{"title":"重述triton和$^3$He的产率比作为富中子颈发射的指标","authors":"Wang, Yijie, Wan, Mengting, Diao, Xinyue, Xiao, Sheng, Qin, Yuhao, Qin, Zhi, Guo, Dong, Si, Dawei, Zhang, Boyuan, Tian, Baiting, Guan, Fenhai, Wu, Qianghua, Wei, Xianglun, Yang, Herun, Ma, Peng, Hu, Rongjiang, Duan, Limin, Duan, Fangfang, Ma, Junbing, Xu, Shiwei, Hu, Qiang, Bai, Zhen, Yang, Yanyun, Wang, Jiansong, Liu, Wenbo, Su, Wanqing, Wei, Xiaobao, Ma, Chunwang, Li, Xinxiang, Wang, Hongwei, Zhang, Yingxun, Warda, Michał, Dobrowolski, Arthur, Nerlo-Pomorska, Bożena, Pomorski, Krzysztof, Ou, Li, Xiao, Zhigang","doi":"10.48550/arxiv.2311.07095","DOIUrl":null,"url":null,"abstract":"The neutron rich neck zone created in heavy ion reaction is experimentally probed by the production of the $A=3$ isobars. The energy spectra and angular distributions of triton and $^3$He are measured with the CSHINE detector in $^{86}$Kr +$^{208}$Pb reactions at 25 MeV/u. While the energy spectrum of $^{3}$He is harder than that of triton, known as \"$^{3}$He-puzzle\", the yield ratio $R({\\rm t/^3He})$ presents a robust rising trend with the polar angle in laboratory. Using the fission fragments to reconstruct the fission plane, the enhancement of out-plane $R({\\rm t/^3He})$ is confirmed in comparison to the in-plane ratios. Transport model simulations reproduce qualitatively the experimental trends, but the quantitative agreement is not achieved. The results demonstrate that a neutron rich neck zone is formed in the reactions. Further studies are called for to understand the clustering and the isospin dynamics related to neck formation.","PeriodicalId":496270,"journal":{"name":"arXiv (Cornell University)","volume":"119 48","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2023-11-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Revisit to the yield ratio of triton and $^3$He as an indicator of\\n neutron-rich neck emission\",\"authors\":\"Wang, Yijie, Wan, Mengting, Diao, Xinyue, Xiao, Sheng, Qin, Yuhao, Qin, Zhi, Guo, Dong, Si, Dawei, Zhang, Boyuan, Tian, Baiting, Guan, Fenhai, Wu, Qianghua, Wei, Xianglun, Yang, Herun, Ma, Peng, Hu, Rongjiang, Duan, Limin, Duan, Fangfang, Ma, Junbing, Xu, Shiwei, Hu, Qiang, Bai, Zhen, Yang, Yanyun, Wang, Jiansong, Liu, Wenbo, Su, Wanqing, Wei, Xiaobao, Ma, Chunwang, Li, Xinxiang, Wang, Hongwei, Zhang, Yingxun, Warda, Michał, Dobrowolski, Arthur, Nerlo-Pomorska, Bożena, Pomorski, Krzysztof, Ou, Li, Xiao, Zhigang\",\"doi\":\"10.48550/arxiv.2311.07095\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The neutron rich neck zone created in heavy ion reaction is experimentally probed by the production of the $A=3$ isobars. The energy spectra and angular distributions of triton and $^3$He are measured with the CSHINE detector in $^{86}$Kr +$^{208}$Pb reactions at 25 MeV/u. While the energy spectrum of $^{3}$He is harder than that of triton, known as \\\"$^{3}$He-puzzle\\\", the yield ratio $R({\\\\rm t/^3He})$ presents a robust rising trend with the polar angle in laboratory. Using the fission fragments to reconstruct the fission plane, the enhancement of out-plane $R({\\\\rm t/^3He})$ is confirmed in comparison to the in-plane ratios. Transport model simulations reproduce qualitatively the experimental trends, but the quantitative agreement is not achieved. The results demonstrate that a neutron rich neck zone is formed in the reactions. Further studies are called for to understand the clustering and the isospin dynamics related to neck formation.\",\"PeriodicalId\":496270,\"journal\":{\"name\":\"arXiv (Cornell University)\",\"volume\":\"119 48\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2023-11-13\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv (Cornell University)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.48550/arxiv.2311.07095\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv (Cornell University)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.48550/arxiv.2311.07095","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Revisit to the yield ratio of triton and $^3$He as an indicator of
neutron-rich neck emission
The neutron rich neck zone created in heavy ion reaction is experimentally probed by the production of the $A=3$ isobars. The energy spectra and angular distributions of triton and $^3$He are measured with the CSHINE detector in $^{86}$Kr +$^{208}$Pb reactions at 25 MeV/u. While the energy spectrum of $^{3}$He is harder than that of triton, known as "$^{3}$He-puzzle", the yield ratio $R({\rm t/^3He})$ presents a robust rising trend with the polar angle in laboratory. Using the fission fragments to reconstruct the fission plane, the enhancement of out-plane $R({\rm t/^3He})$ is confirmed in comparison to the in-plane ratios. Transport model simulations reproduce qualitatively the experimental trends, but the quantitative agreement is not achieved. The results demonstrate that a neutron rich neck zone is formed in the reactions. Further studies are called for to understand the clustering and the isospin dynamics related to neck formation.