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NSR database version of April 11, 2024.

Search: Author = G.Fricke

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1997TE11      Phys.Rev. C56, 2597 (1997)

L.A.A.Terremoto, V.P.Likhachev, M.N.Martins, H.J.Emrich, G.Fricke, T.Krohl, K.W.Neff

Giant Resonances in the 26Mg(e, e'α0)22Ne Reaction

NUCLEAR REACTIONS 26Mg(e, e'α), E=14-26 MeV; measured eα-coin, σ(Eα, Ee, θ(α), θ(e)); deduced multipole components, sum rules. 22Ne deduced resonances.

doi: 10.1103/PhysRevC.56.2597
Citations: PlumX Metrics


1995FR22      At.Data Nucl.Data Tables 60, 177 (1995)

G.Fricke, C.Bernhardt, K.Heilig, L.A.Schaller, L.Schellenberg, E.B.Shera, C.W.De Jager

Nuclear Ground State Charge Radii from Electromagnetic Interactions

NUCLEAR STRUCTURE 40,42,44,46,48Ca, 78,80,82,83,84,86Kr, 84,86,87,88Sr, 90,92,94,96Zr, 92,94,95,96,97,98,100Mo, 144,147,148,149,150,152,154Sm, 154,155,156,157,158,160Gd, 196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,214Pb; analyzed muonic X-ray, (e, e), optical data; deduced rms charge radii.

doi: 10.1006/adnd.1995.1007
Citations: PlumX Metrics


1992FR01      Phys.Rev. C45, 80 (1992)

G.Fricke, J.Herberz, Th.Hennemann, G.Mallot, L.A.Schaller, L.Schellenberg, C.Piller, R.Jacot-Guillarmod

Behavior of the Nuclear Charge Radii Systematics in the s-d Shell from Muonic Atom Measurements

NUCLEAR REACTIONS 18,16O, 19F, 20,21,22Ne, 23Na, 24,25,26Mg, 27Al, Si, 36,38,40Ar(μ-, X), E at rest; measured muonic X-rays; deduced 2P-1S transition energies. 18,16O, 19F, 20,21,22Ne, 23Na, 24,25,26Mg, 27Al, Si, 36,38,40Ar deduced charge radii.

ATOMIC PHYSICS, Mesic-Atoms 18,16O, 19F, 20,21,22Ne, 23Na, 24,25,26Mg, 27Al, Si, 36,38,40Ar(μ-, X), E at rest; measured muonic X-rays; deduced 2P-1S transition energies. 18,16O, 19F, 20,21,22Ne, 23Na, 24,25,26Mg, 27Al, Si, 36,38,40Ar deduced charge radii.

doi: 10.1103/PhysRevC.45.80
Citations: PlumX Metrics


1990PI10      Phys.Rev. C42, 182 (1990)

C.Piller, C.Gugler, R.Jacot-Guillarmod, L.A.Schaller, L.Schellenberg, H.Schneuwly, G.Fricke, T.Hennemann, J.Herberz

Nuclear Charge Radii of the Tin Isotopes from Muonic Atoms

NUCLEAR REACTIONS 112,114,116,117,119,120,124Sn(μ, X), E at rest; measured E X-ray, I X-ray. 112,114,116,117,119,120,124Sn deduced rms radius, equivalent nuclear radii.

ATOMIC PHYSICS, Mesic-Atoms 112,114,116,117,119,120,124Sn(μ, X), E at rest; measured E X-ray, I X-ray. 112,114,116,117,119,120,124Sn deduced rms radius, equivalent nuclear radii.

doi: 10.1103/PhysRevC.42.182
Citations: PlumX Metrics


1989SH02      Phys.Rev. C39, 195 (1989)

E.B.Shera, M.V.Hoehn, G.Fricke, G.Mallot

Nuclear Charge Radii of the Te Isotopes from Muonic Atoms

ATOMIC PHYSICS, Mesic-Atoms 123,124,125,126,128,130Te(μ-, X), E at rest; measured X-ray spectra; deduced transition energies, isotope shifts.

NUCLEAR REACTIONS 123,124,125,126,128,130Te(μ-, X), E at rest; measured X-ray spectra. 123,124,125,126,128,130Te deduced nuclear charge parameters, rms radii, isotope shifts relative to 120Te.

doi: 10.1103/PhysRevC.39.195
Citations: PlumX Metrics


1986KI09      Phys.Rev.Lett. 56, 2789 (1986)

Th.Kihm, K.T.Knopfle, H.Riedesel, P.Voruganti, H.J.Emrich, G.Fricke, R.Neuhausen, R.K.M.Schneider

E1 and E2-E0 Form Factors and Strength Distributions from 28Si(e, e'p) and 28Si(e, e'α) Coincidence Scattering

NUCLEAR REACTIONS 28Si(e, e'p), (e, e'α), E=183.5 MeV; measured e'p-, e'α-coin, σ(E(e')). 28Si deduced form factors, giant resonances, multipole transition strength distribution.

doi: 10.1103/PhysRevLett.56.2789
Citations: PlumX Metrics


1986OF01      Phys.Rev.Lett. 57, 1546 (1986)

E.A.J.M.Offermann, L.S.Cardman, H.J.Emrich, G.Fricke, C.W.de Jager, H.Miska, D.Rychel, H.de Vries

Search for Dispersive Effects in Elastic Electron Scattering from 12C

NUCLEAR REACTIONS 12C(e, e), E=238, 374.5, 419, 747.2 MeV; analyzed from factor; deduced dispersive effect induced energy dependence.

doi: 10.1103/PhysRevLett.57.1546
Citations: PlumX Metrics


1985SC05      Phys.Rev. C31, 1007 (1985)

L.A.Schaller, D.A.Barandao, P.Bergem, M.Boschung, T.Q.Phan, G.Piller, A.Ruetschi, L.Schellenberg, H.Schneuwly, G.Fricke, G.Mallot, H.G.Sieberling

Nuclear Charge Radii of the Even Sulphur Isotopes 32S, 34S, and 36S and of 31P using Muonic Atoms

ATOMIC PHYSICS, Mesic-Atoms 32,34,36S, 31P; measured muonic E X-ray, I X-ray. 32,34,36S deduced equivalent Barrett, rms charge radii. High precision.

doi: 10.1103/PhysRevC.31.1007
Citations: PlumX Metrics


1983BE49      Helv.Phys.Acta 56, 973 (1983)

P.Bergem, F.Bienz, M.Boschung, T.Q.Phan, G.Piller, A.Ruetschi, L.A.Schaller, L.Schellenberg, H.Schneuwly, G.Fricke, G.Mallot, H.G.Sieberling

Muonic Atom Experiments

NUCLEAR MOMENTS 209Bi; measured muonic hfs. 209Bi levels deduced μ. Anti-Compton spectrometer.

ATOMIC PHYSICS, Mesic-Atoms A=12-100; analyzed data; deduced nuclear charge radii. 90Zr, 140Ce, 208Pb; measured muonic 2s-2p transition energies. Gas targets, anti-Compton spectrometer.


1983EM01      Nucl.Phys. A396, 401c (1983)

H.J.Emrich, G.Fricke, G.Mallot, H.Miska, H.-G.Sieberling, J.M.Cavedon, B.Frois, D.Goutte

Radial Distribution of Nucleons in the Isotopes 48,40Ca

NUCLEAR REACTIONS 48Ca(e, e), E=350, 600 MeV; measured σ(θ). 48,40Ca(e, e), E=100, 210, 320 MeV; measured σ(θ) ratio. 40,48Ca deduced radial charge distribution, differences, neutron distribution difference.

doi: 10.1016/0375-9474(83)90034-9
Citations: PlumX Metrics


1982RE12      Phys.Rev. C26, 806 (1982)

W.Reuter, G.Fricke, K.Merle, H.Miska

Nuclear Charge Distribution and rms Radius of 12C from Absolute Elastic Electron Scattering Measurements

NUCLEAR REACTIONS 12C(e, e), E=100-300 MeV; measured absolute σ(θ). 12C deduced rms radius, charge distribution.

doi: 10.1103/PhysRevC.26.806
Citations: PlumX Metrics


1981FR25      Helv.Phys.Acta 54, 317 (1981)

G.Fricke, G.Mallot, T.Q.Phan, G.Piller, A.Ruetschi, L.A.Schaller, L.Schellenberg, H.Schneuwly

Etude du Deplacement Isotopique a Partir des Transitions Muoniques dans l'Argon

ATOMIC PHYSICS, Mesic-Atoms 36,38,40Ar; measured muonic X-rays. 36,38,40Ar deduced rms radii, isotope shifts.


1980SC01      Nucl.Phys. A333, 333 (1980)

L.Schellenberg, B.Robert-Tissot, K.Kaeser, L.A.Schaller, H.Schneuwly, G.Fricke, S.Gluckert, G.Mallot, E.B.Shera

Systematics of Nuclear Charge Radii of the Stable Molybdenum Isotopes From Muonic Atoms

ATOMIC PHYSICS 92,94,95,96,97,98,100Mo; measured muonic X-rays, isotope shift; deduced nuclear charge radii.

NUCLEAR MOMENTS 97Mo; deduced quadrupole moment.

doi: 10.1016/0375-9474(80)90100-1
Citations: PlumX Metrics


1980WO02      Phys.Rev. C22, 264 (1980)

H.D.Wohlfahrt, O.Schwentker, G.Fricke, H.G.Andresen, E.B.Shera

Systematics of Nuclear Charge Distributions in the Mass 60 Region from Elastic Electron Scattering and Muonic X-Ray Measurements

NUCLEAR REACTIONS 54,56,58Fe, 58,60,62,64Ni, 64,66,68,70Zn(e, e), E=100, 150, 275 MeV; measured σ(θ); deduced model-independent isotone, isotope charge distribution differences. Hartree-Fock calculations.

ATOMIC PHYSICS 54,56,58Fe, 58,60,62,64Ni, 64,66,68,70Zn; analyzed muonic X-ray, electron scattering data; deduced model-independent rms radii differences.

doi: 10.1103/PhysRevC.22.264
Citations: PlumX Metrics


1978DU21      Helv.Phys.Acta 51, 513 (1978)

T.Dubler, G.Fricke, S.Gluckert, K.Kaeser, G.Mallot, B.Robert-Tissot, L.A.Schaller, L.Schellenberg, E.B.Shera, H.Schneuwly, H.K.Walter

Muonic Isotope Shifts in the Region 84 ≤ A ≤ 100

NUCLEAR REACTIONS 92,94,96,98,100Mo, Zr, Sr(μ-, X-ray), E=at rest; measured I(K X-ray), E(K X-ray); deduced isotopic shifts, differences in mean square radii. 97Mo level deduced quadrupole moment.


1978WO03      Phys.Lett. 73B, 131 (1978)

H.D.Wohlfahrt, E.B.Shera, M.V.Hoehn, Y.Yamazaki, G.Fricke, R.M.Steffen

Muonic Isotope Shifts in the Stable Ca Nuclei

ATOMIC PHYSICS 43,40,42,44,46,48Ca; measured isotope shift in muonic atoms.

doi: 10.1016/0370-2693(78)90816-X
Citations: PlumX Metrics


1976SH21      Phys.Rev. C14, 731 (1976)

E.B.Shera, E.T.Ritter, R.B.Perkins, G.A.Rinker, L.K.Wagner, H.D.Wohlfahrt, G.Fricke, R.M.Steffen

Systematics of Nuclear Charge Distributions in Fe, Co, Ni, Cu, and Zn Deduced from Muonic X-Ray Measurements

NUCLEAR REACTIONS 54,56,57,58Fe, 59Co, 58,60,61,62,64Ni, 63,65Cu, 64,66,68,70Zn(μ-, X-ray); measured muonic X-rays. 54,56,57,58Fe, 59Co, 58,60,61,62,64Ni, 63,65Cu, 64,66,68,70Zn deduced nuclear charge parameters; isotope, isotone shift.

doi: 10.1103/PhysRevC.14.731
Citations: PlumX Metrics


1975SH03      Phys.Rev.Lett. 34, 535 (1975)

E.B.Shera, E.T.Ritter, G.A.Rinker, Jr., M.J.Bennett, R.B.Perkins, H.D.Wohlfahrt, G.Fricke, L.K.Wagner, P.Kleinheinz, R.K.Sheline, R.M.Steffen, J.W.Negele

Muonic Isotope Shifts in the Even Fe Nuclei

ATOMIC PHYSICS 54,56,58Fe; measured muonic isotope shift.

doi: 10.1103/PhysRevLett.34.535
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1965FR07      Nucl.Phys. 67, 187 (1965)

G.Fricke, G.R.Bishop, D.B.Isabelle

The 6.02 MeV Level of B10

NUCLEAR REACTIONS 10B(e, e'), E = 100-220 MeV; measured σ(Ee'); deduced inelastic form factor. Enriched target.

doi: 10.1016/0029-5582(65)90121-5
Citations: PlumX Metrics


1964AR22      Z. Physik 178, 109 (1964)

H.Artus, G.Fricke, D.E.Von Stein

Erzeugung von Be7 durch Kernphotoeffekt am Beryllium, Bor and Kohlenstoff

NUCLEAR STRUCTURE 10B, 12C, 11B, 9Be; measured not abstracted; deduced nuclear properties.

doi: 10.1007/BF01375487
Citations: PlumX Metrics


1964GU06      Z.Physik 181, 453 (1964)

F.Gudden, G.Fricke, H.-G.Clerc, P.Brix

Eine Anordnung fur Experimente Zur Elektronenstreuung Unterhalb 60 MeV

NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.

doi: 10.1007/BF01380562
Citations: PlumX Metrics


1960BA47      Phys.Rev. 120, 2081 (1960)

W.C.Barber, F.Berthold, G.Fricke, F.E.Gudden

Nuclear Excitation by Scattering of 40-MeV Electrons

NUCLEAR STRUCTURE 12C, 9Be, 206Pb, 207Pb, 208Pb, 6Li, 28Si; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.120.2081
Citations: PlumX Metrics


1960BA50      Priv.Comm. (1960)

W.C.Barber, F.Berthold, G.Fricke, F.E.Gudden

NUCLEAR STRUCTURE 28Si, 6Li, 208Pb, 9Be, 12C; measured not abstracted; deduced nuclear properties.


1960BE08      Bull.Am.Phys.Soc. 5, No.4, 271, Q6 (1960)

F.Berthold, W.C.Barber, G.Fricke, F.E.Gudden

Inelastic Electron Scattering from Levels of Light Nuclei

NUCLEAR STRUCTURE 28Si, 9Be, 6Li; measured not abstracted; deduced nuclear properties.


1960FR03      Naturwissenschaften 47, 129 (1960)

G.Fricke, S.Penselin, E.Recknagel

The Hyperfine Structure Splitting of the 2S1/2 Ground State and the Nuclear Magnetic Dipole Moment of Au197

NUCLEAR STRUCTURE 197Au; measured not abstracted; deduced nuclear properties.

doi: 10.1007/BF00628506
Citations: PlumX Metrics


1959FR49      Naturwissenschaften 46, 106 (1959)

G.Fricke, H.Kopfermann, S.Penselin, K.Schlupmann

Determination of the Hyperfine Structure Splitting of the Scandium Ground State 2D32 and 2D52 and the Quadrupole Moment of the Sc45 Nucleus

doi: 10.1007/BF00638313
Citations: PlumX Metrics


1959FR53      Z.Physik 156, 416 (1959)

G.Fricke, H.Kopfermann, S.Penselin, K.Schlupmann

Bestimmung der Hyperfeinstrukturaufspaltungen der Scandium-Grundzustande 2D3/2 und 2D5/2 und des Quadrupolmomentes des Sc45-Kernes

doi: 10.1007/BF01461238
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1959FR58      Z.Physik 154, 218 (1959); See Also 57Eh40

G.Fricke, H.Kopfermann, S.Penselin

Messung der Hyperfeinstrukturaufspaltungen der beiden Yttrium-Grundzustande 2d(3/2) und 2d(5/2) mit der Atomstrahlresonanzmethode

doi: 10.1007/BF01338376
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1957EH40      Naturwissenschaften 44, 255 (1957)

D.Ehrenstein, G.Fricke, H.Kopfermann, S.Penselin


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