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Superdeformation in $$^{35}$$S

Go, Shintaro*; Ideguchi, Eiji*; Yokoyama, Rin*; Kobayashi, Motoki*; Kisamori, Keiichi*; Takaki, Motonobu*; Miya, Hioyuki*; Ota, Shinsuke*; Michimasa, Shinichiro*; Shimoura, Susumu*; Niikura, Megumi*; Koike, Takeshi*; Yamamoto, Takeshi*; Ito, Yosuke*; Takatsu, Jun*; Yagi, Ayumi*; Nishibata, Hiroki*; Suzuki, Tomokazu*; Shirotori, Kotaro*; Watanabe, Yutaka*; Hirayama, Yoshikazu*; Sugawara, Masahiko*; Koizumi, Mitsuo; Toh, Yosuke  ; Shizuma, Toshiyuki; Kimura, Atsushi; Harada, Hideo  ; Furutaka, Kazuyoshi; Nakamura, Shoji; Kitatani, Fumito; Hatsukawa, Yuichi; Oshima, Masumi; Matea, I.*; Suzuki, Daisuke*; Verney, D.*; Azaiez, F.*

The high-spin states in $$^{35}$$S were investigated at Tandem-ALTO facility in Institut de Physique Nucl$'e$aire d'Orsay The $$^{26}$$Mg($$^{18}$$O, 2$$alpha$$1n)$$^{35}$$S fusion evaporation reaction was used to populate high-spin states in $$^{35}$$S. The germanium $$gamma$$-ray detector array ORGAM was employed to measure $$gamma$$ rays from high-spin states and charged particles evaporated from the compound nuclei were detected by a segmented silicon detector, Si-Ball. A level scheme for $$^{35}$$S was deduced based on the gamma-gamma-coincidence analysis and $$gamma$$-ray angular correlation analysis. The half-life of the transition in the superdeformed band was estimated by measuring the residual Doppler shift. The deduced half-life shows the large collectivity of the band.

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