TY - JOUR
T1 - Production of 265Sg in the 248Cm(22Ne,5n)265Sg reaction and decay properties of two isomeric states in 265Sg
AU - Haba, H.
AU - Kaji, D.
AU - Kudou, Y.
AU - Morimoto, K.
AU - Morita, K.
AU - Ozeki, K.
AU - Sakai, R.
AU - Sumita, T.
AU - Yoneda, A.
AU - Kasamatsu, Y.
AU - Komori, Y.
AU - Shinohara, A.
AU - Kikunaga, H.
AU - Kudo, H.
AU - Nishio, K.
AU - Ooe, K.
AU - Sato, N.
AU - Tsukada, K.
PY - 2012/2/21
Y1 - 2012/2/21
N2 - Two isomeric states of 265Sg, i.e., 265Sga and 265Sgb, proposed in Ch. E. Düllmann and A. Türler were produced in the 248Cm(22Ne,5n)265Sg reaction. Decay properties of 265Sga,b were investigated with a rotating-wheel apparatus for α and spontaneous fission (SF) spectrometry under low background conditions attained by a gas-jet transport system coupled to the RIKEN gas-filled recoil ion separator. Based on genetically correlated α-α(-α) and α-SF decay chains, 18 and 24 events were assigned to 265Sga and 265Sgb, respectively. The half-life T1/2 and α-particle energy Eα of 265Sga were measured to be 8.5-1.6+2.6 s and 8.84 ± 0.05 MeV, respectively, and those of 265Sgb were 14.4-2.5+3.7 s and 8.69 ± 0.05 MeV. As a daughter product of 265Sga ,b, the decay properties of the 3-s isomeric state in 261Rf, i.e., 261Rfb, were also derived: T1/2 = 2.6-0.5+0.7 s, Eα = 8.51 ± 0.06 MeV, and SF branch bSF = 0.82 ± 0.09. These results confirm and refine the decay pattern suggested for the decay chain 269Hs → 265Sga,b → 261Rfa,b → 257No → in Düllmann and Türler. The production cross sections for 265Sga and 265Sgb were determined to be 180-60+80 and 200-50+60 pb at 117.8 MeV, respectively, and they are discussed by comparing with the literature data as well as the theoretical prediction.
AB - Two isomeric states of 265Sg, i.e., 265Sga and 265Sgb, proposed in Ch. E. Düllmann and A. Türler were produced in the 248Cm(22Ne,5n)265Sg reaction. Decay properties of 265Sga,b were investigated with a rotating-wheel apparatus for α and spontaneous fission (SF) spectrometry under low background conditions attained by a gas-jet transport system coupled to the RIKEN gas-filled recoil ion separator. Based on genetically correlated α-α(-α) and α-SF decay chains, 18 and 24 events were assigned to 265Sga and 265Sgb, respectively. The half-life T1/2 and α-particle energy Eα of 265Sga were measured to be 8.5-1.6+2.6 s and 8.84 ± 0.05 MeV, respectively, and those of 265Sgb were 14.4-2.5+3.7 s and 8.69 ± 0.05 MeV. As a daughter product of 265Sga ,b, the decay properties of the 3-s isomeric state in 261Rf, i.e., 261Rfb, were also derived: T1/2 = 2.6-0.5+0.7 s, Eα = 8.51 ± 0.06 MeV, and SF branch bSF = 0.82 ± 0.09. These results confirm and refine the decay pattern suggested for the decay chain 269Hs → 265Sga,b → 261Rfa,b → 257No → in Düllmann and Türler. The production cross sections for 265Sga and 265Sgb were determined to be 180-60+80 and 200-50+60 pb at 117.8 MeV, respectively, and they are discussed by comparing with the literature data as well as the theoretical prediction.
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U2 - 10.1103/PhysRevC.85.024611
DO - 10.1103/PhysRevC.85.024611
M3 - Article
AN - SCOPUS:84857533947
SN - 0556-2813
VL - 85
JO - Physical Review C - Nuclear Physics
JF - Physical Review C - Nuclear Physics
IS - 2
M1 - 024611
ER -