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NSR database version of April 27, 2024.

Search: Author = S.Schneider

Found 21 matches.

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2024SI07      Nucl.Instrum.Methods Phys.Res. A1062, 169239 (2024)

T.Sikorsky, A.Pelczar, S.Schneider, Th.Schumm

Integrating superregenerative principles in a compact, power-efficient NMR/NQR spectrometer: A novel approach with pulsed excitation

NUCLEAR MOMENTS 35Cl; measured frequencies; deduced NQR signal with sub-kHz resolution. Nuclear Quadrupole Resonance (NQR)/Nuclear Magnetic Resonance (NMR) spectroscopy, the Damp-Enhanced Superregenerative Nuclear Spin Analyser (DESSA).

doi: 10.1016/j.nima.2024.169239
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2011JU04      J.Korean Phys.Soc. 59, 1593s (2011)

A.R.Junghans, E.Altstadt, R.Beyer, E.Birgersson, T.Cowan, A.Ferrari, R.Hannaske, A.Matic, K.D.Schilling, R.Schlenk, S.Schneider, R.Schwengner, A.Wagner, F.-P.Weiss, D.Gehre, E.Grosse

The nELBE Neutron Time of Flight Facility

NUCLEAR REACTIONS 56Fe(n, n'), E=800-6000 keV; measured En, In using plastic and ELBE TOFi, Eγ, Iγ using BaF2; deduced σ. Compared with other data and ENDFB-VII.

doi: 10.3938/jkps.59.1593
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2006SC15      Eur.Phys.J. A 28, 107 (2006)

S.Schneider, S.Krewald, Ulf-G.Meissner

The reaction πN → ππN in a meson-exchange approach

NUCLEAR REACTIONS 1H(π+, 2π+), (π+, π+π0), (π-, π-π0), (π-, 2π0), E=150-450 MeV; calculated σ, resonance effects. 1H(π+, 2π+), E=223-305 MeV; calculated σ(θ). Meson exchange model, comparisons with data.

doi: 10.1140/epja/i2006-10030-0
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2003SC11      Phys.Rev. C 67, 044003 (2003)

S.Schneider, J.Haidenbauer, C.Hanhart, J.A.Niskanen

Positive pion absorption on 3He using modern trinucleon wave functions

NUCLEAR REACTIONS 3He(π+, p), E=120, 206, 250 MeV; calculated pion absorption σ(θ), polarization, wave function dependence. 1H(p, π+), E=515, 800 MeV; calculated analyzing power. Trinucleon wave functions, comparison with data.

doi: 10.1103/PhysRevC.67.044003
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2003SC37      Eur.Phys.J. A 18, 421 (2003)

S.Schneider, A.Sibirtsev, Ch.Elster, J.Haidenbauer, S.Krewald, J.Speth

ηN final-state interaction in incoherent photoproduction of η-mesons from the deuteron

NUCLEAR REACTIONS 2H(γ, X), E=630-681 MeV; calculated η-meson production σ, σ(θ), final-state interaction effects.

doi: 10.1140/epja/i2002-10250-2
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2002SI08      Phys.Rev. C65, 044007 (2002)

A.Sibirtsev, S.Schneider, Ch.Elster, J.Haidenbauer, S.Krewald, J.Speth

ηN Final State Interaction in Incoherent Photoproduction of η Mesons from the Deuteron Near Threshold

NUCLEAR REACTIONS 2H(γ, X), E=620-800 MeV; calculated η meson production σ; deduced role of final state interactions. Comparison with data.

doi: 10.1103/PhysRevC.65.044007
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2002SI14      Phys.Rev. C65, 067002 (2002)

A.Sibirtsev, S.Schneider, Ch.Elster, J.Haidenbauer, S.Krewald, J.Speth

Incoherent η Photoproduction from the Deuteron Near Threshold

NUCLEAR REACTIONS 2H(γ, npX), E=620-680 MeV; calculated η meson photoproduction σ, σ(θ). Impulse approximation plus corrections, comparison with data.

doi: 10.1103/PhysRevC.65.067002
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2000SC38      Acta Phys.Pol. B31, 2309 (2000)

S.Schneider

The Reaction πN → ππN in the Framework of a Meson Exchange Model

NUCLEAR REACTIONS 1H(π-, π+π-), E=0.17-0.26 GeV; calculated σ. 1H(π-, π+π-), E=0.284 GeV; calculated σ(θ). Meson exchange model, comparisons with data.


1996QI03      Nucl.Instrum.Methods Phys.Res. B117, 151 (1996)

Y.Qiu, U.Geyer, S.Schneider, M.-P.Macht, W.L.Johnson, T.A.Tombrello

Investigation of Beryllium Diffusion in the Supercooled Liquid and Glassy States of the Amorphous Alloy Zr(41.2)Ti(13.8)Cu(12.5)Ni(10)Be(22.5) by High Energy Helium Elastic Backscattering

NUCLEAR REACTIONS 9Be(α, α), E=6.00-6.52 MeV; measured backscatter σ(θ); deduced beryllium diffusion in Zr(41.2)Ti(13.8)Cu(12.5)Ni(10)Be(22.5).

doi: 10.1016/0168-583X(96)00218-2
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2780.


1995TO04      Phys.Rev. C51, 2989 (1995)

M.Tomaselli, S.M.Schneider, E.Kankeleit, T.Kuhl

Ground-State Magnetization of 209Bi in a Dynamic-Correlation Model

NUCLEAR STRUCTURE 209Bi; calculated μ, rms radius, magnetization distribution. Dynamic-correlation model.

doi: 10.1103/PhysRevC.51.2989
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1994SC48      Z.Phys. D31, 143 (1994)

S.M.Schneider, W.Greiner, G.Soff

The Transition Time for the Ground State Hyperfine Splitting of 209Bi82+

NUCLEAR MOMENTS 209Bi; calculated hfs levels transition time.

ATOMIC PHYSICS 209Bi; calculated hfs levels transition time.

doi: 10.1007/BF01437827
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1993SC31      J.Phys.(London) B26, L581 (1993)

S.M.Schneider, J.Schaffner, W.Greiner, G.Soff

The Hyperfine Structure of 20983Bi82+

NUCLEAR MOMENTS 209Bi; analyzed hfs; deduced QED corrections estimate. Extended nuclear charge distribution.

doi: 10.1088/0953-4075/26/18/001
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1979EY02      Phys.Rev.Lett. 43, 1369 (1979)

W.Eyrich, A.Hofmann, U.Scheib, S.Schneider, F.Vogler, H.Rebel

Decay of the Isoscalar Giant Resonances in 208Pb

NUCLEAR REACTIONS 208Pb(α, α'), E=104 MeV; measured α'γ(θ). 208Pb deduced T=0, GQR, fine structure following n decay.

doi: 10.1103/PhysRevLett.43.1369
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1979SC05      Phys.Lett. 80B, 180 (1979)

S.Schneider, W.Eyrich, A.Hofmann, U.Scheib, F.Vogler

The Influence of Deformations of the Optical Potential on Analyzing Power and p1-γ Angular Correlation in the Reaction 114Cd(p, p')

NUCLEAR REACTIONS 114Cd(p, p'), E=11 MeV; measured σ(θ), A(θ), pγ(θ); deduced influence of β, spin-orbit β in optical potential. Coupled-channels analysis.

doi: 10.1016/0370-2693(79)90192-8
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1979SC15      Phys.Rev. C20, 71 (1979)

S.Schneider, W.Eyrich, A.Hofmann, U.Scheib, F.Vogler

Reaction 114Cd(p, p') by Use of Polarized Protons and Proton-γ Angular Correlations

NUCLEAR REACTIONS 114Cd(p, p'), (p, p'γ), (polarized p, p'), (polarized p, p'γ), E=11 MeV; measured σ(θ), A(θ), pγ(θ), spin flip probability. 114Cd deduced evidence against oblate deformation for harmonic vibrator model. Coupled-channel analysis. Enriched target.

doi: 10.1103/PhysRevC.20.71
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1978EY02      Fizika, Suppl. 10, 45 (1978)

W.Eyrich, A.Hofmann, U.Scheib, S.Schneider, F.Vogler, H.Rebel

The Deformation of 26Mg from Particle-Gamma Angular Correlations

NUCLEAR REACTIONS 24,26Mg, 28Si(α, α'), E=104 MeV; measured αγ(θ). 24,26Mg, 28Si level deduced β. Coupled-channels analysis.


1977EY03      Nucl.Phys. A287, 119 (1977)

W.Eyrich, A.Hofmann, U.Scheib, S.Schneider, F.Vogler, H.Rebel

Alpha-Gamma Angular Correlations in the Reaction 24Mg(α, α1γ) at E = 104 MeV

NUCLEAR REACTIONS 24Mg(α, α'γ), E=104 MeV; measured in-plane α'γ(θ). 24Mg deduced sign of the quadrupole deformation parameter. Coupled channels analyses, enriched target.

doi: 10.1016/0375-9474(77)90567-X
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1976EY02      Phys.Lett. 63B, 406 (1976)

W.Eyrich, A.Hofmann, U.Scheib, S.Schneider, F.Vogler, H.Rebel

Alpha-Gamma Angular Correlation Measurements as a Sensitive Method Determining the Sign of the Nuclear Quadrupole Deformation

NUCLEAR REACTIONS 24Mg(α, α'γ), E=104 MeV; measured γγ(θ). 24Mg levels deduced sign of β2.

doi: 10.1016/0370-2693(76)90381-6
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1976EY03      Nucl.Instrum.Methods 138, 543 (1976)

W.Eyrich, A.Hofmann, U.Scheib, S.Schneider, F.Vogler

Measurement and Evaluation of Particle-γ Angular Correlations for the Study of Nuclear Reaction Mechanisms

NUCLEAR REACTIONS 52Cr(d, pγ); measured pγ-coin. 24Mg(d, d'γ); measured d'γ-coin.

doi: 10.1016/0029-554X(76)90321-9
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1975EY01      Phys.Rev. C11, 1658 (1975)

W.Eyrich, S.Schneider, A.Hofmann, F.Vogler

Gamma-Decay Data from Particle-γ Correlation Functions at Fixed γ Angles

NUCLEAR REACTIONS 52Cr(d, pγ), E=10 MeV; measured σ(Ep, θ), pγ(θ). 53Cr levels deduced γ-mixing.

doi: 10.1103/PhysRevC.11.1658
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1974EY03      Phys.Rev. C10, 2512 (1974)

W.Eyrich, S.Schneider, A.Hofmann, U.Scheib, F.Vogler

Proton-γ Angular Correlations in the Reaction 52Cr(d, pγ)53Cr

NUCLEAR REACTIONS 52Cr(d, pγ), E=10 MeV; measured σ(Ep, Eγ, θ), pγ-coin. 53Cr transitions deduced L.

doi: 10.1103/PhysRevC.10.2512
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Note: The following list of authors and aliases matches the search parameter S.Schneider: , S.M.SCHNEIDER