期刊文献+
共找到6篇文章
< 1 >
每页显示 20 50 100
三轴形变核^(131)Ba中的奇异集体激发模式
1
作者 韦锐 周厚兵 +34 位作者 王思成 丁兵 强赟华 贾晨旭 陈红星 郭松 C.M.Petrache D.Mengoni A.Astier E.Dupont 吕冰锋 D.Bazzacco A.Boso A.Goasduff F.Recchia D.Testov F.Galtarossa G.Jaworski D.R.Napoli S.Riccetto M.Siciliano J.J.Valiente-Dobon C.Andreoiu F.H.Garcia K.Ortner K.Whitmore A.Ataç-Nyberg T.Bäck B.Cederwall E.A.Lawrie I.Kuti D.Sohler T.Marchlewski J.Srebrny A.Tucholski 《物理学报》 SCIE EI CAS CSCD 北大核心 2024年第11期89-100,共12页
利用意大利Legnaro实验室串列静电加速器提供的65 MeV^(13)C束流与122Sn靶的熔合蒸发反应布居了^(131)Ba的高自旋态,并搭建了新的能级纲图.新的能级纲图由15条转动带组成,包括三对手征双重带,其中两对正宇称手征带为赝自旋-手征四重带.... 利用意大利Legnaro实验室串列静电加速器提供的65 MeV^(13)C束流与122Sn靶的熔合蒸发反应布居了^(131)Ba的高自旋态,并搭建了新的能级纲图.新的能级纲图由15条转动带组成,包括三对手征双重带,其中两对正宇称手征带为赝自旋-手征四重带.正负宇称手征带通过一系列增强的E1跃迁连接,表明它们之间存在八极关联.在低自旋区域搭建了一条新的转动带,通过一系列γ跃迁向νh1_(1/2)晕带退激.这种能级结构与摇摆带相似,但基于现有的实验证据还难以将它确认为摇摆带,不能排除其他集体激发机制,如γ振动的影响. 展开更多
关键词 高自旋态 手征带 赝自旋 八极关联 摇摆运动
在线阅读 下载PDF
The density profiles of dark matter halos in spiral galaxies
2
作者 Gianluca Castignani Noemi Frusciante +1 位作者 Daniele Vernieri Paolo Salucci 《Natural Science》 2012年第5期265-270,共6页
In spiral galaxies, we explain their non-Keplerian rotation curves (RCs) by means of a non-luminous component embedding their stellar-gaseous disks. Understanding the detailed properties of this component (labelled Da... In spiral galaxies, we explain their non-Keplerian rotation curves (RCs) by means of a non-luminous component embedding their stellar-gaseous disks. Understanding the detailed properties of this component (labelled Dark Matter, DM) is one of the most pressing issues of Cosmology. We investigate the recent relationship (claimed by Walker et al. 2010, hereafter W + 10) between r, the galaxy radial coordinate, and Vh(r), the dark halo contribution to the circular velocity at r, 1) in the framework of the Universal Rotation Curve (URC) paradigm and directly 2) by means of the kinematics of a large sample of DM dominated spirals. We find a general agreement between the W + 10 claim, the distribution of DM emerging from the URC and that inferred in the (low luminosity) objects of our sample. We show that such a phenomenology, linking the spiral’s luminosity, radii and circular velocities, implies an evident inconsistency with (naive) predictions in the Λ Cold Dark Matter (ΛCDM) scenario. 展开更多
关键词 GALAXIES SPIRAL KINEMATICS and DYNAMICS DARK MATTER
在线阅读 下载PDF
Isospin Splitting of Neutron and Proton Effective Masses in Neutron-rich Nuclear Matter
3
作者 Zuo Wei Cao Ligang +1 位作者 Li Baoan U. Lombardo 《近代物理研究所和兰州重离子加速器实验室年报:英文版》 2005年第1期1-1,3,共2页
We investigate the isospin splitting of neutron and proton effective masses in neutron-rich nuclear matter by using Brueckner-Hartree-Fock (BHF) approach and the extended BHF (EBHF) approach including the ground state... We investigate the isospin splitting of neutron and proton effective masses in neutron-rich nuclear matter by using Brueckner-Hartree-Fock (BHF) approach and the extended BHF (EBHF) approach including the ground state correlation contributions. The realistic nucleon-nucleon interaction adopted in our calculation is the Argonne V18 two-body force supplemented with a microscopic three-body force constructed from the meson-exchange current approach. The result is reported in Fig. 1 where the neutron and proton effective masses are plotted as functions of isospin asymmetry parameterβ. It is shown that in both cases by adopting the BHF and EBHF approaches, the predicted neutron effective mass is greater 展开更多
关键词 丰中子 同位旋 核物质 理论核物理 质子 生效 劈裂 有效质量
在线阅读 下载PDF
证券化应建立在优质资源基础上
4
作者 饶芳 《新财富》 2003年第7期16-17,共2页
陈志武教授在《新财富》今年5、6月号专栏中的财富观,我觉得其核心是证券化。《财富是怎样产生的》主要讲消费,陈教授认为强大的内需是一国经济持续增长的原动力,而巨额储蓄抑制了内需的增长,在出口受阻的情况下.会使该国经济遭受... 陈志武教授在《新财富》今年5、6月号专栏中的财富观,我觉得其核心是证券化。《财富是怎样产生的》主要讲消费,陈教授认为强大的内需是一国经济持续增长的原动力,而巨额储蓄抑制了内需的增长,在出口受阻的情况下.会使该国经济遭受重创。因此,全面启动内需.引导储蓄转向消费、投资是促进经济增长的必由之路。 展开更多
关键词 “内需” 经济增长 消费证券化 生产证券化 资源
原文传递
实体经济与制度、金融创新同等重要
5
作者 郝丹丹 《新财富》 2003年第8期8-8,共1页
关键词 实体经济 制度创新 金融创新 金融泡沫 居民收入
原文传递
Prediction of energy resolution in the JUNO experiment
6
作者 Angel Abusleme Thomas Adam +651 位作者 Kai Adamowicz Shakeel Ahmad Rizwan Ahmed Sebastiano Aiello Fengpeng An Qi An Giuseppe Andronico Nikolay Anfimov Vito Antonelli Tatiana Antoshkina Joao Pedro Athayde Marcondes de André Didier Auguste Weidong Bai Nikita Balashov Wander Baldini Andrea Barresi Davide Basilico Eric Baussan Marco Bellato Marco Beretta Antonio Bergnoli Daniel Bick Lukas Bieger Svetlana Biktemerova Thilo Birkenfeld Iwan Blake David Blum Simon Blyth Anastasia Bolshakova Mathieu Bongrand Clément Bordereau Dominique Breton Augusto Brigatti Riccardo Brugnera Riccardo Bruno Antonio Budano Jose Busto Anatael Cabrera Barbara Caccianiga Hao Cai Xiao Cai Yanke Cai Zhiyan Cai Stéphane Callier Steven Calvez Antonio Cammi Agustin Campeny Chuanya Cao Guofu Cao Jun Cao Rossella Caruso Cédric Cerna Vanessa Cerrone Jinfan Chang Yun Chang Auttakit Chatrabhuti Chao Chen Guoming Chen Pingping Chen Shaomin Chen Xin Chen Yiming Chen Yixue Chen Yu Chen Zelin Chen Zhangming Chen Zhiyuan Chen Zikang Chen Jie Cheng Yaping Cheng YuChin Cheng Alexander Chepurnov Alexey Chetverikov Davide Chiesa Pietro Chimenti Yen-Ting Chin Po-Lin Chou Ziliang Chu Artem Chukanov Gérard Claverie Catia Clementi Barbara Clerbaux Marta Colomer Molla Selma Conforti Di Lorenzo Alberto Coppi Daniele Corti Simon Csakli Chenyang Cui Flavio Dal Corso Olivia Dalager Jaydeep Datta Christophe De La Taille Zhi Deng Ziyan Deng Xiaoyu Ding Xuefeng Ding Yayun Ding Bayu Dirgantara Carsten Dittrich Sergey Dmitrievsky Tadeas Dohnal Dmitry Dolzhikov Georgy Donchenko Jianmeng Dong Evgeny Doroshkevich Wei Dou Marcos Dracos Frédéric Druillole Ran Du Shuxian Du Katherine Dugas Stefano Dusini Hongyue Duyang Jessica Eck Timo Enqvist Andrea Fabbri Ulrike Fahrendholz Lei Fan Jian Fang Wenxing Fang Dmitry Fedoseev Li-Cheng Feng Qichun Feng Federico Ferraro Amélie Fournier Fritsch Fritsch Haonan Gan Feng Gao Feng Gao Alberto Garfagnini Arsenii Gavrikov Marco Giammarchi Nunzio Giudice Maxim Gonchar Guanghua Gong Hui Gong Yuri Gornushkin Marco Grassi Maxim Gromov Vasily Gromov Minghao Gu Xiaofei Gu Yu Gu Mengyun Guan Yuduo Guan Nunzio Guardone Rosa Maria Guizzetti Cong Guo Wanlei Guo Caren Hagner Hechong Han Ran Han Yang Han Miao He Wei He Xinhai He Tobias Heinz Patrick Hellmuth Yuekun Heng Rafael Herrera YuenKeung Hor Shaojing Hou Yee Hsiung Bei-Zhen Hu Hang Hu Jun Hu Peng Hu Shouyang Hu Tao Hu Yuxiang Hu Zhuojun Hu Guihong Huang Hanxiong Huang Jinhao Huang Junting Huang Kaixuan Huang Shengheng Huang Wenhao Huang Xin Huang Xingtao Huang Yongbo Huang Jiaqi Hui Lei Huo Wenju Huo Cédric Huss Safeer Hussain Leonard Imbert Ara Ioannisian Roberto Isocrate Arshak Jafar Beatrice Jelmini Ignacio Jeria Xiaolu Ji Huihui Jia Junji Jia Siyu Jian Cailian Jiang Di Jiang Wei Jiang Xiaoshan Jiang Xiaozhao Jiang Yixuan Jiang Xiaoping Jing Cécile Jollet Li Kang Rebin Karaparabil Narine Kazarian Ali Khan Amina Khatun Khanchai Khosonthongkee Denis Korablev Konstantin Kouzakov Alexey Krasnoperov Sergey Kuleshov Sindhujha Kumaran Nikolay Kutovskiy Loic Labit Tobias Lachenmaier Cecilia Landini Sébastien Leblanc Frederic Lefevre Ruiting Lei Rupert Leitner Jason Leung Demin Li Fei Li Fule Li Gaosong Li Hongjian Li Jiajun Li Min Li Nan Li Qingjiang Li Ruhui Li Rui Li Shanfeng Li Shuo Li Tao Li Teng Li Weidong Li Weiguo Li Xiaomei Li Xiaonan Li Xinglong Li Yi Li Yichen Li Yufeng Li Zhaohan Li Zhibing Li Ziyuan Li Zonghai Li Hao Liang Hao Liang Jiajun Liao Yilin Liao Yuzhong Liao Ayut Limphirat Guey-Lin Lin Shengxin Lin Tao Lin Jiajie Ling Xin Ling Ivano Lippi Caimei Liu Fang Liu Fengcheng Liu Haidong Liu Haotian Liu Hongbang Liu Hongjuan Liu Hongtao Liu Hongyang Liu Jianglai Liu Jiaxi Liu Jinchang Liu Min Liu Qian Liu Qin Liu Runxuan Liu Shenghui Liu Shubin Liu Shulin Liu Xiaowei Liu Xiwen Liu Xuewei Liu Yankai Liu Zhen Liu Lorenzo Loi Alexey Lokhov Paolo Lombardi Claudio Lombardo Kai Loo Chuan Lu Haoqi Lu Jingbin Lu Junguang Lu Meishu Lu Peizhi Lu Shuxiang Lu Bayarto Lubsandorzhiev Sultim Lubsandorzhiev Livia Ludhova Arslan Lukanov Fengjiao Luo Guang Luo Jianyi Luo Shu Luo Wuming Luo Xiaojie Luo Vladimir Lyashuk Bangzheng Ma Bing Ma Qiumei Ma Si Ma Xiaoyan Ma Xubo Ma Jihane Maalmi Jingyu Mai Marco Malabarba Yury Malyshkin Roberto Carlos Mandujano Fabio Mantovani Xin Mao Yajun Mao Stefano M.Mari Filippo Marini Agnese Martini Matthias Mayer Davit Mayilyan Ints Mednieks Yue Meng Anita Meraviglia Anselmo Meregaglia Emanuela Meroni Lino Miramonti Nikhil Mohan Michele Montuschi Axel Müller Massimiliano Nastasi Dmitry V.Naumov Elena Naumova Diana Navas-Nicolas Igor Nemchenok Minh Thuan Nguyen Thi Alexey Nikolaev Feipeng Ning Zhe Ning Hiroshi Nunokawa Lothar Oberauer Juan Pedro Ochoa-Ricoux Alexander Olshevskiy Domizia Orestano Fausto Ortica Rainer Othegraven Alessandro Paoloni George Parker Sergio Parmeggiano Achilleas Patsias Yatian Pei Luca Pelicci Anguo Peng Haiping Peng Yu Peng Zhaoyuan Peng Elisa Percalli Willy Perrin Frédéric Perrot Pierre-Alexandre Petitjean Fabrizio Petrucci Oliver Pilarczyk Luis Felipe Pineres Rico Artyom Popov Pascal PoussotE zio Previtali Fazhi Qi Ming Qi Xiaohui Qi Sen Qian Xiaohui Qian Zhen Qian Hao Qiao Zhonghua Qin Shoukang Qiu Manhao Qu Zhenning Qu Gioacchino Ranucci Reem Rasheed Alessandra Re Abdel Rebii Mariia Redchuk Gioele Reina Bin Ren Jie Ren Yuhan Ren Barbara Ricci Komkrit Rientong Mariam Rifai Mathieu Roche Narongkiat Rodphai Aldo Romani Bedrich Roskovec Xichao Ruan Arseniy Rybnikov Andrey Sadovsky Paolo Saggese Deshan Sandanayake Anut Sangka Giuseppe Sava Utane Sawangwit Michaela Schever Cédric Schwab Konstantin Schweizer Alexandr Selyunin Andrea Serafini Mariangela Settimo Junyu Shao Vladislav Sharov Hexi Shi Jingyan Shi Yanan Shi Vitaly Shutov Andrey Sidorenkov Fedor Simkovic Apeksha Singhal Chiara Sirignano Jaruchit Siripak Monica Sisti Mikhail Smirnov Oleg Smirnov Sergey Sokolov Julanan Songwadhana Boonrucksar Soonthornthum Albert Sotnikov Warintorn Sreethawong Achim Stahl Luca Stanco Konstantin Stankevich Hans Steiger Jochen Steinmann Tobias Sterr Matthias Raphael Stock Virginia Strati Michail Strizh Alexander Studenikin Aoqi SuJun Su Jun Su Shifeng Sun Xilei Sun Yongjie Sun Yongzhao Sun Zhengyang Sun Narumon Suwonjandee Akira Takenaka Xiaohan Tan Jian Tang Jingzhe Tang Qiang Tang Quan Tang Xiao Tang Vidhya Thara Hariharan Alexander Tietzsch Igor Tkachev Tomas Tmej Marco Danilo Claudio Torri Andrea Triossi Riccardo Triozzi Wladyslaw Trzaska Yu-Chen Tung Cristina Tuve Nikita Ushakov Vadim Vedin Carlo Venettacci Giuseppe Verde Maxim Vialkov Benoit Viaud Cornelius Moritz Vollbrecht Katharina von Sturm Vit Vorobel Dmitriy Voronin Lucia Votano Pablo Walker Caishen Wang Chung-Hsiang Wang En Wang Guoli Wang Jian Wang Jun Wang Li Wang Lu Wang Meng Wang Meng Wang Mingyuan Wang Ruiguang Wang Sibo Wang Siguang Wang Wei Wang Wenshuai Wang Xi Wang Xiangyue Wang Yangfu Wang Yaoguang Wang Yi Wang Yi Wang Yifang Wang Yuanqing Wang Yuyi Wang Zhe Wang Zheng Wang Zhimin Wang Apimook Watcharangkool Wei Wei Wei Wei Wenlu Wei Yadong Wei Yuehuan Wei Kaile Wen Liangjian Wen Jun Weng Christopher Wiebusch Rosmarie Wirth Chengxin Wu Diru Wu Qun Wu Yinhui Wu Yiyang Wu Zhi Wu Michael Wurm Jacques Wurtz Christian Wysotzki Yufei Xi Dongmei Xia Shishen Xian Fei Xiao Xiang Xiao Xiaochuan Xie Yijun Xie Yuguang Xie Zhao Xin Zhizhong Xing Benda Xu Cheng Xu Donglian Xu Fanrong Xu Hangkun Xu Jiayang Xu Jilei Xu Jing Xu Jinghuan Xu Meihang Xu Xunjie Xu Yin Xu Yu Xu Baojun Yan Qiyu Yan Taylor Yan Xiongbo Yan Yupeng Yan Changgen Yang Chengfeng Yang Fengfan Yang Jie Yang Lei Yang Pengfei Yang Xiaoyu Yang Yifan Yang Yixiang Yang Zekun Yang Haifeng Yao Jiaxuan Ye Mei Ye Ziping Ye Frédéric Yermia Zhengyun You Boxiang Yu Chiye Yu Chunxu Yu Guojun Yu Hongzhao Yu Miao Yu Xianghui Yu Zeyuan Yu Zezhong Yu Cenxi Yuan Chengzhuo Yuan Ying Yuan Zhenxiong Yuan Baobiao Yue Noman Zafar Kirill Zamogilnyi Vitalii Zavadskyi Fanrui Zeng Shan Zeng Tingxuan Zeng Yuda Zeng Liang Zhan Yonghua Zhan Aiqiang Zhang Bin Zhang Binting Zhang Feiyang Zhang Hangchang Zhang Haosen Zhang Honghao Zhang Jialiang Zhang Jiawen Zhang Jie Zhang Jingbo Zhang Jinnan Zhang Junwei Zhang Lei Zhang Peng Zhang Ping Zhang Qingmin Zhang Shiqi Zhang Shu Zhang Shuihan Zhang Siyuan Zhang Tao Zhang Xiaomei Zhang Xin Zhang Xuantong Zhang Yinhong Zhang Yiyu Zhang Yongpeng Zhang Yu Zhang Yuanyuan Zhang Yumei Zhang Zhenyu Zhang Zhijian Zhang Jie Zhao Rong Zhao Runze Zhao Shujun Zhao Tianhao Zhao Hua Zheng Yangheng Zheng Jing Zhou Li Zhou Nan Zhou Shun Zhou Tong Zhou Xiang Zhou Jingsen Zhu Kangfu Zhu Kejun Zhu Zhihang Zhu Bo Zhuang Honglin Zhuang Liang Zong Jiaheng Zou Jan Züfle The JUNO Collaboration 《Chinese Physics C》 2025年第1期35-59,共25页
This paper presents an energy resolution study of the JUNO experiment,incorporating the latest knowledge acquired during the detector construction phase.The determination of neutrino mass ordering in JUNO requires an ... This paper presents an energy resolution study of the JUNO experiment,incorporating the latest knowledge acquired during the detector construction phase.The determination of neutrino mass ordering in JUNO requires an exceptional energy resolution better than 3% at 1 MeV.To achieve this ambitious goal,significant efforts have been undertaken in the design and production of the key components of the JUNO detector.Various factors affecting the detection of inverse beta decay signals have an impact on the energy resolution,extending beyond the statistical fluctuations of the detected number of photons,such as the properties of the liquid scintillator,performance of photomultiplier tubes,and the energy reconstruction algorithm.To account for these effects,a full JUNO simulation and reconstruction approach is employed.This enables the modeling of all relevant effects and the evaluation of associated inputs to accurately estimate the energy resolution.The results of this study reveal an energy resolution of 2.95% at 1 Mev.Furthermore,this study assesses the contribution of major effects to the overall energy resolution budget.This analysis serves as a reference for interpreting future measurements of energy resolution during JUNO data collection.Moreover,it provides a guideline for comprehending the energy resolution characteristics of liquid scintillator-based detectors. 展开更多
关键词 energy resolution liquid scintillator detector JUNO SIMULATION RECONSTRUCTION
原文传递
上一页 1 下一页 到第
使用帮助 返回顶部