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NSR database version of April 27, 2024.

Search: Author = F.Li

Found 33 matches.

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2023LI23      Phys.Rev. A 107, 052807 (2023)

F.-C.Li, Y.B.Tang

Relativistic coupled-cluster analysis of the second-order effects on the hyperfine structure in ¹³³Cs

ATOMIC PHYSICS ¹³³Cs; calculated the first-order hyperfine structure constants using the single and double approximated relativistic coupled-cluster method; deduced the second-order magnetic dipole–magnetic dipole, magnetic dipole–electric quadrupole effects caused by the off-diagonal hyperfine interaction.

doi: 10.1103/PhysRevA.107.052807
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2022LI40      Phys.Rev. C 106, 014906 (2022)

F.Li, Y.-G.Ma, S.Zhang, G.-L.Ma, Q.Shou

Impact of nuclear structure on the background in the chiral magnetic effect in ⁹⁶₄₄Ru + ⁹⁶₄₄Ru and ⁹⁶₄₀Zr + ⁹⁶₄₀Zr collisions at √ s_NN = 7.7-200 GeV from a multiphase transport model

NUCLEAR REACTIONS ⁹⁶Ru(⁹⁶Ru, X), ⁹⁶Zr(⁹⁶Zr, X), E(cm)=7.7, 27, 62.4, 200 GeV; analyzed experimental data from STAR collaboration of RHIC-BNL for distributions of the number of charged hadrons in the pseudorapidity window, mean charge multiplicity, elliptic and triangular flows as function of centrality using the simulation by string melting version of a multiphase transport (AMPT) model; deduced that quadrupole deformation β₂ and neutron skin effects occur in the most-central collisions, while octupole deformation occurs in the near-central collisions. Relevance to precise determination of the shapes of nuclei in isobaric relativistic heavy-ion collisions.

doi: 10.1103/PhysRevC.106.014906
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2021GA27      Appl.Radiat.Isot. 176, 109828 (2021)

J.Gao, Z.Liao, W.Liu, Y.Hu, H.Ma, L.Xia, F.Li, T.Lan, Y.Yang, J.Yang, J.Liao, N.Liu

Simple and efficient method for producing high radionuclidic purity ¹¹¹In using enriched ¹¹²Cd target

NUCLEAR REACTIONS ¹¹²Cd(p, 2n)¹¹¹In, E=21 MeV; measured reaction products, Eγ, Iγ; deduced yields.

doi: 10.1016/j.apradiso.2021.109828
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2021KU20      Phys. Rev. Res. 3, 023227 (2021)

S.J.Kuhn, S.McKay, J.Shen, N.Geerits, R.M.Dalgliesh, E.Dees, A.A.M.Irfan, F.Li, S.Lu, V.Vangelista, D.V.Baxter, G.Ortiz, S.R.Parnell, W.M.Snow, R.Pynn

Neutron-state entanglement with overlapping paths

doi: 10.1103/PhysRevResearch.3.023227
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2021LI11      Phys.Rev. C 103, 024307 (2021)

F.Li, J.-J.Lu, Z.-H.Li, C.-Y.Chen, G.F.Burgio, H.-J.Schulze

Accurate nuclear symmetry energy at finite temperature within a Brueckner-Hartree-Fock approach

doi: 10.1103/PhysRevC.103.024307
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2021LI50      Phys.Rev. C 104, 034608 (2021)

F.Li, Y.Wang, Z.Gao, P.Li, H.Lu, Q.Li, C.Y.Tsang, M.B.Tsang

Application of machine learning in the determination of impact parameter in the ¹³²Sn + ¹²⁴Sn system

NUCLEAR REACTIONS ¹²⁴Sn(¹³²Sn, X), E=270 MeV/nucleon; analyzed experimental data for charged-particle spectra or other simulated events from RIBF-RIKEN facility to extract impact parameters using the ultrarelativistic quantum molecular dynamics (UrQMD) model, and three machine learning algorithms of artificial neural network (ANN), convolutional neural network (CNN), and light gradient boosting machine (LightGBM).

doi: 10.1103/PhysRevC.104.034608
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2021SU21      Eur.Phys.J. A 57, 313 (2021)

K.-J.Sun, C.M.Ko, F.Li, J.Xu, L.-W.Chen

Enhanced yield ratio of light nuclei in heavy ion collisions with a first-order chiral phase transition

doi: 10.1140/epja/s10050-021-00607-4
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2021ZH61      Phys.Rev. C 104, 044901 (2021)

W.-H.Zhou, H.Liu, F.Li, Y.-F.Sun, J.Xu, C.M.Ko

Elliptic flow splittings in the Polyakov-Nambu-Jona-Lasinio transport model

doi: 10.1103/PhysRevC.104.044901
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2020HU06      Appl.Radiat.Isot. 160, 109133 (2020)

Y.Hu, Y.Tang, F.Li, J.Gao, Y.Yang, J.Yang, J.Liao, N.Liu

Production of ⁹⁸Tc with high isotopic purity

NUCLEAR REACTIONS ⁹⁸Mo(p, n)⁹⁸Tc, E=9.4 MeV; measured reaction products, Eγ, Iγ; deduced production technology.

doi: 10.1016/j.apradiso.2020.109133
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2020LI24      Eur.Phys.J. A 56, 167 (2020)

F.Li, G.Chen

The evolution of information entropy components in relativistic heavy-ion collisions

doi: 10.1140/epja/s10050-020-00169-x
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2020LI37      J.Phys.(London) G47, 115104 (2020)

F.Li, Y.Wang, H.Lu, P.Li, Q.Li, F.Liu

Application of artificial intelligence in the determination of impact parameter in heavy-ion collisions at intermediate energies

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E=1 GeV/nucleon; analyzed available data; calculated true impact parameter versus the predicted impact parameter, rapidity distribution of protons.

doi: 10.1088/1361-6471/abb1f9
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2020TO06      Chin.Phys.C 44, 074101 (2020)

L.Tong, P.Li, F.Li, Y.Wang, Q.Li, F.Liu

Nucleon effective mass splitting and density-dependent symmetry energy effects on elliptic flow in heavy ion collisions at E_lab=0.09 ∼ 1.5 GeV/nucleon

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E = 0.09-1.5 GeV/nucleon; analyzed available data; deduced effects of the neutron-proton effective mass splitting, density-dependent nuclear symmetry energy by incorporating an isospin-depenent form of the momentum-dependent potential in the ultra-relativistic quantum molecular dynamics model.

doi: 10.1088/1674-1137/44/7/074103
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2019ST09      Phys.Rev. C 99, 064908 (2019)

V.Steinberg, J.Staudenmaier, D.Oliinychenko, F.Li, O.Erkiner, H.Elfner

Strangeness production via resonances in heavy-ion collisions at energies available at the GSI Schwerionen synchrotron

doi: 10.1103/PhysRevC.99.064908
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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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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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2017LI17      Phys.Rev. C 95, 055203 (2017)

F.Li, C.M.Ko

Spinodal instabilities of baryon-rich quark matter in heavy ion collisions

doi: 10.1103/PhysRevC.95.055203
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2016LI14      Phys.Rev. C 93, 034901 (2016)

Y.Liu, C.M.Ko, F.Li

Heavy quark correlations and the effective volume for quarkonia production

doi: 10.1103/PhysRevC.93.034901
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2016LI16      Phys.Rev. C 93, 035205 (2016)

F.Li, C.M.Ko

Spinodal instabilities of baryon-rich quark-gluon plasma in the Polyakov-Nambu-Jona-Lasinio model

doi: 10.1103/PhysRevC.93.035205
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2016SU24      Phys.Rev. C 94, 045204 (2016)

Y.Sun, C.M.Ko, F.Li

Anomalous transport model study of chiral magnetic effects in heavy ion collisions

doi: 10.1103/PhysRevC.94.045204
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2014GR16      Phys.Rev. C 90, 064909 (2014)

G.Graef, J.Steinheimer, F.Li, M.Bleicher

Deep sub-threshold Ξ and Λ production in nuclear collisions with the UrQMD transport model

doi: 10.1103/PhysRevC.90.064909
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2014KO26      Nucl.Phys. A928, 234 (2014)

C.M.Ko, T.Song, F.Li, V.Greco, S.Plumari

Partonic mean-field effects on matter and antimatter elliptic flows

doi: 10.1016/j.nuclphysa.2014.05.016
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2014XU02      Phys.Rev.Lett. 112, 012301 (2014)

J.Xu, T.Song, C.M.Ko, F.Li

Elliptic Flow Splitting as Probe of the QCD Phase Structure at Finite Baryon Chemical Potential

doi: 10.1103/PhysRevLett.112.012301
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2012LI28      Phys.Rev. C 85, 064902 (2012)

F.Li, L.-W.Chen, C.M.Ko, S.H.Lee

Contributions of hyperon-hyperon scattering to subthreshold cascade production in heavy ion collisions

doi: 10.1103/PhysRevC.85.064902
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2003ZH07      Nucl.Instrum.Methods Phys.Res. B201, 551 (2003)

X.Zhang, F.Li, B.Ding, Z.Liu

Non-Rutherford elastic scattering cross sections of natural magnesium for protons

NUCLEAR REACTIONS Mg(p, p), E=776-2476 keV; measured σ(θ).

doi: 10.1016/S0168-583X(02)02233-4
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0195.

2000HI06      Phys.Rev. C61, 054609 (2000)

K.Hicks, V.Gladyshev, H.Baghaei, A.Caracappa, A.Cichocki, R.Deininger, R.Finlay, T.Gresko, S.Hoblit, M.Khandaker, O.Kistner, F.X.Li, R.Lindgren, M.Lucas, L.Miceli, B.Norum, J.Rapaport, A.Sandorfi, R.Sealock, L.C.Smith, C.Thorn, S.Thornton, C.S.Whisnant, D.Willits, L.E.Wright

The ¹⁶O(γ(pol), π^-p) Reaction at E_γ ≈ 300 MeV

NUCLEAR REACTIONS ¹⁶O(polarized γ, π^-p), E=290-325 MeV; measured σ(E, θ₁, θ₂), spin asymmetries. Comparison with DWIA results.

doi: 10.1103/PhysRevC.61.054609
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1997CH34      Chin.Phys.Lett. 14, 387 (1997)

Z.-H.Cheng, B.-G.Shen, J.-X.Zhang, M.-X.Mao, J.-J.Sun, C.-L.Yang, F.-S.Li, Y.-D.Zhang

Mossbauer Spectroscopy and X-Ray Diffraction Studies of the Phase Composition of Crystallized Nd(x)Fe(81.5-x)B(18.5) Alloys with 7 ≤ x ≤ 15

NUCLEAR REACTIONS ⁵⁸Fe(γ, γ), E=14.4 keV; measured Mossbauer spectra; deduced crystallized Nd₂Fe(81.5-x)-B(18.5) alloy phase composition. Data on X-ray diffraction also studied.

1995LI50      J.Phys.Condens.Matter 7, L235 (1995)

F.Li, Y.Kong, R.Zhou

A ⁵⁷Fe High-Pressure Mossbauer Study of the Ferromagnetic γ'-Fe₄N

NUCLEAR REACTIONS ⁵⁷Fe(γ, γ), E=14.4 keV; measured Mossbauer spectra vs pressure; deduced average magnetic hyperfine field decrease related features.

doi: 10.1088/0953-8984/7/16/004
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1994CH62      J.Phys.Condens.Matter 6, 3109 (1994)

Z.-H.Cheng, M.-X.Mao, C.-L.Yang, F.-S.Li, B.-G.Shen, Y.-D.Zhang

Magnetism and Hyperfine Fields in YFe₁₀V₂: A combined nuclear magnetic resonance and Mossbauer study

NUCLEAR REACTIONS ⁵⁷Fe(γ, γ), E=14.4 keV; measured Mossbauer spectra; deduced hyperfine filed characteristics. NMR data input, YFe₁₀V₂ sample.

NUCLEAR MOMENTS ⁵⁷Fe, ⁸⁹Y, ⁵¹V; measured NMR; deduced hyperfine field characteristics. Mossbauer data input, YFe₁₀V₂ sample.

doi: 10.1088/0953-8984/6/16/016
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1994CH64      J.Phys.Condens.Matter 6, 7437 (1994)

Z.-H.Cheng, M.-X.Mao, J.-J.Sun, B.-G.Shen, F.-W.Wang, C.-L.Yang, F.-S.Li, Y.-D.Zhang

The Effect of Gd Substitution on the Magnetic Properties and Hyperfine Fields of Melt-Spun Ns₄Fe(77.5)B(18.5) Alloys

NUCLEAR MOMENTS ¹¹B, ⁵⁷Fe; measured NMR spectra; deduced Gd substitution role in magnetic properties, hyperfine fields. Melt-spun Nd₄Fe(77.5)B(18.5) alloys.

doi: 10.1088/0953-8984/6/36/023
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1985TI07      Chin.J.Nucl.Phys. 7, 154 (1985)

Tian Ye, Han Yinlu, Shen Qingbiao, Zhuo Yizhong, Liu Wei, Guo Dongmin, Li Fei

A Global Analysis of Integral Cross Section Calculations with the Microscopic Optical Potential

NUCLEAR REACTIONS ¹²C(n, n), E ≤ 100 MeV; ^44,40Ca(n, n), E ≤ 15 MeV; ⁶⁰Ni(n, n), E ≤ 30 MeV; ²⁴²Pu, ⁹⁸Mo(n, n), E ≤ 100 MeV; ¹⁴⁰Ce(n, n), E ≤ 60 MeV; ²³⁸U, ²³²Th(n, n), E ≤ 15 MeV; calculated elastic, nonelastic, total σ(E). Effective Skyrme force, microscopic optical potential.

1985TI08      Chin.J.Nucl.Phys. 7, 344 (1985)

Tian Ye, Han Yinlu, Shen Qingbiao, Zhuo Yizhong, Liu Wei, Guo Dongmin, Li Fei

A Global Analysis of Neutron Differential Elastic Cross Section Calculations with the Microscopic Optical Potential

NUCLEAR REACTIONS ⁴He, ¹²C, ¹⁶O, ²⁴Mg, ²⁸Si, ³²S, ⁴⁰Ca, ^50,52,54Cr, ^54,56Fe, ^58,60,62,64Ni, ^64,66,68Zn, ^90,92,94Zr, ^{92,94,96,98,100}Mo, ^{118,120,122,124}Sn, ^182,184,186W, ²⁰⁸Pb, ²³²Th, ²³⁸U, ²⁴⁰Pu(n, n), E=1-26 MeV; calculated σ(θ). Microscopic optical potential.

1979CH42      Chin.J.Nucl.Phys. 1, 31 (1979)

Chu Yung-Tai, Fan Guo-Ying, Wu Zhong-Li, Feng En-Pu, Liang Guo-Zhao, Li Fa-Wei, Jiao Dun-Long, Li Xian-Hui, Guo Ying-Xiang, Xia Guo-Zhong, Su Ying-Quan, Xiao Qin-Pian

The Research of Scattering and Transfer Reaction of ¹²C with ¹²C

NUCLEAR REACTIONS ¹²C(¹²C, ¹²C), (¹²C, ¹²C'), (¹²C, ¹¹C), (¹²C, ¹³N), E=49, 60, 72.5 MeV; measured σ(θ). Optical model, zero-range DWBA analyses.

1976BI06      Nucl.Instrum.Methods 133, 279 (1976)

L.Birstein, F.Li, R.Klawer

The Manufacture of Needle Type Si(Li) Detectors for Bio-Medical Use

RADIOACTIVITY ³²P; measured Eβ.

doi: 10.1016/0029-554X(76)90620-0
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Note: The following list of authors and aliases matches the search parameter F.Li: , F.C.LI, F.S.LI, F.W.LI, F.X.LI