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NSR database version of April 26, 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 4s^{2 1}S₀-4s4p ¹P₁ Transition in Calcium Isotopes

NUCLEAR MOMENTS ^{40,42,43,44,46,48}Ca, ^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. ^{40,42,44,46,48}Ca 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,129,135m}Ba; measured optical isotope shift, hfs. ^{126,129m,129,135m}Ba 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, T_1/2. 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 ^{120,122,124,126,128,130}Te, ^{126,128,130,132,134}Xe, ^{128,130,132,134,136}Ba, ^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

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