about
Low-energy enhancement of magnetic dipole radiation.Cross-Section Measurements of theKr86(γ,n)Reaction to Probe thes-Process Branching atKr85Fine Structure of the GiantM1Resonance inZr90Electromagnetic dipole strength of136Ba below the neutron separation energyMagnetic dipole excitations ofCr50Dipole strength inLa139below the neutron-separation energyNuclear Deformation and Neutron Excess as Competing Effects for Dipole Strength in the Pygmy RegionEXILL—a high-efficiency, high-resolution setup for γ-spectroscopy at an intense cold neutron beam facilityThe (n,γ) campaigns at EXILLNuclear astrophysics with radioactive ions at FAIRExperimentally constrained(p,γ)Y89and(n,γ)Y89reaction rates relevant top-process nucleosynthesisUpbend and M1 Scissors Mode in Neutron-rich Nuclei --- Consequences for r-process $(n,\gamma )$ Reaction Ratesβ decay ofAg95High-spin states in109Sn and their decay to the ground stateIn-beam study of 109SnSolving the stellar 62Ni problem with AMSBeta decay of 101SnBeta decay of the proton-rich nuclei 102Sn and 104SnBeta decay of 103SnBeta-decay spectroscopy of 103, 105SnBeta-decay studies near 100SnStudies of β-delayed proton decays of N≃Z nuclei around 100Sn at the GSI-ISOL facilityCharacterization of the neutron beam at nELBECompact high energy x-ray spectrometer based on forward Compton scattering for high intensity laser plasma experimentsCompleting the nuclear reaction puzzle of the nucleosynthesis ofMo92Low-energy enhancement in theγ-ray strength functions ofGe73,74Nature of low-lying electric dipole resonance excitations inGe74First evidence of low energy enhancement in Ge isotopesEvidence for Nontermination of Rotational Bands inKr74Photon scattering experiments on the quasistable, odd-odd mass nucleusLu176Low-lyingE1,M1, andE2strength distributions inXe124,126,128,129,130,131,132,134,136: Systematic photon scattering experiments in the mass region of a nuclear shape or phase transitionSystematics of magnetic dipole strength in the stable even-mass Mo isotopesDecay of1+States as a New Probe of the Structure of0+Shape IsomersInfluence of theN=50neutron core on dipole excitations in87RbSignature inversion caused by triaxiality and unpaired band crossings in 72BrFirst observation of the scissors mode in a gamma -soft nucleus: The case of 196PtQuadrupole moment of the 11(-) intruder isomer in 196Pb and its implications for the 16(-) shears band headStudy of excited states in 85Kr and 86Kr: Evidence for neutron-core excitations in the N=50 nucleus 86KrThree-quasiparticle excitations in 77BrExcited states built on the 6(-) isomer in 3786Rb49
P50
Q54323382-4C2EAF84-1DFC-44BE-B142-5F2234683D5FQ57425745-8ECCF5D9-0330-46D2-AEF3-A3AD3C54C67BQ57428370-7BA0EEC3-68D6-4207-A851-D2CA8D12EA85Q57431056-3A54EA54-AE37-4DFC-85DB-AE02C5D47498Q57433482-FE341F9A-2B61-4119-8F9D-D00EA9471B37Q57439305-57D56B7F-0635-4463-8795-71CC3045A4A1Q57443379-39E72915-497F-48F8-A4D7-44860C0C2B12Q57632863-FD9676D4-9616-4B0A-A1BC-292AC1BDFB1EQ57632934-58E8A9DD-F093-45EA-B734-2ED945342E8FQ57675988-B114EFC2-1B8A-457C-9ADF-5F4F8822A19AQ58215985-0643F26F-36FA-4244-9805-8DF18FAD66F1Q58216008-73373998-D067-45E1-B9BC-6EB90F2C40D3Q58216222-2796347D-39CC-434E-96A5-98E63AA3AD5BQ59478382-34A67ED3-6EEA-4618-BFB8-D9561B486207Q59478388-1C6A6A3E-1F50-4AB1-8A82-05262816E975Q60561248-23322F4B-0F86-4E48-B892-F99A7C2AADDFQ60561275-3D41656D-B8A6-4E28-9D8F-52BB738C4B2CQ60561281-7BB5B368-91ED-4234-BDA8-F6BBC765ECD1Q60561295-E6D7E29A-E47C-4695-B488-58E937B92DEDQ60561296-ACC90083-EA2A-45B8-8CF1-6F48D143026FQ60561297-6AEA9B88-137D-4DD4-A8CC-90041C76ACE4Q60561308-395FC836-8999-42B1-8C6E-B5D88812BDBBQ61646445-DEC7003D-51CD-4FBE-93B6-710D4A6ED43CQ61924138-ADB1A0A0-E3D7-4190-9225-321E434451A9Q63387852-A507B2C3-18E4-4028-9A0F-25E6564552A3Q63387872-A628B7A4-8D26-4B8A-8FF0-DA5E8B2F91D3Q63387874-A6DC7A7A-BB41-49AF-9376-D66AF3777F86Q63387896-BC946A10-B2A9-4D99-B3F3-088ACF835A20Q63388069-D8AAAC9D-2BE4-4590-8A5A-2198E2AD2EB8Q63388344-EDA395BC-0B62-415B-84D7-C4A9A5A36659Q63388352-30344C3C-40FA-49FA-8E11-9BAE29C11A40Q63388353-736CC627-B6D2-4C1E-A68E-155D000F7C6BQ63388357-1833ED36-C1C2-4555-B8FF-634EFCF52DA1Q63388382-005E9B60-AD0D-4388-BF11-11F290419420Q74290305-9B596501-6D82-458A-9156-2F491E1CBD5FQ74566035-DC986E46-D934-458B-94C1-D35ABC95159EQ77807806-7B7F862A-03A2-4795-B116-269FA55CB95FQ78094612-E866EC5E-BEDD-4DD4-AEFD-29A9EAF5B880Q78095250-55EEDA45-B739-4AA2-B555-2F5C9DAB21CCQ78096779-391F436A-414F-41E3-8720-EACDDB88024C
P50
description
forsker
@nb
researcher ORCID ID = 0000-0002-7620-8882
@en
wetenschapper
@nl
name
R. Schwengner
@ast
R. Schwengner
@nl
Ronald Schwengner
@en
Ronald Schwengner
@nb
type
label
R. Schwengner
@ast
R. Schwengner
@nl
Ronald Schwengner
@en
Ronald Schwengner
@nb
altLabel
R. Schwengner
@en
prefLabel
R. Schwengner
@ast
R. Schwengner
@nl
Ronald Schwengner
@en
Ronald Schwengner
@nb
P31
P496
0000-0002-7620-8882