- Vogt, A;
- Birkenbach, B;
- Reiter, P;
- Blazhev, A;
- Siciliano, M;
- Hadyńska-Klęk, K;
- Valiente-Dobón, JJ;
- Wheldon, C;
- Teruya, E;
- Yoshinaga, N;
- Arnswald, K;
- Bazzacco, D;
- Bowry, M;
- Bracco, A;
- Bruyneel, B;
- Chakrawarthy, RS;
- Chapman, R;
- Cline, D;
- Corradi, L;
- Crespi, FCL;
- Cromaz, M;
- de Angelis, G;
- Eberth, J;
- Fallon, P;
- Farnea, E;
- Fioretto, E;
- Freeman, SJ;
- Fu, B;
- Gadea, A;
- Geibel, K;
- Gelletly, W;
- Gengelbach, A;
- Giaz, A;
- Görgen, A;
- Gottardo, A;
- Hayes, AB;
- Hess, H;
- Hirsch, R;
- Hua, H;
- John, PR;
- Jolie, J;
- Jungclaus, A;
- Kaya, L;
- Korten, W;
- Lee, IY;
- Leoni, S;
- Lewandowski, L;
- Liang, X;
- Lunardi, S;
- Macchiavelli, AO;
- Menegazzo, R;
- Mengoni, D;
- Michelagnoli, C;
- Mijatović, T;
- Montagnoli, G;
- Montanari, D;
- Müller-Gatermann, C;
- Napoli, D;
- Pearson, CJ;
- Pellegri, L;
- Podolyák, Zs;
- Pollarolo, G;
- Pullia, A;
- Queiser, M;
- Radeck, F;
- Recchia, F;
- Regan, PH;
- Rosiak, D;
- Saed-Samii, N;
- Şahin, E;
- Scarlassara, F;
- Schneiders, D;
- Seidlitz, M;
- Siebeck, B;
- Sletten, G;
- Smith, JF;
- Söderström, P-A;
- Stefanini, AM;
- Steinbach, T;
- Stezowski, O;
- Szilner, S;
- Szpak, B;
- Teng, R;
- Ur, C;
- Vandone, V;
- Warner, DD;
- Wiens, A;
- Wu, CY;
- Zell, KO
The high-spin structures and isomers of the N=81 isotones Xe135 and Ba137 are investigated after multinucleon-transfer (MNT) and fusion-evaporation reactions. Both nuclei are populated (i) in Xe136+U238 and (ii) Xe136+Pb208 MNT reactions employing the high-resolution Advanced Gamma Tracking Array (AGATA) coupled to the magnetic spectrometer PRISMA, (iii) in the Xe136+Pt198 MNT reaction employing the γ-ray array GAMMASPHERE in combination with the gas-detector array CHICO, and (iv) via a B11+Te130 fusion-evaporation reaction with the HORUS γ-ray array at the University of Cologne. The high-spin level schemesof Xe135 and Ba137 are considerably extended to higher energies. The 2058-keV (19/2-) state in Xe135 is identified as an isomer, closing a gap in the systematics along the N=81 isotones. Its half-life is measured to be 9.0(9) ns, corresponding to a reduced transition probability of B(E2,19/2-→15/2-)=0.52(6) W.u. The experimentally deduced reduced transition probabilities of the isomeric states are compared to shell-model predictions. Latest shell-model calculations reproduce the experimental findings generally well and provide guidance to the interpretation of the new levels.