D.Y. Yin
Chinese Academy of Sciences
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by D.Y. Yin.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2018
R.J. Chen; X.L. Yan; W.W. Ge; Y. Yuan; M. Wang; M.Z. Sun; Y.M. Xing; P. Zhang; C. Y. Fu; P. Shuai; X. Xu; Y. H. Zhang; Tianwei Bao; X.C. Chen; X.J. Hu; W.J. Huang; H.F. Li; J.H. Liu; Yu.A. Livinov; S.A. Livinov; L.J. Mao; Bobing Wu; H. Xu; J. Yang; D.Y. Yin; Qin Zeng; X.H. Zhang; W.H. Zheng; X. H. Zhou; Xin Zhou
Abstract The Isochronous Mass Spectrometry (IMS) is a powerful technique developed in heavy-ion storage rings for measuring masses of very short-lived exotic nuclei. The IMS is based on the isochronous setting of the ring. One of the main parameters of this setting is the transition energy γ t . It has been a challenge to determine the γ t and especially to monitor the variation of γ t during experiments. In this paper we introduce a method to measure the γ t online during IMS experiments by using the acquired experimental data. Furthermore, since the storage ring has (in our context) a relatively large momentum acceptance, the variation of the γ t across the ring acceptance is a source of systematic uncertainty of measured masses. With the installation of two time-of-flight (TOF) detectors, the velocity of each stored ion and its revolution time are simultaneously available for the analysis. These quantities enabled us to determine the γ t as a function of orbital length in the ring. The presented method is especially important for future IMS experiments planned at the new-generation storage ring facilities FAIR in Germany and HIAF in China.
Chinese Physics C | 2016
Guo-Dong Shen; Jiancheng Yang; Jiawen Xia; L.J. Mao; D.Y. Yin; W.P. Chai; Jian Shi; Li-Na Sheng; A. Smirnov; Bo Wu; He Zhao
A new accelerator complex, HIAF (the High Intensity Heavy Ion Accelerator Facility), has been approved in China. It is designed to provide intense primary and radioactive ion beams for research in high energy density physics, nuclear physics, atomic physics as well as other applications. In order to achieve a high intensity of up to 5e11 ppp 238U34+, the Compression Ring (CRing) needs to stack more than 5 bunches transferred from the Booster Ring (BRing). However, the normal bucket to bucket injection scheme can only achieve an intensity gain of 2, so an injection method, fixed barrier bucket (BB) supported by electron cooling, is proposed. To suppress the severe space charge effect during the stacking process, off-alignment is adopted in the cooler to control the transverse emittance. In this paper, simulation and optimization with the BETACOOL program are presented.
Chinese Physics C | 2018
Nadir Khan; Z. M. Huang; Weiqiang Wen; Sultan Mahmood; Li-Jun Dou; Shu-Xing Wang; X. Xu; H.B. Wang; Chong-Yang Chen; Xiao-Ya Chuai; Xiaolong Zhu; Dong-Mei Zhao; L.J. Mao; Jie Li; D.Y. Yin; Jiancheng Yang; Youjin Yuan; Lin-Fan Zhu; Xinwen Ma
The accuracy of dielectronic recombination (DR) data for astrophysics related ions plays a key role in astrophysical plasma modeling. The absolute DR rate coefficient of Fe17+ ions was measured at the main cooler storage ring at the Institute of Modern Physics, Lanzhou, China. The experimental electron-ion collision energy range covers the first Rydberg series up to n = 24 for the DR resonances associated with the core excitations. A theoretical calculation was performed by using FAC code and compared with the measured DR rate coefficient. Overall reasonable agreement was found between the experimental results and calculations. Moreover, the plasma rate coefficient was deduced from the experimental DR rate coefficient and compared with the available results from the literature. At the low energy range, significant discrepancies were found, and the measured resonances challenge state-of-the-art theory at low collision energies.
Chinese Physics C | 2016
Caojie Shao; Deyang Yu; Rongchun Lu; T.C. Zhao; R. S. Mao; Jie Li; Yingli Xue; Wei Wang; Bian Yang; Mingwu Zhang; J. P. Liu; Zhangyong Song; Xiaohong Cai; Ximeng Chen; D.Y. Yin; L.J. Mao; Xiaodong Yang; Jiancheng Yang; Youjin Yuan
The target thickness for nitrogen was determined from the beam energy loss in HIRFL-CSRe during the experimental study of the K-REC process in 197 MeV/u Xe54+-N-2 collisions. Furthermore, the corresponding integrated luminosity of (1.15 +/- 0.06) x 10(30) cm(-2) was obtained. As an independent check on the energy-loss method, we have also determined the integrated luminosity by measuring the produced X-rays from the K-REC process with a known differential cross section. The values of (1.12 +/- 0.06) x 10(30) and (1.09 +/- 0.06) x 10(30) cm(-2) were obtained by using two high-purity germanium (HPGe) detectors which were oriented at 90 degrees and 120 degrees with respect to the beam path, respectively. The consistent results confirmed the feasibility of the energy-loss method, which may have an important impact on future internal target experiments at HIRFL-CSRe.
Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms | 2013
Jiancheng Yang; Jiawen Xia; G Q Xiao; H. Xu; H. W. Zhao; Xin Zhou; X. W. Ma; Y. He; L. Ma; Daqing Gao; J. Meng; Zijian Xu; R. S. Mao; Wei Zhang; Y. Wang; Litao Sun; Youjin Yuan; P. Yuan; W.L. Zhan; Jian Shi; W.P. Chai; D.Y. Yin; Peng Li; Jianxu Li; L.J. Mao; Jun Zhang; Li-Na Sheng
Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms | 2013
Youjin Yuan; Jiancheng Yang; Jiawen Xia; P. Yuan; Wei-Min Qiao; Daqing Gao; G Q Xiao; H. W. Zhao; Hu-Shan Xu; Mingtao Song; Xiaotian Yang; Xiaohong Cai; L. Ma; Xin-An Yang; Kai-Di Man; Yuan He; Zhuyao Zhou; Junhui Zhang; Zijian Xu; Yu Liu; R. S. Mao; Wei Zhang; D.Z. Xie; Litao Sun; Yaqing Yang; D.Y. Yin; Peng Li; Jianxu Li; Jian Shi; W.P. Chai
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2015
L.J. Mao; J. Yang; J.W. Xia; X.D. Yang; Y. Yuan; J. Li; X.M. Ma; Tingxing Yan; D.Y. Yin; W.P. Chai; Lizhi Sheng; Guo-Dong Shen; H. W. Zhao; M.T. Tang
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2014
X. Gao; Youjin Yuan; Jiancheng Yang; S. Litvinov; Meng Wang; Yuri A. Litvinov; Wei Zhang; D.Y. Yin; Guo-Dong Shen; W.P. Chai; Jian Shi; Peng Shang
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2013
Jian Shi; Jiancheng Yang; Jiawen Xia; Y.J. Yuan; R. S. Mao; W.P. Chai; Jie Li; D.Y. Yin
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2018
Bobing Wu; J. Yang; J.W. Xia; X.L. Yan; X.J. Hu; L.J. Mao; Lizhi Sheng; J. Wu; D.Y. Yin; W.P. Chai; Guo-Dong Shen; W.W. Ge; Guanglei Wang; H. W. Zhao; Shuang Ruan; X. W. Ma; M. Wang; S. Litvinov; Wenlong Wen; X.C. Chen; R.J. Chen; M.T. Tang; W. Wu; Cheng Luo; T.C. Zhao; C.F. Shi; X. Fu; J. Liu; L. Y. Liang