3He0), (α, t0), (α, α0); 27Al(α, t0), (α, t1), (α, α0);E=104 MeV; measured σ(θ); deduced normalization factors. 13C, 13N, 28Si, 41Ca, 41Sc deduced absolute S.

doi: 10.1016/0375-9474(72)90198-4
Citations: PlumX Metrics


1972SC23      Phys.Lett. 39B, 627 (1972)

G.W.Schweimer, H.Rebel, G.Nowicki, G.Hauser, R.Lohken

Evidence for Prolate Shape of 32S from 104 MeV α-Particle Scattering

NUCLEAR REACTIONS 32S(α, α), (α, α'), E=104 MeV; measured σ(θ); deduced optical model parameters. 32S deduced deformation parameters.

doi: 10.1016/0370-2693(72)90015-9
Citations: PlumX Metrics


1971HA49      Lett.Nuovo Cim. 2, 405 (1971)

G.Hauser, R.Lohken, G.Nowicki, H.Rebel, G.Schatz, W.Schweimer, J.Specht

Experimental Determination of the Normalization Factors for (α, tau) and (α, t) Reactions

NUCLEAR REACTIONS 40Ca(α, 3He), (α, t), E=104 MeV; measured σ(θ); deduced normalization factors.

doi: 10.1007/BF02780421
Citations: PlumX Metrics


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Note: The following list of authors and aliases matches the search parameter G.Nowicki: , G.P.NOWICKI