Search for key nuclear structure states below 132 Sn M. Górska, M. Pfützner, H. Grawe et al.

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Presentation transcript:

Search for key nuclear structure states below 132 Sn M. Górska, M. Pfützner, H. Grawe et al.

Motivation 1.Competition between: Shell evolution in neutron rich N=82 isotones: according to presented predictions in contrast to N=50 no Z=38,40 subshells Shell quenching in extreme neutron rich nuclei towards 122 Zr : a missing Z=38,40 subshell due to coupling to low-lying 2+ proton valence state creates a minimum neutron gap near mid-proton shell at Z=38,40 2.Astrophysics

Evidence for shell evolution 1/2- in 131 In about 300 keV lower than extrapolated for 99 In low-lying 3/2- and 5/2- states in 131 In Figure shows delta(1p,2p) and 2+ energy for single hole energy sequence as estimated for 131 In and as extrapolated for 99 In (dashed)

N = 82 odd mass chain SM33: ν h11/2 d3/2 s1/2 g7/2d5/2 π g9/2 p1/2 SMJ2: ν h11/2 d3/2 s1/2 g7/2d5/2 π g9/2 p1/2 p3/2 f5/2 Proton SPEs Possible E3 isomer Beta decaying isomer - 17/2- in 129 Ag is M2 isomer to 13/2+ or E2 to 13/2- (if sequence reversed) - isomer would be clear evidence for disappearing Z=38,40 subshell

N = 82 even mass chain Known 8+ seniority isomer possible new 8+ seniority isomer

N = 81 odd mass chain Neutron SPEs Possible new: 21/2+: E3,β 27/2-: E3, β Low spin β dec. isomer Possible new: 19/2+ : M2 23/2-: M2,ß to 19/2+ or E2 to 19/2- (if sequence rev.) 33/2+: E2 to 29/2+ and/or E3 to 27/2 Low spin β dec. isomer

N = 81even mass chain ?? Possible: 5+: E2 as in 130In 14+: M2 to 12- and/or E3 to 11- or ß 16-: E2 to 14- and/or M2 to 14+ low(3+)/high(10-) spin ß dec. isomers

N=80 odd mass chain Nothing new expected 17/2-: M2 to 13/2+ and/or E3 to 11/2+ 27/2+: M2 to 23/2- and/or E3 to 21/2- 29/2+: E3,ß (if sequence reversed) 37/2-: spin trap ß 41/2+: E2 to 37/2+ and/or M2 to 37/2- spin trap

N = 80 even mass chain Known, model check 18+ spin trap ß 10+: E2 to 8+ and/or E3 to : M2 to 14- and/or E3 to 13- or ß 18+: E2

Conclusions - new seniority isomers (not many) - many spin trap isomers - many new ß decaying isomers - core excited isomers (see 131 In) less safely predictable Spectroscopy data on these will serve to understand shell evolution towards 122 Zr