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Experimental extraction of neutron resonance parameters at 20–300 eV for^(147,149)Sm
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作者 Xin-Xiang Li Long-Xiang Liu +29 位作者 Wei Jiang Ya-Ju Chen Jie Ren Hong-Wei Wang Gong-Tao Fan Wen Luo Song Feng Wen Xie Zi-Ang Lin Ting Jiang Gao-Le Yang Zhen-Dong An Xian-Kai Li Zhou-Ji Liao Jie-Ming Xue Xin-Yu Li Ning-Xin Peng De-Xin Wang Su-Ya-La-Tu Zhang Yue Zhang Xin-Rong Hu Zi-Rui Hao Bing Jiang Xiao-He Wang Ji-Feng Hu Ying-Du Liu Chun-Wang Ma Yu-Ting Wang Jian-Jun He Li-Yong Zhang 《Nuclear Science and Techniques》 2025年第10期98-107,共10页
^(147,149)Sm are slow neutron capture(s-process)nuclides in nuclear astrophysics,whose(n,γ)cross sections are important input parameters in nucleosynthesis network calculations in the samarium(Sm)region.In addition,^... ^(147,149)Sm are slow neutron capture(s-process)nuclides in nuclear astrophysics,whose(n,γ)cross sections are important input parameters in nucleosynthesis network calculations in the samarium(Sm)region.In addition,^(149)Sm is a fission product of ^(235)U with a 1%yield,and its neutron resonance parameters play a critical role in reactor neutronics.According to the available nuclear evaluation databases,a significant disagreement has been observed in the resonance peaks of the ^(147,149)Sm(n,γ)crosssectional data within the energy range of 20-300 eV.In this study,tutron capture cross section of a natural samarium target was measured at the back-streaming white neutron beamline of the China Spallation Neutron Source.The neutron capture yield was obtained,and the neutron resonance parameters for ^(147)Sm at 107.0,139.4,241.7,and 257.3 eV and ^(149)Sm at 23.2,24.6,26.1,28.0,51.5,75.2,90.9,125.3,and 248.4 eV were extracted using the SAMMY code based on R-matrix theory.For the parameters Γ_(n) and Γ_(γ) in these energies of ^(147,149)Sm,the percentages consistent with the results of the CENDL-3.2,ENDF/B-Ⅷ.0,JEFF-3.3,JENDL-4.0,and BROND-3.1 database are 27%,65%,65%,42%,and 58%,respectively.However,27% of the results were inconsistent with those of the major libraries.This work enriches experimental data of the ^(147,149)Sm neutron capture resonance and helps clarify the differences between different evaluation databases at the above energies. 展开更多
关键词 Neutron capture cross section Neutron resonance parameters Back-n facility
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Precise measurement of the χ_(c 0) resonance parameters and branching fractions ofχ_(c 0,c 2)→π^(+)π^(−)/K^(+)K^(−)
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作者 M.Ablikim M.N.Achasov +669 位作者 P.Adlarson O.Afedulidis X.C.Ai R.Aliberti A.Amoroso Y.Bai O.Bakina I.Balossino Y.Ban H.-R.Bao V.Batozskaya K.Begzsuren N.Berger M.Berlowski M.Bertani D.Bettoni F.Bianchi E.Bianco A.Bortone I.Boyko R.A.Briere A.Brueggemann H.Cai X.Cai A.Calcaterra G.F.Cao N.Cao S.A.Cetin X.Y.Chai J.F.Chang G.R.Che Y.Z.Che G.Chelkov C.Chen C.H.Chen Chao Chen G.Chen H.S.Chen H.Y.Chen M.L.Chen S.J.Chen S.L.Chen S.M.Chen T.Chen X.R.Chen X.T.Chen Y.B.Chen Y.Q.Chen Z.J.Chen Z.Y.Chen S.K.Choi G.Cibinetto F.Cossio J.J.Cui H.L.Dai J.P.Dai A.Dbeyssi R.E.de Boer D.Dedovich C.Q.Deng Z.Y.Deng A.Denig I.Denisenko M.Destefanis F.De Mori B.Ding X.X.Ding Y.Ding Y.Ding J.Dong L.Y.Dong M.Y.Dong X.Dong M.C.Du S.X.Du Y.Y.Duan Z.H.Duan P.Egorov Y.H.Fan J.Fang J.Fang S.S.Fang W.X.Fang Y.Fang Y.Q.Fang R.Farinelli L.Fava F.Feldbauer G.Felici C.Q.Feng J.H.Feng Y.T.Feng M.Fritsch C.D.Fu J.L.Fu Y.W.Fu H.Gao X.B.Gao Y.N.Gao Yang Gao S.Garbolino I.Garzia L.Ge P.T.Ge Z.W.Ge C.Geng E.M.Gersabeck A.Gilman K.Goetzen L.Gong W.X.Gong W.Gradl S.Gramigna M.Greco M.H.Gu Y.T.Gu C.Y.Guan A.Q.Guo L.B.Guo M.J.Guo R.P.Guo Y.P.Guo A.Guskov J.Gutierrez K.L.Han T.T.Han F.Hanisch X.Q.Hao F.A.Harris K.K.He K.L.He F.H.Heinsius C.H.Heinz Y.K.Heng C.Herold T.Holtmann P.C.Hong G.Y.Hou X.T.Hou Y.R.Hou Z.L.Hou B.Y.Hu H.M.Hu J.F.Hu Q.P.Hu S.L.Hu T.Hu Y.Hu G.S.Huang K.X.Huang L.Q.Huang X.T.Huang Y.P.Huang Y.S.Huang T.Hussain F.Hölzken N.Hüsken N.in der Wiesche J.Jackson S.Janchiv J.H.Jeong Q.Ji Q.P.Ji W.Ji X.B.Ji X.L.Ji Y.Y.Ji X.Q.Jia Z.K.Jia D.Jiang H.B.Jiang P.C.Jiang S.S.Jiang T.J.Jiang X.S.Jiang Y.Jiang J.B.Jiao J.K.Jiao Z.Jiao S.Jin Y.Jin M.Q.Jing X.M.Jing T.Johansson S.Kabana N.Kalantar-Nayestanaki X.L.Kang X.S.Kang M.Kavatsyuk B.C.Ke V.Khachatryan A.Khoukaz R.Kiuchi O.B.Kolcu B.Kopf M.Kuessner X.Kui N.Kumar A.Kupsc W.Kühn L.Lavezzi T.T.Lei Z.H.Lei M.Lellmann T.Lenz C.Li C.Li C.H.Li Cheng Li D.M.Li F.Li G.Li H.B.Li H.J.Li H.N.Li Hui Li J.R.Li J.S.Li K.Li K.L.Li L.J.Li L.K.Li Lei Li M.H.Li P.R.Li Q.M.Li Q.X.Li R.Li S.X.Li T.Li T.Y.Li W.D.Li W.G.Li X.Li X.H.Li X.L.Li X.Y.Li X.Z.Li Y.G.Li Z.J.Li Z.Y.Li C.Liang H.Liang H.Liang Y.F.Liang Y.T.Liang G.R.Liao Y.P.Liao J.Libby A.Limphirat C.C.Lin C.X.Lin D.X.Lin T.Lin B.J.Liu B.X.Liu C.Liu C.X.Liu F.Liu F.H.Liu Feng Liu G.M.Liu H.Liu H.B.Liu H.H.Liu H.M.Liu Huihui Liu J.B.Liu J.Y.Liu K.Liu K.Y.Liu Ke Liu L.Liu L.C.Liu Lu Liu M.H.Liu P.L.Liu Q.Liu S.B.Liu T.Liu W.K.Liu W.M.Liu X.Liu X.Liu Y.Liu Y.Liu Y.B.Liu Z.A.Liu Z.D.Liu Z.Q.Liu X.C.Lou F.X.Lu H.J.Lu J.G.Lu X.L.Lu Y.Lu Y.P.Lu Z.H.Lu C.L.Luo J.R.Luo M.X.Luo T.Luo X.L.Luo X.R.Lyu Y.F.Lyu F.C.Ma H.Ma H.L.Ma J.L.Ma L.L.Ma L.R.Ma M.M.Ma Q.M.Ma R.Q.Ma T.Ma X.T.Ma X.Y.Ma Y.M.Ma F.E.Maas I.MacKay M.Maggiora S.Malde Y.J.Mao Z.P.Mao S.Marcello Z.X.Meng J.G.Messchendorp G.Mezzadri H.Miao T.J.Min R.E.Mitchell X.H.Mo B.Moses N.Yu.Muchnoi J.Muskalla Y.Nefedov F.Nerling L.S.Nie I.B.Nikolaev Z.Ning S.Nisar Q.L.Niu W.D.Niu Y.Niu S.L.Olsen S.L.Olsen Q.Ouyang S.Pacetti X.Pan Y.Pan A.Pathak Y.P.Pei M.Pelizaeus H.P.Peng Y.Y.Peng K.Peters J.L.Ping R.G.Ping S.Plura V.Prasad F.Z.Qi H.Qi H.R.Qi M.Qi T.Y.Qi S.Qian W.B.Qian C.F.Qiao X.K.Qiao J.J.Qin L.Q.Qin L.Y.Qin X.P.Qin X.S.Qin Z.H.Qin J.F.Qiu Z.H.Qu C.F.Redmer K.J.Ren A.Rivetti M.Rolo G.Rong Ch.Rosner M.Q.Ruan S.N.Ruan N.Salone A.Sarantsev Y.Schelhaas K.Schoenning M.Scodeggio K.Y.Shan W.Shan X.Y.Shan Z.J.Shang J.F.Shangguan L.G.Shao M.Shao C.P.Shen H.F.Shen W.H.Shen X.Y.Shen B.A.Shi H.Shi J.L.Shi J.Y.Shi Q.Q.Shi S.Y.Shi X.Shi J.J.Song T.Z.Song W.M.Song Y.J.Song Y.X.Song S.Sosio S.Spataro F.Stieler S.S Su Y.J.Su G.B.Sun G.X.Sun H.Sun H.K.Sun J.F.Sun K.Sun L.Sun S.S.Sun T.Sun W.Y.Sun Y.Sun Y.J.Sun Y.Z.Sun Z.Q.Sun Z.T.Sun C.J.Tang G.Y.Tang J.Tang J.J.Tang Y.A.Tang L.Y.Tao Q.T.Tao M.Tat J.X.Teng V.Thoren W.H.Tian Y.Tian Z.F.Tian I.Uman Y.Wan S.J.Wang B.Wang B.L.Wang Bo Wang D.Y.Wang F.Wang H.J.Wang J.J.Wang J.P.Wang K.Wang L.L.Wang M.Wang N.Y.Wang S.Wang S.Wang T.Wang T.J.Wang W.Wang W.Wang W.P.Wang X.Wang X.F.Wang X.J.Wang X.L.Wang X.N.Wang Y.Wang Y.D.Wang Y.F.Wang Y.H.Wang Y.L.Wang Y.N.Wang Y.Q.Wang Yaqian Wang Yi Wang Z.Wang Z.L.Wang Z.Y.Wang Ziyi Wang D.H.Wei F.Weidner S.P.Wen Y.R.Wen U.Wiedner G.Wilkinson M.Wolke L.Wollenberg C.Wu J.F.Wu L.H.Wu L.J.Wu X.Wu X.H.Wu Y.Wu Y.H.Wu Y.J.Wu Z.Wu L.Xia X.M.Xian B.H.Xiang T.Xiang D.Xiao G.Y.Xiao S.Y.Xiao Y.L.Xiao Z.J.Xiao C.Xie X.H.Xie Y.Xie Y.G.Xie Y.H.Xie Z.P.Xie T.Y.Xing C.F.Xu C.J.Xu G.F.Xu H.Y.Xu M.Xu Q.J.Xu Q.N.Xu W.Xu W.L.Xu X.P.Xu Y.Xu Y.C.Xu Z.S.Xu F.Yan L.Yan W.B.Yan W.C.Yan X.Q.Yan H.J.Yang H.L.Yang H.X.Yang J.H.Yang T.Yang Y.Yang Y.F.Yang Y.F.Yang Y.X.Yang Z.W.Yang Z.P.Yao M.Ye M.H.Ye J.H.Yin Junhao Yin Z.Y.You B.X.Yu C.X.Yu G.Yu J.S.Yu M.C.Yu T.Yu X.D.Yu Y.C.Yu C.Z.Yuan J.Yuan J.Yuan L.Yuan S.C.Yuan Y.Yuan Z.Y.Yuan C.X.Yue A.A.Zafar F.R.Zeng S.H.Zeng X.Zeng Y.Zeng Y.J.Zeng Y.J.Zeng X.Y.Zhai Y.C.Zhai Y.H.Zhan A.Q.Zhang B.L.Zhang B.X.Zhang D.H.Zhang G.Y.Zhang H.Zhang H.Zhang H.C.Zhang H.H.Zhang H.H.Zhang H.Q.Zhang H.R.Zhang H.Y.Zhang J.Zhang J.Zhang J.J.Zhang J.L.Zhang J.Q.Zhang J.S.Zhang J.W.Zhang J.X.Zhang J.Y.Zhang J.Z.Zhang Jianyu Zhang L.M.Zhang Lei Zhang P.Zhang Q.Y.Zhang R.Y.Zhang S.H.Zhang Shulei Zhang X.M.Zhang X.Y Zhang X.Y.Zhang Y.Zhang Y.Zhang Y.T.Zhang Y.H.Zhang Y.M.Zhang Yan Zhang Z.D.Zhang Z.H.Zhang Z.L.Zhang Z.Y.Zhang Z.Y.Zhang Z.Z.Zhang G.Zhao J.Y.Zhao J.Z.Zhao L.Zhao L.Zhao M.G.Zhao N.Zhao R.P.Zhao S.J.Zhao Y.B.Zhao Y.X.Zhao Z.G.Zhao A.Zhemchugov B.Zheng B.M.Zheng J.P.Zheng W.J.Zheng Y.H.Zheng B.Zhong X.Zhong H.Zhou J.Y.Zhou L.P.Zhou S.Zhou X.Zhou X.K.Zhou X.R.Zhou X.Y.Zhou Y.Z.Zhou Z.C.Zhou A.N.Zhu J.Zhu K.Zhu K.J.Zhu K.S.Zhu L.Zhu L.X.Zhu S.H.Zhu T.J.Zhu W.D.Zhu Y.C.Zhu Z.A.Zhu J.H.Zou J.Zu 《Chinese Physics C》 2025年第9期1-11,共11页
By analyzing ψ(3686) data sample containing (107.7±0.6)×10^(6) events taken with the BESIII detector at the BEPCII storage ring in 2009,the χ_(c 0) resonance parameters are precisely measured using χ_(c 0... By analyzing ψ(3686) data sample containing (107.7±0.6)×10^(6) events taken with the BESIII detector at the BEPCII storage ring in 2009,the χ_(c 0) resonance parameters are precisely measured using χ_(c 0,c 2)→π^(+)π^(−)/K^(+)K^(−) events.The mass of χ_(c 0) is determined to be M (χ_(c 0))=(3415.63±0.07±0.07±0.07)MeV/c^(2),and its full width is F (χ_(c 0))=(12.52±0.12±0.13)MeV,where the first uncertainty is statistical,the second systematic,and the third for mass comes from χ_(c 2) mass uncertainty.These measurements improve the precision of χ_(c 0) mass by a factor of four and width by one order of magnitude over the previous individual measurements,and significantly boost our knowledge about the charmonium spectrum.Together with additional (345.4±2.6)×10^(6)(3686) data events taken in 2012,the decay branching fractions of χ_(c 0,c 2)→π^(+)π^(−)/K^(+)K^(−) are measured as well,with precision improved by a factor of three compared to previous measurements.These χ_(c 0) decay branching fractions provide important inputs for the study of glueballs. 展开更多
关键词 χ_(c 0) BESII CHARMONIUM resonance parameter branching fraction
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Measurement of neutron cross sections and resonance parameters of ^(169)Tm below 100 eV
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作者 王文明 李霞 +11 位作者 赵志祥 周祖英 于洪伟 吴海成 魏义祥 T.F. Wang G.N. Kim M.W. Lee K.S. Kim M.H. Cho I.S. Ko W. Namkung 《Chinese Physics C》 SCIE CAS CSCD 2010年第2期177-181,共5页
The neutron total cross-sections of thulium (^169Tm) were measured in the neutron energy region from 0.01 eV to 100 eV by using the time-of-flight method at the Pohang Neutron Facility, which consists of an electron... The neutron total cross-sections of thulium (^169Tm) were measured in the neutron energy region from 0.01 eV to 100 eV by using the time-of-flight method at the Pohang Neutron Facility, which consists of an electron linac, a water-cooled tantalum target with a water moderator, and a 12 m time of flight path, Two thulium plates with different thicknesses were used for the neutron transmission measurement. The background level was determined by using a notch-filter of Co, In, and Cd sheets. The present measurement was compared with the previous ones, and a new set of resonance parameters of ^169Tm isotope was obtained from the transmission rate by using the SAMMY code, with a comparison with the recommended parameters by Mughabghab. 展开更多
关键词 resonance parameters THULIUM n-TOF method SAMMY
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Resonance analysis of^(159)Tb(n,γ)reaction based on the CSNS Back-n experiment 被引量:1
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作者 De-Xin Wang Su-Ya-La-Tu Zhang +14 位作者 Wei Jiang Jie Ren Mei-Rong Huang Jing-Yu Tang Xi-Chao Ruan Hong-Wei Wang Long-Xiang Liu Xue Li Dan-Dan Niu Guo Li Gu-Fu Meng Yong-Shun Huang Zhi-Long Wang Yu Bai Xue Yang 《Nuclear Science and Techniques》 2025年第3期85-94,共10页
The neutron capture resonance parameters for 159Tb are crucial for validating nuclear models,nucleosynthesis during the neutron capture process,and nuclear technology applications.In this study,resonance analyses were... The neutron capture resonance parameters for 159Tb are crucial for validating nuclear models,nucleosynthesis during the neutron capture process,and nuclear technology applications.In this study,resonance analyses were performed for the neutron capture cross sections of 159Tb measured at the China Spallation Neutron Source(CSNS)backscattering white neutron beamline(Back-n)facility.The resonance parameters were extracted from the R-Matrix code SAMMY and fitted to the experimental capture yield up to the 1.2 keV resolved resonance region(RRR).The average resonance parameters were determined by performing statistical analysis on the set of the resonance parameters in the RRR.These results were used to fit the measured average capture cross sections using the FITACS code in the unresolved resonance region from 2 keV to 1 MeV.The contributions of partial waves l=0,1,2 to the average capture cross sections are reported. 展开更多
关键词 Statistical analysis resonance parameters ^(159)Tb(n γ)cross section γ
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Determination of the Earth’s free core nutation parameters by using tidal gravity data 被引量:1
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作者 刘明波 孙和平 +1 位作者 徐建桥 周江存 《Acta Seismologica Sinica(English Edition)》 CSCD 2007年第6期708-711,共4页
The Earth's free core nutation (FCN) is a retrograde eigenrnode which is attributed to the interaction between the solid mantle and the liquid core of the rotational elliptical Earth. This mode appears as an eigenm... The Earth's free core nutation (FCN) is a retrograde eigenrnode which is attributed to the interaction between the solid mantle and the liquid core of the rotational elliptical Earth. This mode appears as an eigenmode of nearly diurnal free wobble (NDFW) in a terrestrial reference frame with a period of about one day (XU et al, 2001). Therefore, the NDFW will lead to an obvious resonance enhancement in the diurnal tidal gravity observations, especially those of the tidal waves with frequencies closed to its eigenfrequency such as P1, K1, ψ1 and Ф1. The FCN resonance parameters can be retrieved accurately by high-precision tidal gravity observations, especially those recorded with the superconducting gravimeters (SG). The Global Geodynamics Project (GGP) organized by IUGG took it as an important content for determining the FCN resonance parameters by using gravity data. However, the results are affected by many factors such as station location, background noise, the selection of the tide-generating potential tables, ocean tide models, data processing techniques and so on. In our study, the FCN parameters will be retrieved by using the SG observations at Wuhan, and the effects of the choices of various tide-generating potential tables, oceanic models and weight functions on the estimation of the FCN parameters will be discussed in detail, 展开更多
关键词 superconducting gravimeter free core nutation resonance parameters
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Three dimensional structure prediction and proton nuclear magnetic resonance analysis of toxic pesticides in human blood plasma 被引量:1
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作者 Amit Kumar Sharma Rajeev Kumar Tiwari Mulayam Singh Gaur 《The Journal of Biomedical Research》 CAS 2012年第3期170-184,共15页
The purpose of this study was to investigate the nuclear magnetic resonance (NMR) assignments of hydrolyzed products extracted from human blood plasma. The correlations between chemical, functional and structural pr... The purpose of this study was to investigate the nuclear magnetic resonance (NMR) assignments of hydrolyzed products extracted from human blood plasma. The correlations between chemical, functional and structural prop- erties of highly toxic pesticides were investigated using the PreADME analysis. We observed that toxic pesticides possessed higher molecular weight and, more hydrogen bond donors and acceptors when compared with less toxic pesticides. The occurrence of functional groups and structural properties was analyzed using ~H-NMR. The ~H- NMR spectra of the phosphomethoxy class of pesticides were characterized by methyl resonances at 3.7-3.9 ppm (8) with the coupling constants of 11-16 Hz (Je-cns). In phosphoethoxy pesticides, the methyl resonance was about 1.4 ppm (8) with the coupling constant of 10 Hz (Je-cH2) and the methylene resonances was 4.2-4.4 ppm (8) with the coupling constant of 0.8 Hz (Jp-cH3), respectively. Our study shows that the values of four parameters such as chemical shift, coupling constant, integration and relaxation time correlated with the concentration of toxic pesticides, and can be used to characterise the proton groups in the molecular structures of toxic pesticides. 展开更多
关键词 ^1H-NMR toxic pesticide nuclear magnetic resonance (NMR) parameter relaxation time computa- tional tool data interpretation
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Determination of the resonant parameters of excited vector strangenia with e^(+)e^(-)→ηФdata
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作者 朱文静 王小龙 《Chinese Physics C》 SCIE CAS CSCD 2023年第11期23-33,共11页
We determine the resonant parameters of the vector statesϕ(1680)andϕ(2170)by performing a combined fit to the e+e−→ηϕcross sections from the threshold to 2.85GeV measured by the BaBar,Belle,BESIII,and CMD-3 experime... We determine the resonant parameters of the vector statesϕ(1680)andϕ(2170)by performing a combined fit to the e+e−→ηϕcross sections from the threshold to 2.85GeV measured by the BaBar,Belle,BESIII,and CMD-3 experiments.The mass(1678_(−3)^(+5)±7)MeV/c^(2) and width(156±5±9)MeV are obtained forϕ(1680),and the mass(2169±5±6)MeV/c^(2) and width(96_(−14)^(+17)±9)MeV are obtained forϕ(2170).The statistical significance ofϕ(2170)is 7.2σ.Depending on the interference betweenϕ(1680),ϕ(2170),and a non-resonantηϕamplitude in the nominal fit,we obtain four solutions andΓe+e−ϕ(1680)⋅B[ϕ(1680)→ηϕ]=(79±4±16),(127±5±12),(65_(−4)^(+5)±13)or(215_(−5)^(+8)±11)eV,andΓ_(ϕ(2170))^(e+e−)⋅B[ϕ(2170)→ηϕ]=(0.56_(−0.02)^(+0.03)±0.07),(0.36_(−0.03)^(+0.05)±0.07),(38±1±5)or(41±2±6)eV.We also search for the production of X(1750)→ηϕ,and the significance is only 2.0σ.We then determine the upper limit ofΓ_(X(1750))^(e+e−)⋅B[X(1750)→ηϕ]at the 90%confidence level. 展开更多
关键词 strangenia resonant parameters Ф(2170) Ф(1680) cross section
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Measurement and analysis of the neutron-induced total cross-sections of 209Bi from 0.3 eV to 20 MeV on the Back-n at CSNS 被引量:2
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作者 薛洁明 冯松 +15 位作者 陈永浩 易晗 李鑫祥 肖敏 程品晶 刘荣 羊奕伟 韩子杰 赵大俊 王豪强 李宝钱 赵继荣 刘梓隽 陈朝敏 罗文 郑波 《Chinese Physics C》 SCIE CAS CSCD 2023年第12期56-63,共8页
The neutron-induced total cross-section of ^(209)Bi is crucial for the physical design and safety assessment of lead-based fast reactors, and the quality of experimental data should be improved for evaluation and appl... The neutron-induced total cross-section of ^(209)Bi is crucial for the physical design and safety assessment of lead-based fast reactors, and the quality of experimental data should be improved for evaluation and application.A recent experiment was conducted on the back-streaming white neutron beamline(Back-n) at the China Spallation Neutron Source(CSNS) using the neutron total cross-section spectrometer(NTOX). The neutron energy was determined using a fast multi-cell fission chamber and the time-of-flight technique. Two high-purity bismuth samples,6 mm and 20 mm in thickness, were chosen for neutron transmission measurements and comparisons. The neutron total cross-sections of ^(209)Bi, ranging from 0.3 e V to 20 Me V, were derived considering neutron flight time determination, flight path calibration, and background subtraction. A comparison of the experimental results with the data in the ENDF/B-VⅢ.0 library showed fair agreement, and the point-wise cross-sections were found to be consistent with existing experimental data. Special attention was given to the determination of resonance parameters, which were analyzed using the R-matrix code SAMMY and Bayesian method in the 0.5 ke V to 20 ke V energy range. The extracted resonance parameters were compared to previously reported results and evaluated data. This study is recognized as the first one where the neutron total cross-section of bismuth across such a broad energy spectrum is measured in a single measurement or experiment, and it provides valuable data for the assessment of related reaction information for evaluated libraries and the advancement of lead-bismuth-based nuclear systems. 展开更多
关键词 Neutron-induced total cross-section BISMUTH Back-n white neutron beamline NTOX neutron resonance parameter
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Study of K*(892) mass and width splitting caused by model difference
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作者 李秀荣 苑长征 《Chinese Physics C》 SCIE CAS CSCD 2009年第5期321-326,共6页
According to the new K^*(892)^0 and K^*(892)^- masses reported by the BELLE experiment and the K^*(892)^0 mass reported by the FOCUS experiment, mass splitting between neutral and charged K^*(892) becomes ... According to the new K^*(892)^0 and K^*(892)^- masses reported by the BELLE experiment and the K^*(892)^0 mass reported by the FOCUS experiment, mass splitting between neutral and charged K^*(892) becomes very small. This is significantly different from the current world average values given by the Particle Data Group 2008. We find that there are differences between models used to fit the K^*(892) decay invariant mass spectra in different measurements and study the model dependence in the measurement of K^*(892) parameters. We refit the K^*(892)^0 mass spectra of the BELLE and FOCUS experiments with the formula used by BELLE in fitting K^*(892)^- to get new mass and width. After refitting, the K^*(892)^0 mass of the BELLE experiment becomes 1.4 MeV/c^2 larger than the initial value and that of the FOCUS experiment is 1 MeV/c^2 smaller than the initial value. We also fit the spectra of some other experiments to extract the K^* (892) parameters using the BELLE K^* (892)^- parametrization. 展开更多
关键词 K^* resonance parameters Breit-Wigner function
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Molecular design and theoretical investigation into one-and two-photon absorption properties of two series of cyclometalated platinum(Ⅱ) complexes
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作者 YANG ZhaoDi ZHANG GuiLing +1 位作者 FENG JiKang REN AiMin 《Science China Chemistry》 SCIE EI CAS 2012年第7期1405-1412,共8页
We have theoretically investigated two series of cyclometalated Pt(II) complexes, a series [Pt (C, N, N) Cl] and b series [Pt (C, N, Npyrazolyl) Cl]. The geometrical and electronic structures are calculated at t... We have theoretically investigated two series of cyclometalated Pt(II) complexes, a series [Pt (C, N, N) Cl] and b series [Pt (C, N, Npyrazolyl) Cl]. The geometrical and electronic structures are calculated at the ECP60MWB//6-31G*(H, C, Cl, N, S) basis set level using DFT method; one-photon absorption (OPA) properties are calculated by using both TDDFT and ZINDO methods and two-photon absorption (TPA) properties are obtained with the ZINDO/SOS method. The resonance integrals parameters (βsp and βd) for Pt are adjusted to -1 and -28.5 eV, respectively, to make max OPA wavelength calculated by ZINDO closest to the experimental data and TDDFT results. The calculated results indicate the molecule 2b ([Pt (Cnaphthyl, N, Npyrazolyl) Cl]) has the biggest potential as outstanding TPA materials because (i) the TPA properties of b series are more outstanding in IR wavelength range, the molecules in b series have good transparencies and possess 1-pyrazolyl-NH that is also available for another metal coordination (e.g., dimerization) and chemical interactions; (ii) when C is CnaphthyI in the C, N, N ligand of cyclometalated Pt(II) complexes, the molecules have the best conjugation effect and the best TPA properties. 展开更多
关键词 cyclometalated Pt (II) complexes ZINDO/SOS method resonance integrals parameters two-photon absorption
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