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NSR database version of April 25, 2024.

Search: Author = C.Guo

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2024LI17      Phys.Rev. C 109, 034310 (2024)

C.B.Li, Y.Zheng, T.X.Li, X.G.Wu, H.Y.Wu, M.Zheng, Z.H.Zhao, Y.Q.Li, R.Hong, Z.Y.He, J.Z.Li, J.L.Wang, C.Y.Guo, Z.X.Zhou, L.Ni, G.S.Li, X.H.Zhou, B.Guo, S.Y.Wang, M.L.Liu, Y.H.Zhang, C.Y.He, F.L.Liu, S.Wang, L.H.Zhu

Lifetime measurements of the first 2⁺ states in ^{116, 118}Te

doi: 10.1103/PhysRevC.109.034310
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2023AN14      Sci. Rep. 13, 12657 (2023)

Z.An, W.Qiu, W.Jiang, G.Yang, X.Li, Z.Liao, Z.Zhuang, X.Zhang, S.Chen, C.Guo, E.Xiao, X.Fang, X.Li, H.Wang, X.Hu, Bi.Jiang, W.Shen, J.Wang, J.Ren, X.Ruan, D.Wang, S.-Y.Zhang, W.Luo, Z.Zhu, H.Lan, Z.Cao, X.Ma, Y.Liu, P.Wang, Y.Yang, P.Su, X.Deng, W.He, Y.Ma, C.Ma, Y.Wang, P.He, R.Tang, T.Zhou, J.Wang, H.Yi, Y.Zhang, Y.Chen, R.Fan, K.Gao, Q.Li, K.Sun, Z.Tan, M.Gu, H.Jing, J.Tang

Measurement of the ¹⁸¹Ta(n, γ) cross sections up to stellar s-process temperatures at the CSNS Back-n

NUCLEAR REACTIONS ¹⁸¹Ta(n, γ), E=0.001-800 keV; measured reaction products, En, In, TOF; deduced σ, resonance parameters using the R-Matrix code SAMMY, Maxwellian average cross sections (MACS). Comparison with available data. The back-streaming white neutron facility (Back-n) of China spallation neutron source (CSNS).

doi: 10.1038/s41598-023-39603-7
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2023DU05      Eur.Phys.J. A 59, 93 (2023)

H.-X.Duan, F.Zhang, J.Su, L.Zhu, C.-C.Guo

Studying sub-saturation density symmetry energy with different nuclear thermometers

NUCLEAR REACTIONS U(¹⁵⁵Gd, X), E not given; ¹⁹⁷Au(¹⁹⁷Au, X), E=35 MeV/nucleon; analyzed available data; deduced the relation between nuclear temperatures and symmetry energy using the IQMD model.

doi: 10.1140/epja/s10050-023-01008-5
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2023GU09      Phys.Rev. A 107, 033116 (2023)

C.Guo, V.Cambier, J.Calvert, M.Favier, M.Andia, L.de Sarlo, S.Bize

Exploiting the two-dimensional magneto-optical trapping of ¹⁹⁹Hg for a mercury optical lattice clock

ATOMIC PHYSICS ¹⁹⁹Hg; measured frequencies; deduced two-dimensional magneto-optical trapping (2D-MOT).

doi: 10.1103/PhysRevA.107.033116
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2023LI05      Phys.Rev. C 107, 014307 (2023)

J.Lin, Y.K.Wang, C.Xu, Z.H.Li, H.Hua, S.Q.Zhang, D.W.Luo, H.Y.Wu, J.Meng, X.G.Wu, Y.Zheng, C.B.Li, T.X.Li, Z.Y.Huang, H.Cheng, C.Y.Guo, Z.X.Zhou, Z.Q.Chen, C.G.Wang

Possible coexistence of magnetic and antimagnetic rotations in ⁶¹Ni

NUCLEAR REACTIONS ⁵⁴Cr(¹¹B, 4n)⁶¹Ni, E=54 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ). ⁶¹Ni; deduced levels, J, π, asymmetric angular distributions from oriented states (ADO), dipole and quadrupole bands structures, configurations, high-spin states. Study provides evidence for possible coexistence of magnetic and antimagnetic rotations in the region around A=60. Comparison with calculations using the microscopic tilted axis cranking covariant density functional theory (TAC-CDFT). Detector array consisted of 6 HPGe with BGO anti-Compton suppressors, 1 clover HPGe detector 2 planar HPGe detectors at HI-13 Tandem Accelerator of the China Institute of Atomic Energy (CIAE).

doi: 10.1103/PhysRevC.107.014307
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2022HU09      Phys.Lett. B 833, 137345 (2022)

H.Huang, W.Q.Zhang, A.N.Andreyev, Z.Liu, D.Seweryniak, Z.H.Li, C.Y.Guo, A.E.Barzakh, P.Van Duppen, B.Andel, S.Antalic, M.Block, A.Bronis, M.P.Carpenter, P.Copp, J.G.Cubiss, B.Ding, D.T.Doherty, Z.Favier, F.Giacoppo, T.H.Huang, B.Kindler, F.G.Kondev, T.Lauritsen, J.G.Li, G.S.Li, B.Lommel, H.Y.Lu, M.Al Monthery, P.Mosat, Y.F.Niu, C.Raison, W.Reviol, G.Savard, S.Stolze, G.L.Wilson, H.Y.Wu, Z.H.Wang, F.R.Xu, Q.B.Zeng, X.H.Yu, F.F.Zeng, X.H.Zhou

First observation of the decay of the 13/2⁺ isomer in ¹⁸³Hg and B(M2) systematics of neutron transitions across the nuclear chart

RADIOACTIVITY ¹⁸³Hg(α) [from ¹⁸⁷Pb α decay]; ^187mPb(α) [from ¹⁴²Nd(⁵⁰Cr, 3n2pγ), E=255 MeV, followed by separation of fragments using Argonne gas-filled analyzer (AGFA) at the ATLAS-ANL facility]; measured reaction products, evaporation residues (EVRs), Eα, Iα, (EVR)α-correlations, αγ(t), Eγ, Iγ, x rays, T_1/2 using double-sided silicon strip detector (DSSD), and four HPGe clover detectors. ^183,183mHg; deduced levels, isomer, J, π, T_1/2 of g.s. and isomer, α branching ratio, K-conversion coefficient, multipolarity, B(M2), Nilsson configurations. ^187mPb; deduced T_1/2. Systematics of decay schemes of 13/2+ isomers in ^{175,177,179,181,183,185}Hg. Systematics of B(M2) values for 7/2-, 9/2+, 11/2- and 13/2+ isomers in even-Z, odd-N nuclei: ²⁵Mg, ³³Si, ^33,35S, ³⁷Ar, ³⁹Ca, ⁵⁹Cr, ⁶¹Fe, ^63,67Ni, ^63,65,67Zn, ^67,69,71Ge, ^69,71Se, ^97,99Mo, ^99,101,103Ru, ^103,105Pd, ^107,109Cd, ^{109,111,113,115}Sn, ¹⁵³Yb, ¹⁶¹Hf, ¹⁶³W, ¹⁶³Os, ^171,189,191Pt, ^{181,183,201,203,205}Hg, ²⁰⁹Pb, ^205,207,211Po, ^207,209,213Rn, ^209,211Ra, ^211,213Th.

doi: 10.1016/j.physletb.2022.137345
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2022ZH22      Phys.Lett. B 829, 137129 (2022)

W.Q.Zhang, A.N.Andreyev, Z.Liu, D.Seweryniak, H.Huang, Z.H.Li, J.G.Li, C.Y.Guo, D.T.Doherty, A.E.Barzakh, P.Van Duppen, J.G.Cubiss, B.Andel, S.Antalic, M.Block, A.Bronis, M.P.Carpenter, P.Copp, B.Ding, Z.Favier, F.Giacoppo, T.H.Huang, X.H.Yu, B.Kindler, F.G.Kondev, T.Lauritsen, G.S.Li, B.Lommel, H.Y.Lu, M.Al Monthery, P.Mosat, Y.F.Niu, C.Raison, W.Reviol, G.Savard, S.Stolze, G.L.Wilson, H.Y.Wu, Z.H.Wang, F.R.Xu, Q.B.Zeng, X.H.Zhou

First observation of a shape isomer and a low-lying strongly-coupled prolate band in neutron-deficient semi-magic ¹⁸⁷Pb

NUCLEAR REACTIONS ¹⁴²Nd(⁵⁰Cr, 3n2p)¹⁸⁷Pb, E=255 MeV beam from ATLAS-ANL facility, followed by separation of evaporation residues (EVRs) using Argonne Gas-Filled Analyzer; measured Eα, Eγ, Iγ, x rays, αγ-coin, γγ-coin, T_1/2 of a new low-energy microsec-isomer by αγ(t) using Gammasphere for γ detection and double-sided silicon strip detector (DSSD) for EVRs and α particles. Recoil-decay tagging (RDT) and isomer-decay tagging (IDT) methods. ¹⁸⁷Pb; deduced high-spin levels, J, π, isomer, K-conversion coefficient, multipolarity, bands, B(E2), B(M1)/B(E2), triple-shape coexistence at low energy. Comparison with band structure in ¹⁸⁵Hg. Systematics of aligned angular momenta plots and experimental Routhians for bands in ^183,185Hg, ¹⁸⁷Pb. ¹⁸⁴Hg, ¹⁸⁶Pb, ¹⁸⁷Tl; observed γ rays. ^186,187m,188Pb; observed α-decay peaks.

doi: 10.1016/j.physletb.2022.137129
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2022ZH46      Phys.Rev. C 106, 024317 (2022)

W.Q.Zhang, A.N.Andreyev, Z.Liu, D.Seweryniak, H.Huang, Z.H.Li, J.G.Li, C.Y.Guo, A.E.Barzakh, P.Van Duppen, M.Al Monthery, B.Andel, S.Antalic, M.Block, A.Bronis, M.P.Carpenter, P.Copp, J.G.Cubiss, B.Ding, D.T.Doherty, Z.Favier, F.Giacoppo, T.H.Huang, B.Kindler, F.G.Kondev, T.Lauritsen, G.S.Li, B.Lommel, H.Y.Lu, P.Mosat, Y.F.Niu, C.Raison, W.Reviol, G.Savard, S.Stolze, G.L.Wilson, H.Y.Wu, Z.H.Wang, F.R.Xu, X.H.Yu, Q.B.Zeng, X.H.Zhou

Identification of excited states in ¹⁸⁸Bi and ¹⁸⁸Po

NUCLEAR REACTIONS ¹⁴²Nd(⁵⁰Cr, 3np)¹⁸⁸Bi, (⁵⁰Cr, 4n)¹⁸⁸Po, E=255 MeV; measured evaporation residues (EVRs), Eα, Eγ, Iγ, x rays, (EVR)γ-coin, αγ-coin, γγ-coin, using four clover HPGe detectors, Gammasphere array with 64 Compton-suppressed HPGe detectors, and DSSD and DSSD+Sibox at the ATLAS-ANL accelerator facility. ^{186,187,187m,188}Pb, ^189,189mBi; deduced recoil-decay tagging (RDT) γ-ray yields. ¹⁸⁸Bi; deduced levels, J, π, isomer, T_1/2 and decay modes of isomer, K-conversion coefficients, multipolarities, configurations. ¹⁸⁸Po; deduced energy of the first 2+ level. ¹⁸⁶Pb; deduced levels, J, π. ^183,184,186Hg, ^{186,187,187m,188}Pb, ^188,189,189mBi; observed Eα. Systematics of 9/2-, 1/2+, 7/2- and 13/2+ level energies in ^{185,187,189,191,193,195}Bi, and those of first 2+, 4+, 6+ and 8+, second 0+, 2+ and 4+ in ^{188,190,192,194,196,198,200,202,204,206,208,210}Po.

doi: 10.1103/PhysRevC.106.024317
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2020SU12      Phys.Rev. C 101, 044606 (2020)

J.Su, L.Zhu, C.Guo

Constraints on the effective mass splitting by the isoscalar giant quadrupole resonance

NUCLEAR STRUCTURE ⁴⁰Ca, ⁹⁰Zr, ²⁰⁸Pb; calculated correlation between the square of the excitation energies of isoscalar giant quadrupole resonances (ISGQRs) and the reciprocal of the weighted effective masses using the microscopic Langevin equation with particle density and kinetic-energy density from the Thomas-Fermi (TF) approach and the Hartree-Fock-Bogolyubov (SHFB) model. Comparison with experimental data. A=30-240; compiled experimental excitation energies of the ISGQRs as a function of mass number, and compared with several theoretical calculations.

doi: 10.1103/PhysRevC.101.044606
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2020SU18      Chin.Phys.C 44, 084106 (2020)

J.Su, L.Zhu, C.Guo, F.-S.Zhang

Isospin dependence of projectile fragmentation at hundreds of MeV/u

NUCLEAR REACTIONS ¹²⁰Sn(¹²⁴Sn, X), (¹⁰⁷Sn, X), E=600 MeV/nucleon; ²⁰⁸Pb(¹³⁶Xe, X), (¹²⁴Xe, X), E=1000 MeV/nucleon; analyzed available data; deduced isospin observables, neutron-to-proton ratios of the light particles emitted from the fragmenting. Isospin-dependent quantum molecular dynamics (IQMD) model and permitting only evaporation in the statistical model GEMINI, the IQMD+GEMINI model.

doi: 10.1088/1674-1137/44/8/084106
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2020ZH22      Int.J.Mod.Phys. E29, 2030004 (2020)

L.Zhu, C.Li, C.-C.Guo, J.Su, P.W.Wen, G.Zhang, F.-S.Zhang

Theoretical progress on production of isotopes in the multinucleon transfer process

NUCLEAR REACTIONS ²³⁸U(⁶⁴Ni, X), E(cm)=307.5 MeV; ²⁰⁸Pb(¹²⁴Xe, X), E(cm)=50 MeV; ¹⁸⁶W(¹⁶⁰Gd, X), E=503 MeV; calculated transfer σ for production of neutron-rich transuranium nuclei.

doi: 10.1142/S0218301320300040
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2019GU08      Phys.Rev. C 99, 044607 (2019)

C.-C.Guo, Y.-G.Ma, Z.-D.An, B.-S.Huang

Influence of α-clustering configurations in ¹⁶O + ¹⁹⁷Au collisions at Fermi energy

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁶O, X), E=40 MeV/nucleon; calculated contour plots of nucleon density, directed flow and flow parameters of free protons as function of rapidity with the chain and a tetrahedron α configurations of ¹⁶O projectile, and transverse momentum dependence of flow parameters. ¹⁹⁷Au(¹²C, X), (¹⁴N, X), (³⁶Ar, X), E=30, 35, 40 MeV/nucleon; calculated charge multiplicity distributions. Extended quantum molecular dynamics model (ImQMD). Comparison with available experimental data. Relevance to α-clustering configurations in light nuclei.

doi: 10.1103/PhysRevC.99.044607
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2019SU17      Phys.Rev. C 100, 014602 (2019)

J.Su, L.Zhu, C.Guo, Z.Zhang

Uniform description of breakup mechanisms in central collision, projectile fragmentation, and proton-induced spallation

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E=35 MeV/nucleon; ⁶³Cu(¹⁹⁷Au, X), E=600 MeV/nucleon; ¹²C(¹⁹⁷Au, X), E=1000 MeV/nucleon; ¹H(⁵⁶Fe, X), E=1000 MeV/nucleon; calculated charge distribution of fragments, multiplicity of intermediate mass fragments with Z=3-30, first and second fragment asymmetries versus the analogous bound charge. ⁴⁸Ti(⁴⁸Ti, X), E=30 MeV/nucleon; ¹²⁰Sn(¹²⁰Sn, X), E=600 MeV/nucleon; ¹H(⁹⁰Zr, X), E=2000 MeV/nucleon; calculated energy-density trajectories of the projectile centers, and fragment mass-excitation, correlations between the intermediate mass fragment (IMF) multiplicity and the total bound charge of the productions in the central collision, projectile fragmentation, and proton-induced spallation. Isospin-dependent quantum molecular dynamics (IQMD) model for breakup mechanisms in central collision, with the evaporations of light particles from the prefragments described by the statistical code GEMINI. Comparison with experimental data.

doi: 10.1103/PhysRevC.100.014602
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2019ZH13      Phys.Lett. B 791, 20 (2019)

L.Zhu, C.Li, J.Su, C.-C.Guo, W.Hua

Advantages of the multinucleon transfer reactions based on ²³⁸U target for producing neutron-rich isotopes around N=126

NUCLEAR REACTIONS ²³⁸U(¹⁸⁶W, X), (¹⁶⁰Gd, X), E(cm)=660, 475 MeV; analyzed available data; deduced mechanism of multinucleon transfer (MNT) reactions for producing neutron-rich heavy nuclei around N=126 using dinuclear system (DNS) model and isospin-dependent quantum molecular dynamics (IQMD) model.

doi: 10.1016/j.physletb.2019.02.015
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2018GU10      Phys.Rev. C 98, 024914 (2018)

Ch.-Q.Guo, H.Liu, J.Xu

Directed flow in an extended multiphase transport model

doi: 10.1103/PhysRevC.98.024914
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2018LI23      Phys.Rev. C 97, 044620 (2018)

P.Li, Y.Wang, Q.Li, C.Guo, H.Zhang

Effects of the in-medium nucleon-nucleon cross section on collective flow and nuclear stopping in heavy-ion collisions in the Fermi-energy domain

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X)E=40-150 MeV/nucleon; calculated directed and elliptic flows of free protons at midrapidity and at the nuclear stopping, yield distributions of free protons as functions of reduced longitudinal and transverse rapidities. Ultrarelativistic quantum molecular dynamics (UrQMD) calculations with medium correction factors and FU3FPI parametrization. Comparison with FOPI and INDRA experimental results.

doi: 10.1103/PhysRevC.97.044620
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2018LI33      Phys.Rev. C 98, 014618 (2018)

F.Li, L.Zhu, Z.-H.Wu, X.-B.Yu, J.Su, C.-C.Guo

Predictions for the synthesis of superheavy elements Z=119 and 120

NUCLEAR REACTIONS ²³⁸U, ^242,244Pu, ²⁴³Am, ^245,248Cm, ²⁴⁹Bk, ²⁴⁹Cf(⁴⁸Ca, 3n), (⁴⁸Ca, 4n), (⁴⁸Ca, 5n), E^*=25-60 MeV; calculated evaporation residue σ(E), and compared with available experimental data. ²⁵²Es(⁴⁰Ca, 3n), E(cm)=204.08 MeV; ²⁵²Es(⁴²Ca, 3n), E(cm)=203.00 MeV; ²⁴⁹Cf(⁴⁵Sc, 3n), E(cm)=211.09 MeV; ²⁵⁵Es(⁴⁰Ca, 4n), E(cm)=207.02 MeV; ²⁵⁴Es(⁴⁰Ca, 3n), E(cm)=203.60 MeV; ²⁴⁷Bk(⁴⁷Ti, 3n), E(cm)=219.19 MeV; ²⁴⁸Bk(⁴⁶Ti, 3n), E(cm)=217.76 MeV; ²⁴²Cm(⁵¹V, 2n), E(cm)=225.86 MeV; ²⁴⁸Cf(⁴⁵Sc, 2n), E(cm)=209.29 MeV; ²⁴¹Am(⁵²Cr, 2n), E(cm)=231.94 MeV; ²⁵²Es(⁴⁴Ca, 3n), E(cm)=204.27 MeV; ²⁵³Es(⁴³Ca, 3n), E(cm)=202.49 MeV; ²⁵⁴Es(⁴²Ca, 3n), E(cm)=201.65 MeV; ²⁵¹Cf(⁴⁵Sc, 3n), E(cm)=210.03 MeV; ²⁴⁹Bk(⁴⁷Ti, 3n), E(cm)=217.18 MeV; ²⁴⁸Bk(⁴⁸Ti, 3n), E(cm)=219.47 MeV; ²⁴⁵Cm(⁵¹V, 3n), E(cm)=229.29 MeV; ²⁴⁷Bk(⁴⁹Ti, 3n), E(cm)=222.17 MeV; ²⁴⁶Cm(⁵⁰V, 3n), E(cm)=225.70 MeV; ²⁴⁴Cm(⁵¹V, 2n), E(cm)=224.00 MeV; ²⁵⁵Es(⁴²Ca, 4n), E(cm)=205.95 MeV; ²⁴³Am(⁵³Cr, 3n), E(cm)=236.20 MeV; ²⁵⁴Es(⁴³Ca, 4n), E(cm)=206.90 MeV; ²⁵³Es(⁴⁴Ca, 4n), E(cm)=210.94 MeV; ²⁴³Am(⁵²Cr, 2n), E(cm)=229.49 MeV; ²⁵⁴Es(⁴⁴Ca, 3n), E(cm)=201.64 MeV; ²⁵⁵Es(⁴³Ca, 3n), E(cm)=201.49 MeV; ²⁵⁵Es(⁴⁴Ca, 4n), E(cm)=207.59 MeV; ²⁵²Es(⁴⁶Ca, 3n), E(cm)=206.00 MeV; ²⁴⁸Bk(⁵⁰Ti, 3n), E(cm)=222.48 MeV; ²⁴⁷Cm(⁵¹V, 3n), E(cm)=226.83 MeV; ²⁵⁴Cf(⁴⁵Sc, 4n), E(cm)=211.93 MeV; ²⁴⁹Bk(⁴⁹Ti, 3n), E(cm)=218.88 MeV; ²⁵⁴Es(⁴⁶Ca, 3n), E(cm)=203.64 MeV; ²⁵⁵Es(⁴⁶Ca, 4n), E(cm)=210.13 MeV; ²⁵²Es(⁴⁸Ca, 3n), E(cm)=208.42 MeV; ²⁵⁵Es(⁴⁶Ca, 3n), E(cm)=204.13; ²⁵⁴Es(⁴⁸Ca, 3n), E(cm)=205.96 MeV; ²⁵⁵Es(⁴⁸Ca, 4n), E(cm)=212.72 MeV; ²⁴²Cm(⁵⁰Cr, 2n), E(cm)=234.22 MeV; ²⁴⁹Cf(⁴⁶Ti, 3n), E(cm)=222.89 MeV; ²⁴⁸Cf(⁴⁶Ti, 2n), E(cm)=219.12 MeV; ²⁵⁷Fm(⁴⁰Ca, 5n), E(cm)=222.66 MeV; ²⁵⁷Fm(⁴⁰Ca, 4n), E(cm)=211.66 MeV; ²⁵⁷Fm(⁴⁰Ca, 3n), E(cm)=205.66 MeV; ²⁵¹Cf(⁴⁶Ti, 3n), E(cm)=220.39 MeV; ²⁵²Es(⁴⁵Sc, 3n), E(cm)=214.17 MeV; ²⁵⁰Cf(⁴⁶Sc, 2n), E(cm)=218.88 MeV; ²⁴⁷Bk(⁵⁰V, 3n), E(cm)=231.13 MeV; ²⁴⁴Cm(⁵²Cr, 2n), E(cm)=234.88 MeV; ²⁴⁵Cm(⁵²Cr, 3n), E(cm)=240.80 MeV; ²⁴³Cm(⁵³Cr, 2n), E(cm)=236.02 MeV; ²⁴⁷Cm(⁵⁰Cr, 3n), E(cm)=235.12 MeV; ²⁵⁷Fm(⁴²Ca, 3n), E(cm)=205.29 MeV; ²⁵⁴Es(⁴⁵Sc, 3n), E(cm)=213.40 MeV; ²⁵⁷Fm(⁴³Ca, 4n), E(cm)=210.97 MeV; ²⁵⁷Fm(⁴⁴Ca, 3n), E(cm)=205.27 MeV; ²⁵⁷Fm(⁴⁶Ca, 3n), E(cm)=207.84 MeV; ²⁵⁰Cm(⁵³Cr, 3n), E(cm)=234.59 MeV; ²⁵⁷Fm(⁴⁸Ca, 3n), E(cm)=211.07 MeV; calculated production σ for Z=119 and 120 superheavy isotopes. Dinuclear system (DNS) model.

doi: 10.1103/PhysRevC.98.014618
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2018SU08      Phys.Rev. C 97, 054604 (2018)

J.Su, L.Zhu, C.Guo

Influence of the nuclear level density on the odd-even staggering in ⁵⁶Fe + spallation at energies from 300 to 1500 MeV/nucleon

NUCLEAR REACTIONS ¹H(⁵⁶Fe, X), E=300-1500 MeV/nucleon; calculated level-density parameter, energy backshift, σ(E), differential σ(E), odd-even staggering (OES), and neutron- and proton-separation energies for Z=8-26, T_z=-1/2, 0, +1/2, +1 residual nuclei; deduced influence of level density on OES. ⁵⁴Fe, ⁵²Mn; calculated level densities as function of excitation energy. Calculations performed using isospin-dependent quantum molecular dynamics (IQMD) model using statistical model GEMINI code. Comparison with experimental values.

doi: 10.1103/PhysRevC.97.054604
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2018SU17      Phys.Rev. C 98, 024315 (2018)

J.Su, L.Zhu, C.Guo

Isoscalar giant monopole resonance within the Bohr-Mottelson model

NUCLEAR STRUCTURE A=20-240; analyzed excitation energies and incompressibility parameters, widths, surface and symmetry parameters, Coulomb parameter of the incompressibility of the Isoscalar giant monopole resonance (ISGMR) as a function of the mass number in nuclei from ¹²C to ²³⁸U using Bohr-Mottelson model. Comparison with other theoretical predictions.

doi: 10.1103/PhysRevC.98.024315
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2018WU06      Phys.Rev. C 97, 064609 (2018)

Z.-H.Wu, L.Zhu, F.Li, X.-B.Yu, J.Su, C.-C.Guo

Synthesis of neutron-rich superheavy nuclei with radioactive beams within the dinuclear system model

NUCLEAR REACTIONS ^242,244Pu, ²⁴³Am, ^245,248,250Cm, ²⁴⁹Bk, ^250,251Cf(⁴⁸Ca, 2n), (⁴⁸Ca, 3n), (⁴⁸Ca, 4n), (⁴⁸Ca, 5n), E^*=25-60 MeV; ²³⁴Th(⁴²S, 2n), (⁴²S, 3n), (⁴²S, 4n), (⁴²S, 5n), E^*=20-65 MeV; ²³⁴Th, ²⁴⁴Pu(⁴⁶Ar, 2n), (⁴⁶Ar, 3n), (⁴⁶Ar, 4n), (⁴⁶Ar, 5n), E^*=20-65 MeV; ²³⁴Th, ²³⁸U, ²⁴⁸Cm, ²⁵⁵Es(⁴⁴Cl, 2n), (⁴⁴Cl, 3n), (⁴⁴Cl, 4n), (⁴⁴Cl, 5n), E^*=20-65 MeV; ²²⁸Ra(⁴⁵Cl, 2n), (⁴⁵Cl, 3n), (⁴⁵Cl, 4n), (⁴⁵Cl, 5n), E^*=20-65 MeV; ²⁴⁴Pu, ²⁴⁸Cm(⁴³Cl, 2n), (⁴³Cl, 3n), (⁴³Cl, 4n), (⁴³Cl, 5n), E^*=20-65 MeV; ²⁴⁴Pu, ²⁵⁴Cf, ²⁵⁵Es(⁴¹S, 2n), (⁴¹S, 3n), (⁴¹S, 4n), (⁴¹S, 5n), E^*=20-65 MeV; ²⁵⁷Fm(⁴²Ar, 2n), (⁴²Ar, 3n), (⁴²Ar, 4n), (⁴²Ar, 5n), E^*=20-65 MeV; ²⁶⁰Md(³⁸Cl, 2n), (³⁸Cl, 3n), (³⁸Cl, 4n), (³⁸Cl, 5n), E^*=20-65 MeV; calculated evaporation residue σ. ²²⁸Ra(⁴⁵Cl, 2n), E^*=36.0 MeV; ²²⁸Ra(⁴⁶Cl, 3n), E^*=46.0 MeV; ²²⁶Ra(⁴⁷Cl, 2n), E^*=36.0 MeV; ²³⁴Th(⁴²S, 4n), E^*=43.0 MeV; ²²⁸Ra(⁴⁶Ar, 2n), E^*=34.0 MeV; ²³⁴Th(⁴³S, 5n), E^*=51.0 MeV; ²³⁴Th(⁴²S, 3n), E^*=41.0 MeV; ²³⁴Th(⁴³S, 4n), E^*=46.0 MeV; ²³⁴Th(⁴⁴S, 5n), E^*=59.0 MeV; ²³⁴Th(⁴⁴Cl, 2n), E^*=37.0 MeV; ²³⁴Th(⁴⁵Cl, 3n), E^*=44.0 MeV; ²²⁸Ra(⁵⁰K, 2n), E^*=36.0 MeV; ²³⁴Th(⁴⁶Ar, 2n), E^*=34.0 MeV; ²³⁸U(⁴³S, 3n), E^*=41.0 MeV; ²³⁸U(⁴²S, 2n), E^*=37.0 MeV; ²³⁸U(⁴⁴Cl, 3n), E^*=38.0 MeV; ²³⁸U(⁴³Cl, 2n), E^*=36.0 MeV; ²³⁸U(⁴³S, 3n), E^*=41.0 MeV; ²³⁴Th(⁴⁷K, 2n), E^*=33.0 MeV; ²⁴⁴Pu(⁴¹S, 3n), E^*=38.0 MeV; ²⁴⁴Pu(⁴²S, 4n), E^*=42.0 MeV; ²³⁸U(⁴⁶Ar, 2n), E^*=33.0 MeV; ²⁴⁴Pu(⁴³Cl, 4n), E^*=44.0 MeV; ²⁴²Pu(⁴⁴Cl, 3n), E^*=37.0 MeV; ²⁴⁴Pu(⁴²Cl, 3n), E^*=38.0 MeV; ²⁴⁴Pu(⁴⁶Ar, 4n), E^*=38.0 MeV; ²⁴⁴Pu(⁴⁵Ar, 3n), E^*=44.0 MeV; ²⁴²Pu(⁴⁶Ar, 2n), E^*=33.0 MeV; ²⁴⁸Cm(⁴³Cl, 4n), E^*=38.0 MeV; ²⁵⁰Cm(⁴²Cl, 5n), E^*=43.0 MeV; ²⁴⁸Cm(⁴⁴Cl, 5n), E^*=43.0 MeV; ²⁴⁸Cm(⁴⁴Cl, 4n), E^*=38.0 MeV; ²⁵⁰Cm(⁴²Cl, 4n), E^*=39.0 MeV; ²⁵⁰Cm(⁴³Cl, 5n), E^*=45.0 MeV; ²⁵⁴Cf(⁴¹S, 5n), E^*=40.0 MeV; ²⁵³Cf(⁴²S, 5n), E^*=40.0 MeV; ²⁵⁰Cm(⁴⁴Ar, 4n), E^*=37.0 MeV; ²⁵⁵Es(⁴¹S, 5n), E^*=40.0 MeV; ²⁵⁴Cf(⁴²Cl, 5n), E^*=40.0 MeV; ²⁵³Cf(⁴³Cl, 5n), E^*=39.0 MeV; ²⁵⁵Es(⁴¹S, 4n), E^*=37.0 MeV; ²⁵³Cf(⁴³Cl, 4n), E^*=36.0 MeV; ²⁵⁴Cf(⁴²Cl, 4n), E^*=37.0 MeV; ²⁵⁰Cm(⁴⁸Ca, 4n), E^*=35.0 MeV; ²⁴⁸Cm(⁴⁸Ca, 2n), E^*=31.0 MeV; ²⁵⁰Cm(⁴⁶Ca, 2n), E^*=35.0 MeV; ²⁵⁵Es(⁴⁴Cl, 5n), E^*=40.0 MeV; ²⁵⁴Cf(⁴⁴Ar, 4n), E^*=36.0 MeV; ²⁵⁷Fm(⁴¹S, 4n), E^*=37.0 MeV; ²⁵⁰Cm(⁴⁸Ca, 3n), E^*=31.0 MeV; ²⁵⁵Es(⁴⁴Cl, 4n), E^*=36.0 MeV; ²⁵³Cf(⁴⁶Ar, 4n), E^*=34.0 MeV; ²⁵⁴Cf(⁴⁶Ar, 5n), E^*=41.0 MeV; ²⁵⁰Cf(⁴⁸Ca, 3n), E^*=34.0 MeV; ²⁵⁰Cm(⁴⁹Ti, 4n), E^*=42.0 MeV; ²⁵²Cf(⁴⁶Ca, 3n), E^*=36.0 MeV; ²⁶⁰Md(³⁸Cl, 3n), E^*=41.0 MeV; ²⁶⁰Md(³⁹Cl, 4n), E^*=42.0 MeV; ²⁵⁷Fm(⁴²Ar, 4n), E^*=41.0 MeV; ²⁵¹Cf(⁴⁸Ca, 3n), E^*=30.0 MeV; ²⁵²Cf(⁴⁸Ca, 4n), E^*=38.0 MeV; ²⁵⁰Cm(⁴⁹Ti, 3n), E^*=34.0 MeV; ²⁵⁷Fm(⁴²Ar, 3n), E^*=33.0 MeV; ²⁵⁷Fm(⁴³Ar, 4n), E^*=38.0 MeV; ²⁶⁰Md(³⁹Cl, 3n), E^*=37.0 MeV; ²⁴⁴Pu(⁴³Cl, n), E^*=40.0 MeV; ²³⁸Cm(⁴⁸Ca, 2np), E^*=41.0 MeV; ²⁵⁴Cf(⁴¹S, 5n), E^*=40.0 MeV; ²⁴⁸Cm(⁴⁸Ca, 2nα), E^*=46.0 MeV; ²⁴⁸Cm(⁴³Cl, 4n), E^*=38.0 MeV; ²⁴²Pu(⁴⁸Ca, 2np), E^*=35.0 MeV; ²⁴⁸Cm(⁴⁴Cl, 4n), E^*=38.0 MeV; ²⁴²Pu(⁴⁸Ca, np), E^*=40.0 MeV; ²⁴⁴Pu(⁴⁸Ca, 3np), E^*=45.0 MeV; ²⁵⁵Es(⁴¹S, 5n), E^*=40.0 MeV; ²⁴⁵Cm(⁴⁸Ca, np), E^*=32.0 MeV; ²⁴⁹Bk(⁴⁸Ca, 2nα), E^*=37.0 MeV; ²⁵⁵Es(⁴¹S, 4n), E^*=37.0 MeV; ²⁴⁸Cm(⁴⁸Ca, 3np), E^*=44.0 MeV; ²⁴⁹Bk(⁴⁸Ca, nα), E^*=32.0 MeV; calculated evaporation residue σ, and optimal incident beam energies. ⁴⁸Ca(²³⁸U, 2n), (²³⁸U, 3n), (²³⁸U, 4n), E(cm)=184.13-214.13 MeV; calculated evaporation residue σ, potential energy surface, driving potential, survival and complete fusion probabilities, and capture σ. Dinuclear system model. ²⁷¹Db, ^272,273Sg, ²⁷⁶Bh, ²⁷⁸Hs, ²⁷⁹Mt, ²⁸²Ds, ²⁸³Rg, ²⁸⁶Cn, ^287,288Nh, ²⁹⁰Fl, ^291,292Mc, ^294,295Lv, ^295,296Og; calculated evaporation residue σ, and optimal incident beam energies for various reactions. Comparison with available experimental data. Relevance to synthesis of neutron-rich superheavy nuclei using radioactive ion beams, such as those at ATLAS-ANL.

doi: 10.1103/PhysRevC.97.064609
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2018ZH17      Phys.Rev. C 97, 044614 (2018)

L.Zhu, P.-W.Wen, C.-J.Lin, X.-J.Bao, J.Su, C.Li, C.-C.Guo

Shell effects in a multinucleon transfer process

NUCLEAR REACTIONS ¹⁹⁸Pt(¹³⁶Xe, X), E(cm)=643, 420 MeV; ²⁰⁸Pb(¹³⁶Xe, X), E(cm)=450, 526 MeV; ¹⁸⁶W(¹³⁶Xe, X), E(cm)=408 MeV; ¹⁸⁶W(¹⁵⁰Nd, X), E(cm)=451 MeV; calculated potential energy surfaces, total kinetic energy losses (TKEL), and production σ with and without shell corrections using dinuclear system (DNS) model; deduced shell effects on producing trans-target nuclei. Comparison with experimental values.

doi: 10.1103/PhysRevC.97.044614
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2018ZH39      Phys.Rev. C 98, 034609 (2018)

L.Zhu, J.Su, P.-W.Wen, C.-C.Guo, C.Li

Multinucleon transfer process in the reaction ¹⁶⁰Gd + ¹⁸⁶W

NUCLEAR REACTIONS ¹⁸⁶W(¹⁶⁰Gd, X), E(cm)=430, 450, 503, 550 MeV; calculated potential energy surface as a function of mass asymmetry and β₂ deformation, σ(E) for production of primary products as function of mass number, TKEL and β₂, N/Z distribution of primary products, and production σ(E) of Os and Np isotopes, ²⁰²Os, ²⁰¹Re, ²⁴⁰Np, ²⁴¹U, and isotopes of Z=60-100, N=90-150. Dinuclear system (DNS) model with GEMINI code for multinucleon transfer (MNT) process.

doi: 10.1103/PhysRevC.98.034609
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2017GU14      Phys.Rev. C 95, 054622 (2017)

C.Q.Guo, Y.G.Ma, W.B.He, X.G.Cao, D.Q.Fang, X.G.Deng, C.L.Zhou

Isovector dipole resonance and shear viscosity in low energy heavy-ion collisions

NUCLEAR REACTIONS ¹⁰⁰Mo(⁴⁰Ca, X), E=5, 7.5, 10, 12.5, 15 MeV/nucleon; calculated time evolution of nuclear matter density and kinetic-energy density, temperature, chemical potential, and the entropy density of the compound nucleus, post equilibration time evolution of the stress tensor, ratio of shear viscosity over entropy density as function of temperature, giant dipole moment in coordinate space, isovector giant dipole resonance (IVGDR) photon spectra and centroid energies. Green-Kubo method in the framework of an extended quantum molecular dynamics model (EQMD).

doi: 10.1103/PhysRevC.95.054622
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2017GU22      Chin.Phys.Lett. 34, 092101 (2017)

C.-C.Guo, W.-B.He, Y.-G.Ma

Collective Flows of ¹⁶O+¹⁶O Collisions with α-Clustering Configurations

NUCLEAR REACTIONS ¹⁶O(¹⁶O, X), E=40-60 MeV/nucleon; calculated flow parameters. An extended quantum molecular dynamics model, four α-clustering (linear chain, kite, square and tetrahedron) configurations.

doi: 10.1088/0256-307X/34/9/092101
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2017GU32      Eur.Phys.J. A 53, 233 (2017)

C.-Q.Guo, C.-J.Zhang, J.Xu

Revisiting directed flow in relativistic heavy-ion collisions from a multiphase transport model

doi: 10.1140/epja/i2017-12431-2
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2017QU02      Phys.Rev. C 95, 044616 (2017)

W.W.Qu, G.L.Zhang, S.Terashima, T.Furumoto, Y.Ayyad, Z.Q.Chen, C.L.Guo, A.Inoue, X.Y.Le, H.J.Ong, D.Y.Pang, H.Sakaguchi, Y.Sakuragi, B.H.Sun, A.Tamii, I.Tanihata, T.F.Wang, R.Wada, Y.Yamamoto

Repulsive three-body force and channel-coupling effects via ¹²C+¹²C scattering at 100A MeV

NUCLEAR REACTIONS ¹²C(¹²C, ¹²C), (¹²C, ¹²C'), E=100 MeV/nucleon; measured scattered ¹²C using Grand Raiden high-resolution magnetic spectrometer, and ¹⁰B, ¹¹C and other particles by the energy loss and time-of-flight (TOF) information, differential cross sections for the ground state, 4.44 MeV, 2+ state, and the sum of the 7.65 MeV, 0+ and the 9.64 MeV, 3- states in ¹²C using the Ring Cyclotron facility at RCNP-Osaka. Comparison with microscopic coupled-channel calculations, using the double folding method with three different complex G-matrix interactions, the ESC, CEG07b, and MPa.

doi: 10.1103/PhysRevC.95.044616
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2546.

2016WA18      Phys.Rev. C 94, 024608 (2016)

Y.Wang, C.Guo, Q.Li, Z.Li, J.Su, H.Zhang

Influence of differential elastic nucleon-nucleon cross section on stopping and collective flow in heavy-ion collisions at intermediate energies

NUCLEAR REACTIONS ¹H(p, p), (n, n), E=150, 250, 400, 800 MeV; calculated normalized NN differential cross sections versus the cosine of the center-of-mass scattering angle, and compared with experimental data at ≈400 MeV. ¹⁹⁷Au(¹⁹⁷Au, X), E=150, 250, 400, 800 MeV/nucleon; calculated longitudinal and transverse rapidity distributions, directed and elliptic flows of free protons using three nucleon-nucleon (NN) elastic differential cross sections: parameterized differential cross section, differential cross section from the collision term of the self-consistent relativistic Boltzmann-Uehling-Uhlenbeck equation, and the isotropic differential cross section within the new version of the ultrarelativistic quantum molecular dynamics (UrQMD) model.

doi: 10.1103/PhysRevC.94.024608
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2015FU02      Acta Phys.Pol. B46, 127 (2015)

H.Fujioka, Y.Ayyad, J.Benlliure, K.-T.Brinkmann, S.Friedrich, H.Geissel, J.Gellanki, C.Guo, E.Gutz, E.Haettner, M.N.Harakeh, R.S.Hayano, Y.Higashi, S.Hirenzaki, C.Hornung, Y.Igarashi, N.Ikeno, K.Itahashi, M.Iwasaki, D.Jido, N.Kalantar-Nayestanaki, R.Kanungo, R.Knoebel, N.Kurz, V.Metag, I.Mukha, T.Nagae, H.Nagahiro, M.Nanova, T.Nishi, H.J.Ong, S.Pietri, A.Prochazka, C.Rappold, M.P.Reiter, J.L.Rodriguez-Sanchez, C.Scheidenberger, H.Simon, B.Sitar, P.Strmen, B.Sun, K.Suzuki, I.Szarka, M.Takechi, Y.K.Tanaka, I.Tanihata, S.Terashima, Y.N.Watanabe, H.Weick, E.Widmann, J.S.Winfield, X.Xu, H.Yamakami, J.Zhao

Search for η'(958)-nucleus Bound States by (p, d) Reaction at GSI and FAIR

NUCLEAR REACTIONS C(p, d), E=2.5 GeV; measured reaction products, Ep, Ip; deduced preliminary results for η'-mesic nuclei.

doi: 10.5506/APhysPolB.46.127
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2015GU07      Phys.Rev. C 91, 054615 (2015)

C.Guo, Y.Wang, Q.Li, Pe.Wen, F.-S.Zhang

Mass-splitting effect on flows in heavy-ion collisions in the Fermi-energy domain

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E=100 MeV/nucleon; calculated time evolution of neutron and proton densities, rapidity distributions and transverse momentum of neutrons and protons, and effect of neutron-proton effective mass splitting (NPEMS) on flows in heavy-ion collisions at the Fermi-energy domain for directed and elliptic flows. Ultrarelativistic quantum molecular dynamics (UrQMD) model.

doi: 10.1103/PhysRevC.91.054615
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2015GU14      Int.J.Mod.Phys. E24, 1550040 (2015)

C.L.Guo, G.L.Zhang, M.Li

Calculation of α half-lives for Z ≥ 94 nuclei by proximity potential with a new universal function

RADIOACTIVITY ^{232,233,234,235,236,237,238,239,240}Pu, ^{238,239,240,241,242,243}Am, ^{240,241,242,243,244}Cm, ^245,247Bk, ^242,244Cf, ^{250,251,252,253,254}Cf, ^251,252,253Es, ²⁵⁵Es, ^251,252Fm, ^254,256Fm, ²⁵⁴No, ^261,263,265Sg, ²⁶⁶Sg, ²⁷¹Sg, ^{264,265,266,267}Bh, ²⁷²Bh, ^{264,265,266,267}Hs, ²⁶⁹Hs, ²⁷⁵Hs, ²⁷⁰Ds, ²⁸⁴Cn, ^286,288Fl, ^290,292Lv, ²⁹⁴Og(α); calculated T_1/2. Comparison with experimental data.

doi: 10.1142/S0218301315500408
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2015GU16      Phys.Rev. C 92, 014615 (2015)

C.L.Guo, G.L.Zhang, S.P.Hu, J.C.Yang, H.Q.Zhang, P.R.S.Gomes, J.Lubian, X.G.Wu, J.Zhong, C.Y.He, Y.Zheng, C.B.Li, G.S.Li, W.W.Qu, F.Wang, L.Zheng, L.Yu, Q.M.Chen, P.W.Luo, H.W.Li, Y.H.Wu, W.K.Zhou, B.J.Zhu, H.B.Sun

Coupling effects on the fusion of ⁶Li + ¹⁵⁴Sm at energies slightly above the Coulomb barrier

NUCLEAR REACTIONS ¹⁵⁴Sm(⁶Li, X)¹⁵⁴Eu/¹⁵⁶Gd/¹⁵⁶Tb/¹⁵⁷Tb, E=26-36 MeV; measured Eγ, Iγ from different evaporation residues formed via complete and incomplete fusion, complete and incomplete fusion σ(E), σ(E) for 3n+4n channels using on-line γ method at HI-13 Tandem Accelerator of CIAE-Beijing; deduced complete fusion suppression factor as a function of energy. Comparison with theoretical estimates using PACE2.

doi: 10.1103/PhysRevC.92.014615
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0190.

2015QU02      Phys.Lett. B 751, 1 (2015)

W.W.Qu, G.L.Zhang, S.Terashima, T.Furumoto, Y.Ayyad, Z.Q.Chen, C.L.Guo, A.Inoue, X.Y.Le, H.J.Ong, D.Y.Pang, H.Sakaguchi, Y.Sakuragi, B.H.Sun, A.Tamii, I.Tanihata, T.F.Wang, R.Wada, Y.Yamamoto

Effects of repulsive three-body force in ¹²C + ¹²C scattering at 100A MeV

NUCLEAR REACTIONS ¹²C(¹²C, ¹²C), (¹²C, ¹²C'), E=100 MeV/nucleon; measured reaction products; deduced σ(θ). Three double-folding models with complex G-matrix interactions, the CEG07b, MPa, and ESC model calculations.

doi: 10.1016/j.physletb.2015.10.008
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2494.

2015WA10      Eur.Phys.J. A 51, 37 (2015)

Y.Wang, C.Guo, Q.Li, H.Zhang

³H/³He ratio as a probe of the nuclear symmetry energy at sub-saturation densities

NUCLEAR REACTIONS ⁴⁰Ca(⁴⁰Ca, t), (⁴⁰Ca, ³He), ⁹⁰Zr(⁹⁰Zr, t), (⁹⁰Zr(³He), ⁹⁶Ru(⁹⁶Ru, t), (⁹⁶Ru), ³He), ¹⁹⁷Au(¹⁹⁷Au, t), (¹⁹⁷Au, ³He), E=0.12-1 GeV/nucleon; calculated ³H to ³He ratio using UrQMG (ultrarelativistic QMD) with different Skyrme forces; deduced symmetry energy using FOPI data.

doi: 10.1140/epja/i2015-15037-8
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2014GU18      Phys.Rev. C 90, 034606 (2014)

C.Guo, Y.Wang, Q.Li, F.-S.Zhang

Effect of the spin-orbit interaction on flows in heavy-ion collisions at intermediate energies

doi: 10.1103/PhysRevC.90.034606
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2014GU28      Eur.Phys.J. A 50, 187 (2014)

C.L.Guo, G.L.Zhang

Analysis of proton radioactivity of nuclei by using proximity potential with a new universal function

RADIOACTIVITY ¹⁰⁵Sb, ¹⁰⁹I, ^112,113Cs, ^145,146,147Tm, ^150,151Lu, ^155,156,157Ta, ^160,161Re, ^{164,165,166,167}Ir, ¹⁷¹Au, ¹⁷⁷Tl, ¹⁸⁵Bi(p); calculated T_1/2. Compared with other calculations and data.

doi: 10.1140/epja/i2014-14187-5
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2014WA06      Phys.Rev. C 89, 034606 (2014)

Y.Wang, C.Guo, Q.Li, H.Zhang, Z.Li, W.Trautmann

Collective flow of light particles in Au + Au collisions at intermediate energies

doi: 10.1103/PhysRevC.89.034606
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2014WA13      Phys.Rev. C 89, 044603 (2014)

Y.Wang, C.Guo, Q.Li, H.Zhang, Y.Leifels, W.Trautmann

Constraining the high-density nuclear symmetry energy with the transverse-momentum-dependent elliptic flow

doi: 10.1103/PhysRevC.89.044603
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2013GU01      Nucl.Phys. A897, 54 (2013)

C.L.Guo, G.L.Zhang, X.Y.Le

Study of the universal function of nuclear proximity potential from density-dependent nucleon-nucleon interaction

NUCLEAR REACTIONS ⁴⁰Ca(¹⁶O, X), (⁴⁰Ca, X), ⁴⁸Ca(⁴⁸Ca, X), ⁸⁹Y(³²S, X), (³⁴S, X), ^90,96Zr(³⁶S, X), (⁴⁰Ca, X), ⁹²Zr(¹²C, X), (¹⁶O, X), (²⁸Si, X), (³⁵Cl, X), ¹²⁴Sn(⁴⁰Ca, X), ¹⁴⁴Sm(¹⁶O, X), (¹⁷O, X), (²⁸Si, X), ¹⁴⁸Sm(¹⁶O, X), ¹⁹⁷Au(¹⁹F, X), ²⁰⁴Pb(¹²C, X), ²⁰⁸Pb(⁹Be, X), (¹⁶O, X), (¹⁹F, X), (²⁸Si, X), (⁶⁴Ni, X), (⁷⁰Zn, X), (⁸⁶Kr, X), E not given; calculated proximity interaction barrier using double-folding model with density dependent NN interaction. Compared with other calculations and data.

doi: 10.1016/j.nuclphysa.2012.10.003
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2012GU04      Chin.Phys.C 36, 205 (2012)

C.-L.Guo, G.-L.Zhang, I.Tanihata, X.-Y.Le

Simulation of ¹²C+¹²C elastic scattering at high energy by using the Monte Carlo method

NUCLEAR REACTIONS ¹²C(¹²C, X), E=200-400 MeV/nucleon; calculated the relation between scattering angles and kinetic energy. Monte Carlo method.

doi: 10.1088/1674-1137/36/3/003
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2011LI11      Phys.Rev. C 83, 044617 (2011)

Q.Li, C.Shen, C.Guo, Y.Wang, Z.Li, J.Lukasik, W.Trautmann

Nonequilibrium dynamics in heavy-ion collisions at low energies available at the GSI Schwerionen Synchrotron

doi: 10.1103/PhysRevC.83.044617
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1993JI03      Phys.Lett. 172A, 263 (1993)

Z.Jiang, W.Peng, C.Guo, Y.Yu, H.Yu

Hyperfine Structure of Some Odd Parity Levels in the Thulium Spectrum

NUCLEAR MOMENTS ¹⁶⁹Tm; measured hfs; deduced magnetic dipole hyperfine constant. Laser atomic beam spectroscopy.

doi: 10.1016/0375-9601(93)91018-Z
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Note: The following list of authors and aliases matches the search parameter C.Guo: , C.C.GUO, C.L.GUO, C.Q.GUO, C.Y.GUO