摘要
Super heavy nucleus (SHN) is usually produced at its excited state, and will decay via light particle emission or fission. The survival probability of the excited compound nucleus is considered as one of the crucial factors for producing SHN, which is determined by the competition between the neutron emission and the fission. It is well known that the fission barrier of a nucleus decreases with the increasing angular momentum of the nucleus. The behavior of the survival probability with the angular momentum is of interesting.
Super heavy nucleus （SHN） is usually produced at its excited state, and will decay via light particle emission or fission. The survival probability of the excited compound nucleus is considered as one of the crucial factors for producing SHN, which is determined by the competition between the： neutron emission and the fission. It is well known that the fission barrier of a nucleus decreases with the increasing angular momentum of the nucleus. The behavior of the survival probability with the angular momentum is of interesting.
