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NSR database version of April 27, 2024.

Search: Author = J.Eichler

Found 22 matches.

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2007EI01      Phys.Rep. 439, 1 (2007)

J.Eichler, T.Stohlker

Radiative electron capture in relativistic ion-atom collisions and the photoelectric effect in hydrogen-like high-Z systems

doi: 10.1016/j.physrep.2006.11.003
Citations: PlumX Metrics


1995KA61      Z.Phys. D35, 15 (1995)

T.Kandler, Th.Stohlker, P.H.Mokler, C.Kozhuharov, H.Geissel, C.Scheidenberger, P.Rymuza, Z.Stachura, A.Warczak, R.W.Dunford, J.Eichler, A.Ichihara, T.Shirai

Photon Angular Distribution of Radiative Electron Capture into the M Shell of He-Like Uranium Ions at 110-140 MeV/u

NUCLEAR REACTIONS C(U, X), E at 110-140 MeV/nucleon; measured radiative electron capture (into M-shell) associated γ(θ).

doi: 10.1007/BF01439978
Citations: PlumX Metrics


1994EI03      Nucl.Phys. A572, 147 (1994)

J.Eichler

Angular Distribution of De-Excitation X-Rays from Radiative Electron Capture in Relativistic Atomic Collisions

doi: 10.1016/0375-9474(94)90426-X
Citations: PlumX Metrics


1993IC01      At.Data Nucl.Data Tables 55, 63 (1993)

A.Ichihara, T.Shirai, J.Eichler

Cross Sections for Electron Capture in Relativistic Atomic Collisions

ATOMIC PHYSICS C, 27Al, Cu, Ag, 197Au, U; calculated electron capture σ. Relativistic eikonal approximation.

doi: 10.1006/adnd.1993.1016
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1989CO19      Phys.Rev. A40, 4093 (1989)

L.F.S.Coelho, M.B.Gaspar, J.Eichler

Kβ-to-Kα X-Ray Intensity Ratios after Ionization by γ Rays

NUCLEAR REACTIONS 55Mn, Cu, Zn, Ag, Cd, In, Sn(γ, X), E=59.54 keV; measured I(K X-ray) ratios. Hyperpure Ge detector, 241Am γ-source.

ATOMIC PHYSICS 55Mn, Cu, Zn, Ag, Cd, In, Sn(γ, X), E=59.54 keV; measured I(K X-ray) ratios. Hyperpure Ge detector, 241Am γ-source.

doi: 10.1103/PhysRevA.40.4093
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1986DE04      Z.Phys. A323, 101 (1986)

S.de Barros, S.D.de Magalhaes, H.Wolf, J.Barreto, J.Eichler, N.Lisbona, I.O.de Souza, D.M.Vianna

Excitation Function and Half-Life for the Fission Isomer 240mPu from the 238U(α, 2n)240mPu Reaction

RADIOACTIVITY 240mPu(SF) [from 238U(α, 2n), E=20.1-27.3 MeV]; measured T1/2.

NUCLEAR REACTIONS, ICPND 238U(α, 2n), E=20.1-27.3 MeV; measured residual fission isomer production σ(E). 240mPu deduced delayed fission σ, isomeric σ ratio.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0691.


1985EI02      Phys.Rev. A32, 789 (1985)

J.Eichler, S.de Barros

Coherent Scattering of 59.54-keV γ Rays by Al, Cu, Zn, Cd, and Pb

ATOMIC PHYSICS 27Al, Cu, Zn, Cd, Pb(γ, γ), E=59.54 keV; measured coherent σ(θ). Second-order perturbation theory.

doi: 10.1103/PhysRevA.32.789
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1982EI02      Z.Naturforsch., 37a, 1124 (1982)

J.Eichler, S.de Barros, A.M.Goncalves

Compton Cross Section of 662 keV Photons from the K-Shell of Co, Cu, Ge, , Nb, Mo and Ag

ATOMIC PHYSICS Co, Cu, Ge, Nb, Mo, Ag(γ, X), E=662 keV; measured I(K X-ray); deduced photoelectric, Compton σ(total).


1981DE23      Z.Naturforsch. 36a, 595 (1981)

S.de Barros, J.Eichler, O.Goncalves, M.Gaspar

Experiments on Rayleigh Scattering of 145 keV and 317 keV and Photons

ATOMIC PHYSICS Pb, W, Sn, Cd, Ag, Mo, Cu(γ, γ), E=145, 317 keV; measured σ(θ). Dirac-Hartree-Fock-Slater form factor calculations, Rayleigh scattering.


1981DE30      Phys.Rev. C24, 1765 (1981)

S.de Barros, J.Eichler, M.Gaspar, O.Goncalves

Rayleigh Scattering of 468 keV Photons by Different Atoms

ATOMIC PHYSICS Pb, W, Sn, Cd, Ag, Mo, Cu(γ, γ), E=468 keV; measured σ(θ). Rayleigh scattering, Dirac-Hartree-Fock-Slater wave functions.

doi: 10.1103/PhysRevC.24.1765
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1972EI03      Nucl.Phys. A182, 33 (1972)

J.Eichler, M.Yamamura

Quadrupling and Pairing in the Shell Model

doi: 10.1016/0375-9474(72)90200-X
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1971DJ03      Nucl.Phys. A165, 560 (1971)

F.Djadali, J.Eichler

Measurement of the Circular γ-Polarization after n-Capture in 141Ce, 144Nd and 140La Using Ge(Li) Detectors

NUCLEAR REACTIONS 140Ce, 143Nd, 139La(n, γ), E=thermal; measured γ-circular polarization, Eγ. 141Ce, 144Nd, 140La, deduced levels, J, π. Natural targets, Ge(Li) detector.

doi: 10.1016/0375-9474(71)90470-2
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1971EI08      HMI-B-114 (1971)

J.Eichler

Theorie der Kernmodelle (Zweiter Teil)


1970EI03      Z.Phys. 233, 154 (1970)

J.Eichler, F.Djadali

Beitrag zur Kernspektroskopie an 36Cl, 90Y und 40K durch Messung der Polarisation von γ-Strahlung nach Neutroneneinfang

NUCLEAR REACTIONS 35Cl, 39K, 89Y(polarized n, γ), E=thermal; measured γ-circular polarization. 36Cl level deduced γ-mixing. 40K, 90Y levels deduced J, π.

doi: 10.1007/BF01396032
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1970EI04      Nucl.Phys. A147, 150 (1970)

J.Eichler, F.Djadali

Measurement of the Average Circular γ-Polarization and Determination of Spins for Compound States Formed in Thermal Neutron Capture

NUCLEAR REACTIONS 95Mo, 113Cd, 115In, 121,123Sb, 127I, 133Cs, 141Pr, 155,157Gd, 159Tb, 165Ho, 181Ta, 199Hg(polarized n, γ), E = thermal; measured average γ-circular polarization. 96Mo, 114Cd, 116In, 122,124Sb, 128I, 134Cs, 142Pr, 156,158Gd, 160Tb, 166Ho, 182Ta, 200Hg deduced J for compound state. Natural targets.

doi: 10.1016/0375-9474(70)90517-8
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1970EI06      Nucl.Phys. A157, 166 (1970)

J.Eichler, A.Faessler

Alpha Clusters in Hartree-Fock Calculations

NUCLEAR STRUCTURE 12C, 16O, 20Ne; calculated moments, binding energy, deformation.

doi: 10.1016/0375-9474(70)90106-5
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1969EI01      Z.Physik 219, 114 (1969)

J.Eichler

Messung der Zirkularen Polarisation von γ-Strahlung nach Einfang Polarisierter Thermischer Neutronen in Kernen

NUCLEAR REACTIONS 27Al, 59Co, Mo, Sm(n, γ), E=thermal; measured circular polarization; 28Al levels deduced γ-mixing. 60Co, 96Mo, 150Sm levels, deduced J, π.

doi: 10.1007/BF01392952
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1969EI05      Z.Physik 227, 352 (1969)

J.Eichler, P.Heine

An Experimental Test of Parity Violation in Nuclear Forces Studied in 113Cd(n, γ)

NUCLEAR REACTIONS 113Cd(polarized n, γ), E = thermal; measured γ(θ); deduced no parity violation.

doi: 10.1007/BF01394434
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1968DE34      Advan.Nucl.Phys. 1, 1 (1968)

J.de Boer, J.Eichler

The Reorientation Effect


1968EI01      Nucl.Phys. A120, 535 (1968); Erratum Nucl.Phys. A127, 693(1969)

J.Eichler

An Experimental Study of Time-Reversal Invariance in Nuclear Gamma Decay

NUCLEAR REACTIONS 35Cl(n, γ), E=thermal, polarized neutrons; measured γγ coin. 36Cl deduced amplitude of time-reversal non-invariance for γ-decay. Natural target.

doi: 10.1016/0375-9474(68)90460-0
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1963EI04      Bull.Am.Phys.Soc. 8, No.4, 385, WB13 (1963)

J.Eichler

On the 1- States in O16

NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.


1963EI05      Phys.Letters 4, 344 (1963)

J.Eichler, S.Wahlborn

Analysis of the Data for the Beta Decays Rb86 → Sr86 and Rb84 → Kr84

NUCLEAR STRUCTURE 84Rb, 86Rb; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(63)90503-1
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