ENTRY S0320 20251010 S032000000001 SUBENT S0320001 20251010 20260228 S032000100001 BIB 12 48 S032000100002 TITLE Charge-changing cross section measurements of 300 S032000100003 MeV/nucleon 28Si on carbon and data analysis S032000100004 AUTHOR (Chang-Jian Wang, Ge Guo, Hooi Jin Ong, Yu-Nan Song, S032000100005 Bao-Hua Sun, Isao Tanihata, Satoru Terashima, S032000100006 Xiu-Lin Wei, Jun-Yao Xu, Xiao-Dong Xu, Ji-Chao Zhang, S032000100007 Yong Zheng, Li-Hua Zhu, Yong Cao, Guang-Wei Fan, S032000100008 Bing-Shui Gao, Jia-Xing Han, Guang-Shuai Li, S032000100009 Chen-Gui Lu, Hao-Tian Qi, Yun Qin, Zhi-Yu Sun, S032000100010 Lu-Ping Wan, Kai-Long Wang, Shi- Tao Wang, S032000100011 Xin-Xu Wang, Mei-Xue Zhang, Wen-Wen Zhang, S032000100012 Xiao-Bin Zhang, Xue-Heng Zhang, Zi-Cheng Zhou) S032000100013 INSTITUTE (3CPRBHN,3CPRIMP,3CPRUCA) S032000100014 (3CPRCPR) Anhui University of Science and Technology, S032000100015 Huainan S032000100016 REFERENCE (J,CPH/C,47,084001,2023) S032000100017 #doi:10.1088/1674-1137/acd366 S032000100018 FACILITY (CYCLO,3CPRIMP) The second Radioactive Ion Beam Line S032000100019 in Lanzhou (RIBLL2) of the Heavy Ion Research S032000100020 Facility in Lanzhou (HIRFL) S032000100021 INC-SOURCE 9Be(40Ar,28Si). A primary Ar-40 beam was accelerated S032000100022 to 400 MeV/nucleon at the main cooler storage S032000100023 ring(CSRm) and guided in the slow extraction mode to S032000100024 impinge on a 10-mm thick beryllium target. The S032000100025 secondary beam of interest was then transported by S032000100026 the RIBLL2 to bombard the reaction target. S032000100027 SAMPLE The reaction target was made of natural carbon with a S032000100028 thickness of 1.855 g/cm2. S032000100029 DETECTOR (SCIN,IOCH,MWDC) Upstream of the reaction target, a S032000100030 fast timing scintillator detector and a multiple S032000100031 sampling ionization chamber sandwiched by two S032000100032 multi-wire drift chambers were installed. Downstream S032000100033 of the reaction target, there was a similar setup S032000100034 consisting of one ionization chamber and two drift S032000100035 chambers. The combination of two multi-wire drift S032000100036 chambers before and after the reaction target was S032000100037 utilized to determine the trajectories of incoming S032000100038 and outgoing particles. The Time-of-Flight and S032000100039 energy-loss for incident ions were determined on an S032000100040 event-by-event basis by the scintillator detectors S032000100041 and multiple sampling ionization chamber. S032000100042 METHOD (TOFDE) The particle identification for the incoming S032000100043 ions upstream of the reaction target was achieved by S032000100044 employing the standard delta-E-TOF-Bp method. S032000100045 ERR-ANALYS (ERR-T) The total uncertainty. S032000100046 (ERR-S) The statistical uncertainty. S032000100047 (ERR-1) The contamination from neighboring isotopes. S032000100048 STATUS (TABLE,,Chang-Jian Wang+,J,CPH/C,47,084001,2023) S032000100049 HISTORY (20251010C) Chen Ying S032000100050 ENDBIB 48 0 S032000100051 NOCOMMON 0 0 S032000100052 ENDSUBENT 51 0 S032000199999 SUBENT S0320002 20251010 20260228 S032000200001 BIB 1 1 S032000200002 REACTION (6-C-0(14-SI-28,TCC),,SIG) S032000200003 ENDBIB 1 0 S032000200004 NOCOMMON 0 0 S032000200005 DATA 6 1 S032000200006 EN EN-RSL-HW DATA ERR-T ERR-S ERR-1 S032000200007 MEV/A MEV/A MB MB MB MB S032000200008 304. 9. 1125. 11. 10.5 0.6S032000200009 ENDDATA 3 0 S032000200010 ENDSUBENT 9 0 S032000299999 ENDENTRY 2 0 S032099999999