NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = H.Kaiser Found 26 matches. 2011YA26 Nucl.Instrum.Methods Phys.Res. B 269, 425 (2011) H.Yan, D.V.Baxter, C.Y.Jiang, H.Kaiser, Y.C.Shin, W.M.Snow, X.Tong A measurement of the change of the energy dependence of the total cross-section of phase II solid methane from confinement in aerogel glass NUCLEAR REACTIONS H(n, x), E=3.096E-4-0.1686 eV; measured products. Data were imported from EXFOR entry 14289.
doi: 10.1016/j.nimb.2010.12.035
2006WI17 Physica B 385-386, 1374 (2006) F.E.Wietfeldt, M.Huber, T.C.Black, H.Kaiser, M.Arif, D.L.Jacobson, S.A.Werner Measuring the neutron's mean square charge radius using neutron interferometry
doi: 10.1016/j.physb.2006.05.187
2004KA62 Phys.Rev. C 70, 064307 (2004) L.Kaubler, H.Schnare, R.Schwengner, H.Prade, F.Donau, P.von Brentano, J.Eberth, J.Enders, A.Fitzler, C.Fransen, M.Grinberg, R.-D.Herzberg, H.Kaiser, P.von Neumann-Cosel, N.Pietralla, A.Richter, G.Rusev, Ch.Stoyanov, I.Wiedenhover Dipole and quadrupole excitations in 88Sr up to 6.8 MeV NUCLEAR REACTIONS 88Sr(γ, γ'), E=6.8 MeV bremsstrahlung; measured Eγ, Iγ. 88Sr deduced levels, J, π, configurations, B(E1), B(M1), B(E2). Comparison with model predictions.
doi: 10.1103/PhysRevC.70.064307
2003BL07 Phys.Rev.Lett. 90, 192502 (2003) T.C.Black, P.R.Huffman, D.L.Jacobson, W.M.Snow, K.Schoen, M.Arif, H.Kaiser, S.K.Lamoreaux, S.A.Werner Precision Neutron Interferometric Measurement of the nd Coherent Neutron Scattering Length and Consequences for Models of Three-Nucleon Forces NUCLEAR REACTIONS 2H(n, n), E=low; measured coherent scattering length. Neutron interferometry, comparison with previous results and model predictions.
doi: 10.1103/PhysRevLett.90.192502
2003EN07 Nucl.Phys. A724, 243 (2003) J.Enders, P.von Brentano, J.Eberth, A.Fitzler, C.Fransen, R.-D.Herzberg, H.Kaiser, L.Kaubler, P.von Neumann-Cosel, N.Pietralla, V.Yu.Ponomarev, A.Richter, R.Schwengner, I.Wiedenhover Nuclear resonance fluorescence experiments on 204, 206, 207, 208Pb up to 6.75 MeV NUCLEAR REACTIONS 204,206,207,208Pb(γ, γ'), E=6.75 MeV bremsstrahlung; measured Eγ, Iγ(θ). 204,206,207,208Pb deduced levels, J, π, B(M1), B(E2), pygmy resonance features. Quasiparticle-phonon model analysis.
doi: 10.1016/S0375-9474(03)01554-9
2003SC12 Phys.Rev. C 67, 044005 (2003) K.Schoen, D.L.Jacobson, M.Arif, P.R.Huffman, T.C.Black, W.M.Snow, S.K.Lamoreaux, H.Kaiser, S.A.Werner Precision neutron interferometric measurements and updated evaluations of the n-p and n-d coherent neutron scattering lengths NUCLEAR REACTIONS 1,2H(n, n), E=low; measured coherent neutron scattering lengths. Neutron interferometry, comparison with model predictions.
doi: 10.1103/PhysRevC.67.044005
2002BE18 Phys.Rev. C65, 035801 (2002) D.Belic, C.Arlandini, J.Besserer, J.de Boer, J.J.Carroll, J.Enders, T.Hartmann, F.Kappeler, H.Kaiser, U.Kneissl, E.Kolbe, K.Langanke, M.Loewe, H.J.Maier, H.Maser, P.Mohr, P.von Neumann-Cosel, A.Nord, H.H.Pitz, A.Richter, M.Schumann, F.-K.Thielemann, S.Volz, A.Zilges Photo-Induced Depopulation of the 180Tam Isomer via Low-Lying Intermediate States: Structure and astrophysical implications NUCLEAR REACTIONS 180mTa(γ, γ'), E=0.8-3.1 MeV bremsstrahlung; measured delayed Eγ, Iγ, X-ray spectra; deduced activation yields. 180Ta deduced intermediate states energies, transition strengths. Astrophysical implications discussed. Comparisons with previous results, model predictions. RADIOACTIVITY 180Ta(EC), (β-); measured T1/2.
doi: 10.1103/PhysRevC.65.035801
2001VO13 Nucl.Phys. A688, 237c (2001) P.von Neumann-Cosel, C.Arlandini, D.Belic, J.Besserer, J.de Boer, J.J.Carroll, J.Enders, T.Hartmann, F.Kappeler, H.Kaiser, U.Kneissl, M.Loewe, H.J.Maier, H.Maser, P.Mohr, A.Nord, H.H.Pitz, A.Richter, M.Schumann, S.Volz, A.Zilges Photoactivation of 180mTa and s-Process Nucleosynthesis of Nature's Rarest Naturally Occuring Isotope NUCLEAR REACTIONS 180Ta(γ, γ'), E=0.8-3.1 MeV; measured Eγ, σ; deduced 180Ta effective half-life under s-process conditions.
doi: 10.1016/S0375-9474(01)00706-0
2000EN08 Nucl.Phys. A674, 3 (2000) J.Enders, P.von Brentano, J.Eberth, A.Fitzler, C.Fransen, R.-D.Herzberg, H.Kaiser, L.Kaubler, P.von Neumann-Cosel, N.Pietralla, V.Yu.Ponomarev, A.Richter, H.Schnare, R.Schwengner, S.Skoda, H.G.Thomas, H.Tiesler, D.Weisshaar, I.Wiedenhover Note on a Search for the Two-Octupole Phonon 2+ State in 208Pb with Resonant Photon Scattering NUCLEAR REACTIONS 208Pb(γ, γ'), E=6.75 MeV bremsstrahlung; measured Eγ, Iγ. 208Pb deduced levels, J, π, B(E2), no two-phonon octupole vibration. Comparison with quasiparticle-phonon model.
doi: 10.1016/S0375-9474(00)00157-3
2000EN10 Phys.Lett. 486B, 279 (2000) J.Enders, P.von Brentano, J.Eberth, A.Fitzler, C.Fransen, R.-D.Herzberg, H.Kaiser, L.Kaubler, P.von Neumann-Cosel, N.Pietralla, V.Yu.Ponomarev, H.Prade, A.Richter, H.Schnare, R.Schwengner, S.Skoda, H.G.Thomas, H.Tiesler, D.Weisshaar, I.Wiedenhover Structure and Evolution of Electric Dipole Strength in 204, 206, 208Pb below the Neutron Emission Threshold NUCLEAR REACTIONS 204,206,208Pb(γ, γ'), E=6.75 MeV bremsstrahlung; measured Eγ, Iγ. 204,206,208Pb deduced E1 strength distributions. Comparison with model predictions.
doi: 10.1016/S0370-2693(00)00730-9
2000KA08 Eur.Phys.J. A 7, 15 (2000) L.Kaubler, H.Schnare, R.Schwengner, P.von Brentano, F.Donau, J.Eberth, J.Enders, A.Fitzler, C.Fransen, M.Grinberg, E.Grosse, R.-D.Herzberg, H.Kaiser, P.von Neumann-Cosel, N.Pietralla, H.Prade, A.Richter, S.Skoda, Ch.Stoyanov, H.-G.Thomas, H.Tiesler, D.Weisshaar, I.Wiedenhover Is the 4.742 MeV State in 88Sr the 1- Two-Phonon State ? NUCLEAR REACTIONS 88Sr, 11B, 12,13C(γ, γ'), E=6.7 MeV bremsstrahlung; measured Eγ, Iγ, γ polarization. 88Sr deduced levels, J, π, B(λ), no two-phonon state.
doi: 10.1007/s100500050004
1999BE65 Phys.Rev.Lett. 83, 5242 (1999) D.Belic, C.Arlandini, J.Besserer, J.de Boer, J.J.Carroll, J.Enders, T.Hartmann, F.Kappeler, H.Kaiser, U.Kneissl, M.Loewe, H.J.Maier, H.Maser, P.Mohr, P.von Neumann-Cosel, A.Nord, H.H.Pitz, A.Richter, M.Schumann, S.Volz, A.Zilges Photoactivation of 180Tam and Its Implications for the Nucleosynthesis of Nature's Rarest Naturally Occurring Isotope NUCLEAR REACTIONS Ta, 180mTa(γ, γ'), E=0.8-3.1 MeV bremsstrahlung; measured ground-state production yield. Implications for s-process nucleosynthesis discussed. Enriched and natural targets.
doi: 10.1103/PhysRevLett.83.5242
1999EN02 Phys.Rev. C59, R1851 (1999) J.Enders, H.Kaiser, P.von Neumann-Cosel, C.Rangacharyulu, A.Richter Comprehensive Analysis of the Scissors Mode in Heavy Even-Even Nuclei NUCLEAR STRUCTURE A=144-196; analyzed moments of inertia, g-factors, B(M1) in even-even nuclei; deduced relationship between scissors mode, ground state band. Sum-rule approach.
doi: 10.1103/PhysRevC.59.R1851
1999HE31 Phys.Rev. C60, 051307 (1999) R.-D.Herzberg, C.Fransen, P.von Brentano, J.Eberth, J.Enders, A.Fitzler, L.Kaubler, H.Kaiser, P.von Neumann-Cosel, N.Pietralla, V.Yu.Ponomarev, H.Prade, A.Richter, H.Schnare, R.Schwengner, S.Skoda, H.G.Thomas, H.Tiesler, D.Weisshaar, I.Wiedenhover Resolved Dipole Strength Below the E1 Giant Resonance in 138Ba NUCLEAR REACTIONS 138Ba(γ, γ'), E=6.7 MeV bremsstrahlung; measured Eγ, Iγ, γ polarization. 138Ba deduced levels, J, π, B(E1). Euroball cluster detectors.
doi: 10.1103/PhysRevC.60.051307
1999KA65 Nucl.Phys. A660, 41 (1999); Erratum Nucl.Phys. A669, 368 (2000); Erratum Nucl.Phys. A679, 869 (2001) H.Kaiser, P.von Brentano, E.Caurier, J.Eberth, J.Enders, A.Fitzler, C.Fransen, R.-D.Herzberg, L.Kaubler, P.von Neumann-Cosel, N.Pietralla, A.Poves, H.Prade, A.Richter, H.Schnare, R.Schwengner, S.Skoda, H.G.Thomas, H.Tiesler, D.Weisshaar, I.Wiedenhover Dipole Excitations in the Semi-Magic Nucleus 51V Studied with the (γ, γ') Reaction NUCLEAR REACTIONS 51V(γ, γ'), E=6.7 MeV bremsstrahlung; measured Eγ, Iγ, integrated σ. 51V deduced levels, Γ0, dipole strength distribution. Shell-model calculations with large model spaces. Composite HPGe detectors.
doi: 10.1016/S0375-9474(99)00375-9
1987AR12 Phys.Rev. A35, 2810 (1987) M.Arif, H.Kaiser, S.A.Werner, J.O.Willis Precision Measurement of the Bound-Coherent-Neutron Scattering Length of 235U NUCLEAR REACTIONS 235U(n, n), E=30-92 meV; measured bound coherent scattering lengths. Neutron interferometry.
doi: 10.1103/PhysRevA.35.2810
1986KA11 Physica 136B, 134 (1986) H.Kaiser, M.Arif, S.A.Werner, J.O.Willis Precision Measurement of the Scattering Amplitude of 235U NUCLEAR REACTIONS 235U(n, n), E=thermal; measured coherent scattering amplitudes. Interferometer.
doi: 10.1016/S0378-4363(86)80039-0
1979KA45 Z.Phys. A 291, 231 (1979) H.Kaiser, H.Rauch, G.Badurek, W.Bauspiess, U.Bonse Measurement of coherent neutron scattering lengths of gases NUCLEAR REACTIONS 1H(n, n), 1H(n, x), 2H(n, n), 2H(n, x), 3He(n, n), 3He(n, x), 4He(n, x), N(n, x), O(n, x), Ne(n, x), Ar(n, x), Kr(n, x), Xe(n, x), E=0.022707 eV; measured products, Eπ, Iπ; deduced scattering amplitudes, σ, σ(E). Data were imported from EXFOR entry 21622.
doi: 10.1007/BF01409188
1977KA31 Phys.Lett. B 71, 321 (1977) H.Kaiser, H.Rauch, W.Bauchspiess, U.Bonse Measurement Of The Coherent Neutron Scattering Length Of 3He By Neutron Interferometry NUCLEAR REACTIONS 3He(n, n), E=0.025 eV; measured products, 3He; deduced scattering amplitudes. Data were imported from EXFOR entry 20885.
doi: 10.1016/0370-2693(77)90227-1
1972FA02 Phys.Rev. C5, 120 (1972); Erratum Phys.Rev. C5, 1143 (1972) L.W.Fagg, W.L.Bendel, E.C.Jones, Jr., L.Cohen, H.F.Kaiser States in 36Ar Excited by 180° Electron Scattering NUCLEAR REACTIONS 36Ar(e, e'), E=39, 56 MeV; measured σ(Ee'). 36Ar deduced levels, J, π, transition radii, level-width, M1, M2 transitions.
doi: 10.1103/PhysRevC.5.120
1971BE18 Phys.Rev. C3, 1821 (1971) W.L.Bendel, L.W.Fagg, S.K.Numrich, E.C.Jones, Jr., H.F.Kaiser Excitation of 20Ne by 180° Electron Scattering NUCLEAR REACTIONS 20Ne(e, e'), E=39, 56 MeV; measured σ(Ee'). 20Ne deduced levels, level-width, transition radii.
doi: 10.1103/PhysRevC.3.1821
1971FA15 Phys.Rev. C4, 2089 (1971) L.W.Fagg, W.L.Bendel, L.Cohen, E.C.Jones, Jr., H.F.Kaiser, H.Uberall Magnetic Transition Strength in 32S and 40Ca from 180° Electron Scattering NUCLEAR REACTIONS 32S, 40Ca(e, e'), E=39, 56 MeV; measured σ(Ee'). 32S, 40Ca deduced levels, level-width, transition radii.
doi: 10.1103/PhysRevC.4.2089
1969FA12 Phys.Rev. 187, 1384 (1969) L.W.Fagg, W.L.Bendel, E.C.Jones, Jr., H.F.Kaiser, T.F.Godlove States of 25Mg Excited by 180° Electron Scattering NUCLEAR REACTIONS 25Mg(e, e'), E=39, 56 MeV; measured σ(Ee'). 25Mg deduced levels, J, π, level-width, T, transition radii.
doi: 10.1103/PhysRev.187.1384
1968BE33 Phys.Rev. 173, 1103 (1968) W.L.Bendel, L.W.Fagg, R.A.Tobin, H.F.Kaiser Inelastic Electron Scattering from 26Mg at 180° NUCLEAR REACTIONS 26Mg(e, e'), E=39.56 MeV; measured σ(Ee'). 26Mg deduced levels.
doi: 10.1103/PhysRev.173.1103
1968FA05 Phys.Rev. 171, 1250 (1968) L.W.Fagg, W.L.Bendel, R.A.Tobin, H.F.Kaiser Inelastic Electron Scattering from 24Mg at 180° NUCLEAR REACTIONS 24Mg(e, e'), E=39, 65 MeV; measured σ(Ee'). 24Mg levels deduced level-width.
doi: 10.1103/PhysRev.171.1250
1962KA09 Z.Phys. 166, 355 (1962) Die Messung der ungestorten Winkelkorrelation sukzessiver Kernstrahlungen in dunnen Aufdampfschichten NUCLEAR STRUCTURE 111In; measured not abstracted; deduced nuclear properties.
doi: 10.1007/BF01380782
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