NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = Cao Yufang Found 13 matches. 2024DA07 Ann.Nucl.Energy 199, 110276 (2024) E.E.Davidson, B.R.Betzler, Y.Cao, T.Fei The importance of delayed neutron precursors in gamma dose calculations for activated primary heat exchanger components in the Molten Salt Breeder Reactor
doi: 10.1016/j.anucene.2023.110276
2023LI64 Nucl.Instrum.Methods Phys.Res. A1057, 168780 (2023) G.Li, S.Chen, Sh.Jia, Zh.Lu, J.Cai, S.Jiang, Y.Cao, P.Sun, H.Xu, J.Fan, J.Li, S.Jing Prediction of explosives by a de-broadening model based on RBF neural network NUCLEAR REACTIONS C, N, O(n, n'), E not given; analyzed available data; deduced identification in previous explosives identification researches by choosing the inelastic scattering peaks. The radial basis function network (RBF network).
doi: 10.1016/j.nima.2023.168780
2023WA22 Chin.Phys.C 47, 084001 (2023) C.-J.Wang, G.Guo, H.J.Ong, Y.-N.Song, B.-H.Sun, I.Tanihata, S.Terashima, X.-L.Wei, J.-Y.Xu, X.-D.Xu, J.-C.Zhang, Yo.Zheng, L.-H.Zhu, Y.Cao, G.-W.Fan, B.-S.Gao, J.-X.Han, G.-S.Li, C.-G.Lu, H.-T.Qi, Y.Qin, Z.-Y.Sun, L.-P.Wan, K.-L.Wang, S.-T.Wang, X.-X.Wang, M.-X.Zhang, W.-W.Zhang, X.-B.Zhang, X.-H.Zhang, Z.-C.Zhou Charge-changing cross section measurements of 300 MeV/nucleon 28Si on carbon and data analysis NUCLEAR REACTIONS C(28Si, X), E=304 MeV/nucleon; measured reaction products; deduced σ. Comparison with available data. The second Radioactive Ion Beam Line in Lanzhou (RIBLL2).
doi: 10.1088/1674-1137/acd366
2022CA06 Phys.Rev. C 105, 034304 (2022) Uncertainty analysis for the nuclear liquid drop model and implications for the symmetry energy coefficients ATOMIC MASSES 200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315U; calculated binding energies using liquid drop model (LD), including Wigner energy term, and associated statistical uncertainties using Monte Carlo bootstrap approach based on nonparametric sampling. Comparison with available experimental evaluated masses from AME2020.
doi: 10.1103/PhysRevC.105.034304
2020CA18 Phys.Rev. C 102, 024311 (2020) Y.Cao, S.E.Agbemava, A.V.Afanasjev, W.Nazarewicz, E.Olsen Landscape of pear-shaped even-even nuclei NUCLEAR STRUCTURE Z=40-100, N=40-200; calculated ground state octupole deformations β3 and octupole deformation energies of even-even nuclei in the (Z, N) plane using the Skyrme energy density functionals (SEDFs): UNEDF0, UNEDF1, UNEDF2, SLy4, and SV-min. 80Zr, 112,146Ba, 224Ra, 286Th; calculated Single-particle energy splitting between the unusual-parity intruder shell and the normal-parity shell using (SEDFs): UNEDF0, UNEDF1, UNEDF2, SLy4, SV-min, DD-ME2, NL3*, DD-PC1 and PC-PK1. 212,214,216,218,220,222,224,226,228,230Rn, 214,216,218,220,222,224,226,228,230,232Ra, 216,218,220,222,224,226,228,230,232,234Th, 216,218,220,222,224,226,228,230,232,234U, 138,140,142,144,146,148,150,152Ba, 140,142,144,146,148,150,152,154Ce, 142,144,146,148,150,152,154,156Nd; calculated deformation parameters β2, β3, and octupole deformation energies using the Skyrme energy density functionals models. 112,114,144,146,148Ba, 144,146,148Ce, 146,148,196,198Nd, 150,194,196,198Sm, 196,198,200Gd, 198,200,202Dy, 200,202Er, 218,220,222,224,278,280,282Rn, 218,220,222,224,226,228,280,282,284,286,288Ra, 220,222,224,226,228,282,284,286,288,290Th, 222,224,226,228,230,282,284,286,288,290U, 224,226,228,230,232,284,286,288,290,292Pu, 224,226,228,230,284,286,288,290,292,294Cm, 226,228,230,284,286,288,290,292,294,296Cf, 226,228,230,232,284,286,288,290,292,294,296,298Fm, 230,286,288,290,292,294,296,298No, 288,290,292,294,296,300Rf, 290,292,294Sg; calculated β3 deformation parameter, octupole deformation energies, proton moments Q20 and Q30 for octupole-deformed nuclei obtained in five Skyrme energy density functionals, and four covariant energy density functionals. Comparison between Skyrme and covariant models, and with relevant experimental data. See also supplemental material.
doi: 10.1103/PhysRevC.102.024311
2020HE15 Phys.Rev. C 102, 014322 (2020) Effects of high-j orbitals, pairing, and deformed neutron shells on upbendings of ground-state bands in the neutron-rich even-even isotopes 170-184Hf NUCLEAR STRUCTURE 170,172,174,176,178,180,182,184Hf; calculated neutron and proton levels with Nilsson configurations near the Fermi surface, levels, J, π, neutron and proton occupation probabilities, contribution from the neutron shells to the angular momentum alignment in the ground state bands, neutron kinematic moment of inertia with and without pairing. Cranked shell model with pairing correlations treated by the particle-number conserving method. Comparison with experimental data.
doi: 10.1103/PhysRevC.102.014322
2020NE02 Phys.Rev. C 101, 014319 (2020) L.Neufcourt, Y.Cao, S.Giuliani, W.Nazarewicz, E.Olsen, O.B.Tarasov Beyond the proton drip line: Bayesian analysis of proton-emitting nuclei RADIOACTIVITY 19Mg, 45Fe, 48Ni, 54Zn, 67Kr(2p); calculated Q(2p) using eleven global mass models: Skyrme models SkM*, SkP, SLy4, SV-min, UNEDF0, UNEDF1, UNEDF2, BCPM and D1M, FRDM-2012 and HFB-24, and Bayesian model averaging (BMA) results: BMA-0, BMA-I, BMA-II, BMA-III, and comparing with experimental data from AME2016 and later literature. Z=17-82; calculated nuclear binding-energy, and probability of proton decay, relative to the neutron number of the lightest proton-bound isotope with known experimental S(p) or S(2p), in the proton-rich region using BMA-I and BMA-II model averaging methods. 25,26,27S, 29,30,31Ar, 33,34,35Ca, 37,38,39Ti, 40,41,42,43Cr, 44,45,46Fe, 47,48,49,50Ni, 52,53,54,55Zn, 56,57,58,59Ge, 61,62,63,64Se, 64,65,66,67,68Kr, 68,69,70,71,72Sr, 72,73,74,75,76Zr, 76,77,78,79,80Mo, 80,81,82,83,84Ru, 83,84,85,86,87,88Pd, 87,88,89,90,91Cd, 91,92,93,94,95Sn, 100,101,102,103Te, 104,105,106,107Xe, 108,109,110,111,112Ba, 111,112,113,114,115,116Ce, 115,116,117,118,119Nd, 119,120,121,122,123,124Sm, 123,124,125,126,127,128,129Gd, 128,129,130,131,132,133,134Dy, 131,132,133,134,135,136,137Er, 135,136,137,138,139,140,141,142Yb, 141,142,143,144,145,146,147Hf, 145,146,147,148,149,150W, 150,151,152,153,154,155Os, 152,153,154,155,156,157,158Pt, 156,157,158,159,160,161,162Hg(2p); calculated Q(2p) and half-lives using BMA-1 method. 30Ar, 34Ca, 39Ti, 42Cr, 58Ge, 62Se, 66Kr, 70Sr, 74Zr, 78Mo, 82Ru, 86Pd, 90Cd, 103Te; predicted as most promising 2p emitters. 131,132Dy, 134,135Er, 144,145Hf; predicted as excellent candidates for the sequential emission of two protons. Bayesian Gaussian processes for separation-energy residuals and combined via Bayesian model averaging for mass predictions, with uncertainty quantification of theoretical predictions.
doi: 10.1103/PhysRevC.101.014319
2020NE04 Phys.Rev. C 101, 044307 (2020) L.Neufcourt, Y.Cao, S.A.Giuliani, W.Nazarewicz, E.Olsen, O.B.Tarasov Quantified limits of the nuclear landscape NUCLEAR STRUCTURE Z=5-119, N=11-293; calculated S(n) for odd-N. Z=8-119, N=20-296; calculated S(2n) for even-N. Z=25-119, N-21-176; calculated S(p) for odd-Z. Z=14-118, N=8-170; calculated S(2p) for even-Z. Quantified predictions of proton and neutron separation energies and Bayesian probabilities of existence of particle-bound isotopes throughout the nuclear landscape using nuclear density-functional theory with several energy density functionals, together with current global mass models and experimental atomic mass data in the general framework of Bayesian model averaging (BMA); deduced existence of 7759 particle-bound nuclei with Z<120, having existence probability of >0.5. Relevance to discovery potential with modern radioactive ion-beam facilities, such as FRIB at MSU.
doi: 10.1103/PhysRevC.101.044307
2019NE02 Phys.Rev.Lett. 122, 062502 (2019) L.Neufcourt, Y.Cao, W.Nazarewicz, E.Olsen, F.Viens Neutron Drip Line in the Ca Region from Bayesian Model Averaging NUCLEAR STRUCTURE 50,51,52,53,54,55,56,57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72,73,74,75,76,77,78,79,80,81,82Ca, 52Cl, 53Ar, 49S; calculated one- and two-neutron separation energies, posterior probability of existence of neutron-rich nuclei in the Ca region.
doi: 10.1103/PhysRevLett.122.062502
2018NE08 Phys.Rev. C 98, 034318 (2018) L.Neufcourt, Yu.Cao, W.Nazarewicz, F.Viens Bayesian approach to model-based extrapolation of nuclear observables ATOMIC MASSES Z=2-110, N=4-160; analyzed S(2n) of even-even nuclei from AME-2003 and AME-2016 evaluations, JYFLTRAP experimental data, and various global mass models; calculated S(2n), residuals of S(2n) for six global mass models, and S(2n) credibility interval to extrapolated nuclei with the chain of Sn nuclei as a representative example using Bayesian Gaussian processes and neural networks.
doi: 10.1103/PhysRevC.98.034318
2009LI34 Nucl.Technology 168, 391 (2009) Monte Carlo Application in Shielding Design for an X-Ray Container/Vehicle Inspection System
doi: 10.13182/NT09-A9215
1999LI56 High Energy Phys. and Nucl.Phys. (China) 23, 320 (1999) Y.Li, J.Gu, X.Yu, J.Liu, Y.Cao, J.Zeng, W.Li, S.Shi Study of the Low Excited States of 72Ge
1988PA08 Chin.J.Nucl.Phys. 10, 178 (1988) Pan Feng, Pan Zhenyong, Cao Yufang U (6/10) Supersymmetry in Zn Isotopes NUCLEAR STRUCTURE 63,64Zn; calculated levels, B(E2), one-nucleon transfer intensities; deduced supersymmetry multiplets.
Back to query form |