教育经历
[1] 2001.9-2007.7北京大学 | 粒子物理与原子核物理 | 博士 | 研究生
[2] 1997.9-2001.7
兰州大学物理科学与技术学院 | 微电子 | 学士 | 本科
工作经历
[1] 2010.8-至今北京航空航天大学物理科学与核能工程学院 |核科学与技术系 |
2011年入选教育部新世纪优秀人才支持计划，同年受聘为北京航空航天大学物理科学与核能工程学院教授，现任物理科学与核能工程学院副院长；2016年获国家自然科学基金委优秀青年科学基金资助，同年，还荣获第六届“胡济民”教育科学奖；2017年被评为青年****。在PRL、PRD、PRC、 NPA、 PTP、EPJA等粒子物理与原子核物理领域的著名期刊上发表SCI文章百余篇，被引用2500多次。
社会兼职
[1]Science Bulletin Executive Board Members[2]2016.10-至今
中国核物理学会理事
研究方向
[1] 主要研究方向为理论核物理、核天体物理、超标准模型物理、医学物理团队成员
北航理论核物理组帕文 巴尔德拉马 马努路：教授，博士生导师 联系方式：pavonvalderrama@ipno.in2p
张时声：副教授，硕士生导师 联系方式：zss76@buaa.edu.cn
宋春艳：副教授 硕士生导师 联系方式：cysong@buaa.edu.cn
王文玲：讲师 联系方式: wangwenling@buaa.edu.cn
科研项目
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1)Meson-baryon Scattering in Extend-on-mass-shell scheme at $\mathcal{O}(p^3)$.
By Junxu Lu, Lisheng Geng, Xiulei Ren, Menglin Du.
[arXiv:1902.03395 [hep-ph]].
2)Heavy-quark spin and flavour symmetry partners of the X(3872) revisited: what can we learn from the one boson exchange model?.
By Ming-Zhu Liu, Tian-Wei Wu, Manuel Pavon Valderrama, Ju-Jun Xie, Li-Sheng Geng.
[arXiv:1902.03044 [hep-ph]].
3)Tetra and pentaquarks from the molecular perspective.
By E. Oset, En Wang, J.J. Xie, L.S. Geng, V.R. Debastiani, J.M. Dias, W.H. Liang.
10.1051/epjconf/**3.
EPJ Web Conf. 199 (2019) 01003.
4)Magnetic moments of the spin-1/2 singly charmed baryons in covariant baryon chiral perturbation theory.
By Rui-Xiang Shi, Yang Xiao, Li-Sheng Geng.
[arXiv:1812.07833 [hep-ph]].
5)Opportunities in Flavour Physics at the HL-LHC and HE-LHC.
By A. Cerri et al..
[arXiv:1812.07638 [hep-ph]].
6)Meson-baryon scattering up to the next-to-next-to-leading order in covariant baryon chiral perturbation theory.
By Jung-Xu Lu, Li-Sheng Geng, Xiu-Lei Ren, Meng-Lin Du.
[arXiv:1812.03799 [nucl-th]].
7)Covariant chiral nucleon-nucleon contact Lagrangian up to order $\mathcal{O}(q^4)$.
By Yang Xiao, Li-Sheng Geng, Xiu-Lei Ren.
[arXiv:1812.03005 [nucl-th]].
10.1103/PhysRevC.99.024004.
Phys.Rev. C99 (2019) no.2, 024004.
8)Strong decays of the $\Xi_b(6227)$ as a $\Sigma_b\bar{K}$ molecule.
By Yin Huang, Cheng-jian Xiao, Li-Sheng Geng, Jun He.
[arXiv:1811.10769 [hep-ph]].
10.1103/PhysRevD.99.014008.
Phys.Rev. D99 (2019) no.1, 014008.
9)Strangeness $S=?2$ baryon-baryon interactions in relativistic chiral effective field theory.
By Kai-Wen Li, Tetsuo Hyodo, Li-Sheng Geng.
[arXiv:1809.03199 [nucl-th]].
10.1103/PhysRevC.98.065203.
Phys.Rev. C98 (2018) no.6, 065203.
10)Bound state formation in the $DDK$ system.
By A. Martinez Torres, K.P. Khemchandani, Li-Sheng Geng.
[arXiv:1809.01059 [hep-ph]].
11)Strong decay modes $\bar{K}\Xi$ and $\bar{K}\Xi\pi$ of the $\Omega(2012)$ in the $\bar{K}\Xi(1530)$ and $\eta\Omega$ molecular scenario.
By Yin Huang, Ming-Zhu Liu, Jun-Xu Lu, Ju-Jun Xie, Li-Sheng Geng.
[arXiv:1807.06485 [hep-ph]].
10.1103/PhysRevD.98.076012.
Phys.Rev. D98 (2018) no.7, 076012.
12)Magnetic moments of the spin-1/2 doubly charmed baryons in covariant baryon chiral perturbation theory.
By Ming-Zhu Liu, Yang Xiao, Li-Sheng Geng.
[arXiv:1807.00912 [hep-ph]].
10.1103/PhysRevD.98.014040.
Phys.Rev. D98 (2018) no.1, 014040.
13)$\Xi$(2030) and $\Xi$(2120) as $\bar{K}^*\Sigma$ molecular states.
By Yin Huang, Rong Wang, Jun He, Ju-Jun Xie, Lisheng Geng.
[arXiv:1806.05422 [hep-ph]].
14)The $X(4140)$ and $X(4160)$ resonances in the $e^+e^-\to \gamma J/\psi \phi $ reaction.
By En Wang, Ju-Jun Xie, Li-Sheng Geng, Eulogio Oset.
[arXiv:1806.05113 [hep-ph]].
15)$D \Xi$ and $D^* \Xi$ molecular states from one boson exchange.
By Ming-Zhu Liu, Tian-Wei Wu, Ju-Jun Xie, Manuel Pavon Valderrama, Li-Sheng Geng.
[arXiv:1805.08384 [hep-ph]].
10.1103/PhysRevD.98.014014.
Phys.Rev. D98 (2018) no.1, 014014.
16)$K^*$ mesons with hidden charm arising from $KX(3872)$ and $KZ_c(3900)$ dynamics.
By Xiu-Lei Ren, Brenda B. Malabarba, Li-Sheng Geng, K.P. Khemchandani, A. Martínez Torres.
[arXiv:1805.08330 [hep-ph]].
10.1016/j.physletb.2018.08.034.
Phys.Lett. B785 (2018) 112-117.
17)Particle number conserving BCS approach in the relativistic mean field model and its application to $^{32-74}$Ca.
By Rong An, Lisheng Geng, Shisheng Zhang, Lang Liu.
[arXiv:1804.08496 [nucl-th]].
10.1088/1674-1137/42/11/114101.
Chin.Phys. C42 (2018) no.11, 114101.
18)Octet baryon magnetic moments at next-to-next-to-leading order in covariant chiral perturbation theory.
By Yang Xiao, Xiu-Lei Ren, Jun-Xu Lu, Li-Sheng Geng, Ulf-G. Meißner.
[arXiv:1803.04251 [hep-ph]].
10.1140/epjc/s10052-018-5960-4.
Eur.Phys.J. C78 (2018) 489.
19)Strangeness S=?1 hyperon-nucleon interactions: Chiral effective field theory versus lattice QCD.
By Jing Song, Kai-Wen Li, Li-Sheng Geng.
[arXiv:1802.04433 [nucl-th]].
10.1103/PhysRevC.97.065201.
Phys.Rev. C97 (2018) no.6, 065201.
20)Strong and radiative decays of $D\Xi$ molecular state and newly observed $\Omega_c$ states.
By Yin Huang, Cheng-jian Xiao, Qi Fang Lü, Rong Wang, Jun He, Lisheng Geng.
[arXiv:1801.03598 [hep-ph]].
10.1103/PhysRevD.97.094013.
Phys.Rev. D97 (2018) no.9, 094013.
21)Relativistic chiral description of the $^1S_0$ nucleon-nucleon scattering.
By Xiu-Lei Ren, Kai-Wen Li, Li-Sheng Geng, Jie Meng.
[arXiv:1712.10083 [nucl-th]].
22)Pion–nucleon sigma term revisited in covariant baryon chiral perturbation theory.
By Xiu-Lei Ren, Xi-Zhe Ling, Li-Sheng Geng.
[arXiv:1710.07164 [hep-ph]].
10.1016/j.physletb.2018.05.063.
Phys.Lett. B783 (2018) 7-12.
23)Analysis of the $B^+\to J/\psi \phi K^+$ data at low $J/\psi \phi$ invariant masses and the $X(4140)$ and $X(4160)$ resonances.
By En Wang, Ju-Jun Xie, Li-Sheng Geng, Eulogio Oset.
[arXiv:1710.02061 [hep-ph]].
10.1103/PhysRevD.97.014017.
Phys.Rev. D97 (2018) no.1, 014017.
24)Relativistic baryon-baryon interactions in chiral perturbation theory.
By Xiu-Lei Ren, Kai-Wen Li, Li-Sheng Geng.
[arXiv:1709.10266 [nucl-th]].
25)Evidence for Z=6 `magic number' in neutron-rich carbon isotopes.
By D.T. Tran et al..
[arXiv:1709.03355 [nucl-ex]].
10.1038/s41467-018-04024-y.
26)Exotic doubly charmed ${D}_{s0}^{*}(2317)D$ and ${D}_{s1}^{*}(2460){D}^{*}$ molecules.
By Mario Sanchez Sanchez, Li-Sheng Geng, Jun-Xu Lu, Tetsuo Hyodo, Manuel Pavon Valderrama.
[arXiv:1707.03802 [hep-ph]].
10.1103/PhysRevD.98.054001.
Phys.Rev. D98 (2018) no.5, 054001.
27)Heavy Baryon Molecules in Effective Field Theory.
By Jun-Xu Lu, Li-Sheng Geng, Manuel Pavon Valderrama.
[arXiv:1706.02588 [hep-ph]].
28)Are there near-threshold Coulomb-like Baryonia?.
By Li-Sheng Geng, Jun-Xu Lu, Manuel Pavon Valderrama, Xiu-Lei Ren.
[arXiv:1705.00516 [hep-ph]].
10.1103/PhysRevD.97.091501.
Phys.Rev. D97 (2018) no.9, 091501.
29)Scale Invariance in Heavy Hadron Molecules.
By Lisheng Geng, Junxu Lu, Manuel Pavon Valderrama.
[arXiv:1704.06123 [hep-ph]].
10.1103/PhysRevD.97.094036.
Phys.Rev. D97 (2018) no.9, 094036.
30)Role of the $N^*(1535)$ in the $\Lambda^+_c \to \bar{K}^0 \eta p$ decay.
By Ju-Jun Xie, Li-Sheng Geng.
[arXiv:1704.05714 [hep-ph]].
10.1103/PhysRevD.96.054009.
Phys.Rev. D96 (2017) no.5, 054009.
31)Towards the discovery of new physics with lepton-universality ratios of $b\to s\ell\ell$ decays.
By Li-Sheng Geng, Benjamín Grinstein, Sebastian Jäger, Jorge Martin Camalich, Xiu-Lei Ren, Rui-Xiang Shi.
[arXiv:1704.05446 [hep-ph]].
10.1103/PhysRevD.96.093006.
Phys.Rev. D96 (2017) no.9, 093006.
32)$\Sigma^*_{1/2^-}(1380)$ in the $\Lambda^+_c \to \eta \pi^+ \Lambda$ decay.
By Ju-Jun Xie, Li-Sheng Geng.
[arXiv:1703.09502 [hep-ph]].
10.1103/PhysRevD.95.074024.
Phys.Rev. D95 (2017) no.7, 074024.
33)The \(\Lambda _{b} \to J/\psi K^{0}\Lambda \) and \(\Lambda _{b}\) into \(J/\psi \eta \Lambda \) Reactions and a Hidden-Charm Pentaquark State with Strangeness.
By E. Oset et al..
10.7566/JPSCP.13.020043.
JPS Conf.Proc. 13 (2017) 020043.
34)Hyperon-nucleon Scattering in a Covariant Chiral Effective Field Theory Approach.
By Kai-Wen Li, Xiu-Lei Ren, Li-Sheng Geng, Bingwei Long.
[arXiv:1701.06272 [nucl-th]].
10.22323/1.281.0276.
PoS INPC2016 (2017) 276.
35)Towards a relativistic formulation of baryon-baryon interactions in chiral perturbation theory.
By Xiu-Lei Ren, Kai-Wen Li, Li-Sheng Geng.
[arXiv:1801.00844 [nucl-th]].
10.11804/NuclPhysRev.34.03.392.
Nucl.Phys.Rev. 34 (2017) 392.
36)Leading order relativistic hyperon-nucleon interactions in chiral effective field theory.
By Kai-Wen Li, Xiu-Lei Ren, Li-Sheng Geng, Bing-Wei Long.
[arXiv:1612.08482 [nucl-th]].
10.1088/1674-1137/42/1/014105.
Chin.Phys. C42 (2018) no.1, 014105.
37)On the chiral covariant approach to $\rho\rho$ scattering.
By Li-Sheng Geng, Raquel Molina, Eulogio Oset.
[arXiv:1612.07871 [nucl-th]].
10.1088/1674-1137/41/12/124101.
Chin.Phys. C41 (2017) no.12, 124101.
38)Predictions for pentaquark states of hidden charm molecular nature and comparison with experiment.
By Eulogio Oset et al..
10.1051/epjconf/**4.
EPJ Web Conf. 130 (2016) 06004.
39)Photo-production of tensor mesons.
By Ju-Jun Xie, Li-Sheng Geng, Eulogio Oset.
10.1051/epjconf/**1.
EPJ Web Conf. 130 (2016) 05021.
40)Leading order relativistic chiral nucleon-nucleon interaction.
By Xiu-Lei Ren, Kai-Wen Li, Li-Sheng Geng, Bing-Wei Long, Peter Ring, Jie Meng.
[arXiv:1611.08475 [nucl-th]].
10.1088/1674-1137/42/1/014103.
Chin.Phys. C42 (2018) no.1, 014103.
41)$f_2$(1810) as a triangle singularity.
By Ju-Jun Xie, Li-Sheng Geng, Eulogio Oset.
[arXiv:1610.09592 [hep-ph]].
10.1103/PhysRevD.95.034004.
Phys.Rev. D95 (2017) no.3, 034004.
42)Production of the $\Lambda_c(2940)$ by kaon-induced reactions on a proton target.
By Yin Huang, Jun He, Ju-Jun Xie, Li-Sheng Geng.
[arXiv:1610.06994 [hep-ph]].
10.1103/PhysRevD.99.014045.
Phys.Rev. D99 (2019) no.1, 014045.
43)Reactions Looking for Hidden Charm Pentaquarks with or without Strangeness.
By Eulogio Oset et al..
10.5506/APhysPolBSupp.9.529.
Acta Phys.Polon.Supp. 9 (2016) 529-535.
44)Study of reactions disclosing hidden charm pentaquarks with or without strangeness.
By Eulogio Oset et al..
10.1016/j.nuclphysa.2016.04.038.
Nucl.Phys. A954 (2016) 371-392.
45)$B_s\pi $ – $B\bar{K}$ interactions in finite volume and $X(5568)$.
By Jun-Xu Lu, Xiu-Lei Ren, Li-Sheng Geng.
[arXiv:1607.06327 [hep-ph]].
10.1140/epjc/s10052-017-4660-9.
Eur.Phys.J. C77 (2017) no.2, 94.
46)Consistency between SU(3) and SU(2) covariant baryon chiral perturbation theory for the nucleon mass.
By Xiu-Lei Ren, L. Alvarez-Ruso, Li-Sheng Geng, T. Ledwig, Jie Meng, M. J. Vicente Vacas.
[arXiv:1606.03820 [nucl-th]].
10.1016/j.physletb.2017.01.024.
Phys.Lett. B766 (2017) 325-333.
47)The $a_0(980)$ and $\Lambda(1670)$ in the $\Lambda^+_c \to \pi^+ \eta \Lambda$ decay.
By Ju-Jun Xie, Li-Sheng Geng.
[arXiv:1604.02756 [nucl-th]].
10.1140/epjc/s10052-016-4342-z.
Eur.Phys.J. C76 (2016) no.9, 496.
48)Strangeness $S=-1$ hyperon-nucleon scattering in covariant chiral effective field theory.
By Kai-Wen Li, Xiu-Lei Ren, Li-Sheng Geng, Bingwei Long.
[arXiv:1603.07802 [hep-ph]].
10.1103/PhysRevD.94.014029.
Phys.Rev. D94 (2016) no.1, 014029.
49)$\Lambda_c(2595)$ resonance as a dynamically generated state: The compositeness condition and the large $N_c$ evolution.
By Jun-Xu Lu, Hua-Xing Chen, Zhi-Hui Guo, J. Nieves, Ju-Jun Xie, Li-Sheng Geng.
[arXiv:1603.05388 [hep-ph]].
10.1103/PhysRevD.93.114028.
Phys.Rev. D93 (2016) no.11, 114028.
50)Weak decays of heavy hadrons into dynamically generated resonances.
By Eulogio Oset et al..
[arXiv:1601.03972 [hep-ph]].
10.1142/S**0010.
Int.J.Mod.Phys. E25 (2016) **.
51)The $\Lambda_{b}\rightarrow J/\psi K^{0}\Lambda$ reaction and a hidden-charm pentaquark state with strangeness.
By Jun-Xu Lu, En Wang, Ju-Jun Xie, Li-Sheng Geng, Eulogio Oset.
[arXiv:1601.00075 [hep-ph]].
10.1103/PhysRevD.93.094009.
Phys.Rev. D93 (2016) 094009.
52)Octet baryon masses and sigma terms in covariant baryon chiral perturbation theory.
By Xiu-Lei Ren, Li-Sheng Geng, Jie Meng.
[arXiv:1512.08841 [nucl-th]].
10.22323/1.253.0085.
PoS CD15 (2016) 085.
53)Novel nonperturbative approach for radiative $\bar{B}^0(\bar{B}^0_s)\rightarrow J/\psi \gamma$ decays.
By Li-Sheng Geng, Eulogio Oset.
[arXiv:1512.08563 [hep-ph]].
10.1103/PhysRevD.94.014018.
Phys.Rev. D94 (2016) no.1, 014018.
54)Hidden-charm pentaquark state in $\Lambda^0_b \to J/\psi p \pi^-$ decay.
By En Wang, Hua-Xing Chen, Li-Sheng Geng, De-Min Li, Eulogio Oset.
[arXiv:1512.01959 [hep-ph]].
10.1103/PhysRevD.93.094001.
Phys.Rev. D93 (2016) no.9, 094001.
55)Looking for a hidden-charm pentaquark state with strangeness S=?1 from Ξ$_b^?$ decay into J/ψK$^?$Λ.
By Hua-Xing Chen, Li-Sheng Geng, Wei-Hong Liang, Eulogio Oset, En Wang, Ju-Jun Xie.
[arXiv:1510.01803 [hep-ph]].
10.1103/PhysRevC.93.065203.
Phys.Rev. C93 (2016) no.6, 065203.
56)Photoproduction of the $f'_2(1525), a_2(1320)$, and $K^*_2(1430)$.
By Ju-Jun Xie, Eulogio Oset, Li-Sheng Geng.
[arXiv:1509.06469 [nucl-th]].
10.1103/PhysRevC.93.025202.
Phys.Rev. C93 (2016) no.2, 025202.
57)F-wave heavy-light meson spectroscopy in QCD sum rules and heavy quark effective theory.
By Dan Zhou, Hua-Xing Chen, Li-Sheng Geng, Xiang Liu, Shi-Lin Zhu.
[arXiv:1506.00766 [hep-ph]].
10.1103/PhysRevD.92.114015.
Phys.Rev. D92 (2015) no.11, 114015.
58)$S$-wave $KK^*$ interactions in a finite volume and the $f_1(1285)$.
By Li-Sheng Geng, Xiu-Lei Ren, Yu Zhou, Hua-Xing Chen, Eulogio Oset.
[arXiv:1503.06633 [hep-ph]].
10.1103/PhysRevD.92.014029.
Phys.Rev. D92 (2015) no.1, 014029.
59)Thermodynamics of hadrons using the Gaussian functional method in the linear sigma model.
By Shotaro Imai, Hua-Xin Chen, Hiroshi Toki, Li-Sheng Geng.
10.1142/**29_0010.
60)D-wave heavy-light mesons from QCD sum rules.
By Dan Zhou, Er-Liang Cui, Hua-Xing Chen, Li-Sheng Geng, Xiang Liu, Shi-Lin Zhu.
[arXiv:1410.1727 [hep-ph]].
10.1103/PhysRevD.90.114035.
Phys.Rev. D90 (2014) no.11, 114035.
61)Signature of an $h_1$ state from $J/\psi \to \eta K^{*0}\bar{K}^{*0}$ and theoretical description of the $Z_c(3900)$ and $Z_c(4020)$ as $D \bar D^*$ and $D^* \bar D^*$ molecular states.
By E. Oset et al..
[arXiv:1409.8541 [hep-ph]].
10.1051/epjconf/**.
EPJ Web Conf. 81 (2014) 01011.
62)Dynamically generated $J^P=1/2^-(3/2^-)$ singly charmed and bottom heavy baryons.
By Jun-Xu Lu, Yu Zhou, Hua-Xing Chen, Ju-Jun Xie, Li-Sheng Geng.
[arXiv:1409.3133 [hep-ph]].
10.1103/PhysRevD.92.014036.
Phys.Rev. D92 (2015) no.1, 014036.
63)Kπ interaction in finite volume and the K* resonance.
By Dan Zhou, Er-Liang Cui, Hua-Xing Chen, Li-Sheng Geng, Li-Hua Zhu.
[arXiv:1409.0178 [hep-lat]].
10.1103/PhysRevD.91.094505.
Phys.Rev. D91 (2015) no.9, 094505.
64)The $\bar{p} p \to \phi \phi $ reaction in an effective Lagrangian approach.
By Ju-Jun Xie, Li-Sheng Geng, Xu-Rong Chen.
[arXiv:1407.7403 [nucl-th]].
10.1103/PhysRevC.90.048201.
Phys.Rev. C90 (2014) no.4, 048201.
65)Meson-baryon components in the states of the baryon decuplet.
By F. Aceti, L.R. Dai, L.S. Geng, E. Oset, Y. Zhang.
10.1142/S**00775.
Int.J.Mod.Phys.Conf.Ser. 26 (2014) **.
66)Meson baryon components in the states of the baryon decuplet.
By F. Aceti, L.R. Dai, L.S. Geng, E. Oset, Y. Zhang.
10.1051/epjconf/**.
EPJ Web Conf. 73 (2014) 04009.
67)Octet-baryon axial-vector charges and SU(3)-breaking effects in the semileptonic hyperon decays.
By T. Ledwig, J. Martin Camalich, L.S. Geng, M. J. Vicente Vacas.
[arXiv:1405.5456 [hep-ph]].
10.1103/PhysRevD.90.054502.
Phys.Rev. D90 (2014) no.5, 054502.
68)Octet baryon masses and sigma terms in covariant baryon chiral perturbation theory.
By Xiu-Lei Ren, Li-Sheng Geng, Jie Meng.
[arXiv:1405.4990 [nucl-th]].
10.1142/**29_0033.
69)Test of the $h_1(1830)$ made of $K^{*}\bar{K}^*$ with the $\eta_c\rightarrow \phi K^{*}\bar{K}^{*}$ decay.
By Xiu-Lei Ren, Li-Sheng Geng, Eulogio Oset, Jie Meng.
[arXiv:1405.0153 [nucl-th]].
10.1140/epja/i2014-14133-7.
Eur.Phys.J. A50 (2014) 133.
70)Pseudoscalar meson and vector meson interactions and dynamically generated axial-vector mesons.
By Yu Zhou, Xiu-Lei Ren, Hua-Xing Chen, Li-Sheng Geng.
[arXiv:1404.6847 [nucl-th]].
10.1103/PhysRevD.90.014020.
Phys.Rev. D90 (2014) no.1, 014020.
71)Lowest-lying octet baryon masses up $\mathcal{O}(p^4)$ to in covariant baryon chiral perturbation theory.
By Xiu-Lei Ren, Lisheng Geng, Jie Meng, Hiroshi Toki.
10.1142/S**02154.
Int.J.Mod.Phys.Conf.Ser. 29 (2014) **.
72)Scalar strangeness content of the nucleon and baryon sigma terms.
By Xiu-Lei Ren, Li-Sheng Geng, Jie Meng.
[arXiv:1404.4799 [hep-ph]].
10.1103/PhysRevD.91.051502.
Phys.Rev. D91 (2015) no.5, 051502.
73)Meson-baryon components in the states of the baryon decuplet.
By F. Aceti, L.R. Dai, L.S. Geng, E. Oset, Y. Zhang.
[arXiv:1301.2554 [hep-ph]].
10.1140/epja/i2014-14057-2.
Eur.Phys.J. A50 (2014) 57.
74)Chiral extrapolation and finite-volume dependence of the hyperon vector couplings.
By Li-Sheng Geng, Kai-Wen Li, J. Martin Camalich.
[arXiv:1402.7133 [hep-ph]].
10.1103/PhysRevD.89.113007.
Phys.Rev. D89 (2014) no.11, 113007.
75)Baryon chiral perturbation theory with Wilson fermions up to $\mathcal{O}(a^2)$ and discretization effects of latest $n_f=2+1$ LQCD octet baryon masses.
By Xiu-Lei. Ren, Li-Sheng Geng, Jie Meng.
[arXiv:1311.7234 [hep-ph]].
10.1140/epjc/s10052-014-2754-1.
Eur.Phys.J. C74 (2014) no.2, 2754.
76)Off-shell effects on the interaction of Nambu-Goldstone bosons and $D$ mesons.
By M. Altenbuchinger, Li-Sheng Geng.
[arXiv:1310.5224 [hep-ph]].
10.1103/PhysRevD.89.054008.
Phys.Rev. D89 (2014) no.5, 054008.
77)Scattering lengths of Nambu-Goldstone bosons off $D$ mesons and dynamically generated heavy-light mesons.
By M. Altenbuchinger, L. -S. Geng, W. Weise.
[arXiv:1309.4743 [hep-ph]].
10.1103/PhysRevD.89.014026.
Phys.Rev. D89 (2014) no.1, 014026.
78)Lowest-lying octet baryon masses in covariant baryon chiral perturbation theory.
By Xiu-Lei Ren, Lisheng Geng, Jie Meng, Hiroshi Toki.
[arXiv:1309.3380 [nucl-th]].
10.1142/S**00684.
Int.J.Mod.Phys.Conf.Ser. 26 (2014) **.
79)Study of hadrons using the Gaussian functional method in the O(4) linear σ model.
By Hua-Xing Chen, Shotaro Imai, Hiroshi Toki, Li-Sheng Geng.
[arXiv:1309.0591 [nucl-th]].
10.1088/1674-1137/39/6/064103.
Chin.Phys. C39 (2015) no.6, 064103.
80)Decuplet baryon masses in covariant baryon chiral perturbation theory.
By Xiu-Lei Ren, Li-Sheng Geng, Jie Meng.
[arXiv:1307.1896 [nucl-th]].
10.1103/PhysRevD.89.054034.
Phys.Rev. D89 (2014) no.5, 054034.
81)Low-lying even parity meson resonances and spin-flavor symmetry revisited.
By C. García-Recio, L.S. Geng, J. Nieves, L.L. Salcedo, En Wang, Ju-Jun Xie.
[arXiv:1304.1021 [hep-ph]].
10.1103/PhysRevD.87.096006.
Phys.Rev. D87 (2013) no.9, 096006.
82)Virtual decuplet effects on octet baryon masses in covariant baryon chiral perturbation theory.
By Xiu-Lei Ren, Lisheng Geng, Jie Meng, Hiroshi Toki.
[arXiv:1302.1953 [nucl-th]].
10.1103/PhysRevD.87.074001.
Phys.Rev. D87 (2013) no.7, 074001.
83)Recent developments in SU(3) covariant baryon chiral perturbation theory.
By Lisheng Geng.
[arXiv:1301.6815 [nucl-th]].
10.1007/s11467-013-0327-7.
Front.Phys.(Beijing) 8 (2013) 328-348.
84)Thermodynamics of hadrons using the Gaussian functional method in the linear sigma model.
By Shotaro Imai, Hua-Xing Chen, Hiroshi Toki, Li-Sheng Geng.
[arXiv:1401.3100 [hep-ph]].
10.22323/1.205.0195.
PoS Hadron2013 (2013) 195.
85)Quark mass dependence of the ground-state octet baryons in next-to-next-to-next-to-leading order covariant baryon chiral perturbation theory.
By X.-L. Ren, L.S. Geng, J. Martin Camalich, J. Meng, H. Toki.
[arXiv:1212.1855 [nucl-th]].
10.1007/s00601-012-0581-1.
Few Body Syst. 54 (2013) 1491-1494.
86)Octet baryon masses in next-to-next-to-next-to-leading order covariant baryon chiral perturbation theory.
By X.-L. Ren, L.S. Geng, J. Martin Camalich, J. Meng, H. Toki.
[arXiv:1209.3641 [nucl-th]].
10.1007/JHEP12(2012)073.
JHEP 1212 (2012) 073.
87)The strangeness content of the nucleon from effective field theory and phenomenology.
By J.M. Alarcon, L.S. Geng, J. Martin Camalich, J.A. Oller.
[arXiv:1209.2870 [hep-ph]].
10.1016/j.physletb.2014.01.065.
Phys.Lett. B730 (2014) 342-346.
88)Octet-baryon masses in finite space.
By Xiu-Lei Ren, Lisheng Geng, Jie Meng.
[arXiv:1209.0849 [nucl-th]].
10.1142/**85_0035.
89)Masses and magnetic moments of ground-state baryons in covariant baryon chiral perturbation theory.
By L.S. Geng, J. Martin Camalich, L. Alvarez-Ruso, M.J. Vicente-Vacas.
[arXiv:1209.0538 [nucl-th]].
10.1142/**85_0013.
90)Vector meson-vector meson interaction and dynamically generated resonances.
By E. Oset, L.S. Geng, R. Molina.
10.1088/1742-6596/348/1/012004.
J.Phys.Conf.Ser. 348 (2012) 012004.
91)SU(3) Breaking Corrections to the $D$, $D^*$, $B$, and $B^*$ decay Constants.
By M. Altenbuchinger, L.S. Geng, W. Weise.
[arXiv:1109.0460 [hep-ph]].
10.1016/j.physletb.2012.06.025.
Phys.Lett. B713 (2012) 453-456.
92)Finite-volume effects on octet-baryon masses in covariant baryon chiral perturbation theory.
By Li-sheng Geng, Xiu-lei Ren, J. Martin-Camalich, W. Weise.
[arXiv:1108.2231 [hep-ph]].
10.1103/PhysRevD.84.074024.
Phys.Rev. D84 (2011) 074024.
93)Precision Spectroscopy of Deeply Bound Pionic Atoms and Partial Restoration of Chiral Symmetry in Medium.
By Natsumi Ikeno, Rie Kimura, Junko Yamagata-Sekihara, Hideko Nagahiro, Daisuke Jido, Kenta Itahashi, Li-Sheng Geng, Satoru Hirenzaki.
[arXiv:1107.5918 [nucl-th]].
10.1143/PTP.126.483.
Prog.Theor.Phys. 126 (2011) 483-509.
94)Light quark mass dependence of the $D$ and $D_s$ decay constants.
By L.S. Geng, M. Altenbuchinger, W. Weise.
[arXiv:1012.0666 [hep-ph]].
10.1016/j.physletb.2010.12.060.
Phys.Lett. B696 (2011) 390-395.
95)Analysis of the $N_f=2+1$ lattice QCD results on the lowest-lying baryon masses using covariant ChPT.
By Jorge Martin Camalich, Lisheng Geng, Manuel Jose Vicente Vacas.
[arXiv:1011.2884 [hep-lat]].
10.22323/1.105.0089.
PoS LATTICE2010 (2010) 089.
96)The $f_0(1370)$, $f_0(1710)$, $f_2(1270)$, $f_2'(1525)$, and $K_2^*(1430)$ as dynamically generated states from vector meson - vector meson interaction.
By L.S. Geng, E. Oset, R. Molina, A. Martinez Torres, T. Branz, F.K. Guo, L.R. Dai, B.X. Sun.
[arXiv:1010.4941 [hep-ph]].
10.1063/1.**.
AIP Conf.Proc. 1322 (2010) 214-222.
97)Properties of the ground-state baryons in chiral perturbation theory.
By J. Martin Camalich, L.S. Geng, J.M. Vicente Vacas.
[arXiv:1009.1860 [hep-ph]].
10.1016/j.nuclphysbps.2010.10.055.
Nucl.Phys.Proc.Suppl. 207-208 (2010) 212-215.
98)Vector meson-vector meson interaction and dynamically generated resonances.
By E. Oset, L.S. Geng, R. Molina, D. Nicmorus.
10.1063/1.**.
AIP Conf.Proc. 1257 (2010) no.1, 247-251.
99)Dynamically generated resonances.
By E. Oset et al..
[arXiv:1008.0466 [hep-ph]].
10.1143/PTPS.186.124.
Prog.Theor.Phys.Suppl. 186 (2010) 124-133.
100)Low-energy interactions of Nambu-Goldstone bosons with $D$ mesons in covariant chiral perturbation theory.
By L.S. Geng, N. Kaiser, J. Martin-Camalich, W. Weise.
[arXiv:1008.0383 [hep-ph]].
10.1103/PhysRevD.82.054022.
Phys.Rev. D82 (2010) 054022.
101)Low-lying even parity meson resonances and spin-flavor symmetry.
By C. Garcia-Recio, L.S. Geng, J. Nieves, L.L. Salcedo.
[arXiv:1005.0956 [hep-ph]].
10.1103/PhysRevD.83.016007.
Phys.Rev. D83 (2011) 016007.
102)The lowest-lying baryon masses in covariant SU(3)-flavor chiral perturbation theory.
By J. Martin Camalich, L.S. Geng, M.J. Vicente Vacas.
[arXiv:1003.1929 [hep-lat]].
10.1103/PhysRevD.82.074504.
Phys.Rev. D82 (2010) 074504.
103)Lowest-lying spin-1/2 and spin-3/2 baryon magnetic moments in chiral perturbation theory.
By L.S. Geng, J. Martin-Camalich, L. Alvarez-Ruso, M.J. Vicente-Vacas.
[arXiv:1001.0465 [hep-ph]].
10.1088/1674-1137/34/9/030.
Chin.Phys. C34 (2010) no.9, 1307-1311.
104)Analysis of the LQCD results on the lowest-lying baryon masses in chiral perturbation theory.
By J. Martin Camalich, L.S. Geng, M.J. Vicente Vacas.
10.1063/1.**,10.1063/1.**.
AIP Conf.Proc. 1322 (2010) 440-444, AIP Conf.Proc. 1343 (2011) 308-310.
105)Deeply Bound Kaonic Clusters.
By E. Oset et al..
[arXiv:0912.3145 [nucl-th]].
106)Properties of hyperons in chiral perturbation theory.
By J. Martin Camalich, L.S. Geng, L. Alvarez-Ruso, M.J. Vicente Vacas.
[arXiv:0911.3429 [hep-ph]].
10.1016/j.nuclphysa.2010.01.213.
Nucl.Phys. A835 (2010) 337-341.
107)Two-photon and one photon-one vector meson decay widths of the f(0)(1370), f(2)(1270), f(0)(1710), f-prime(2)(1525), and K*(2)(1430).
By T. Branz, L.S. Geng, E. Oset.
[arXiv:0911.0206 [hep-ph]].
10.1103/PhysRevD.81.054037.
Phys.Rev. D81 (2010) 054037.
108)Study of the f(2)(1270), f(2)-prime(1525), f(0)(1370) and f(0)(1710) in the J/psi radiative decays.
By L.S. Geng, F.K. Guo, C. Hanhart, R. Molina, E. Oset, B.S. Zou.
[arXiv:0910.5192 [hep-ph]].
10.1140/epja/i2010-10971-5.
Eur.Phys.J. A44 (2010) 305-311.
109)SU(3)-breaking corrections to the hyperon vector coupling f(1)(0) in covariant baryon chiral perturbation theory.
By L.S. Geng, J.Martin Camalich, M.J. Vicente Vacas.
[arXiv:0910.3628 [hep-ph]].
10.22323/1.086.0099.
PoS CD09 (2009) 099.
110)Electromagnetic structure of the low-lying baryons in covariant chiral perturbation theory.
By Jorge Martin Camalich, Luis Alvarez-Ruso, Lisheng Geng, Manuel Jose Vicente Vacas.
[arXiv:0910.1563 [hep-ph]].
10.22323/1.086.0097.
PoS CD09 (2009) 097.
111)Electromagnetic structure of the lowest-lying decuplet resonances in covariant chiral perturbation theory.
By L.S. Geng, J. Martin Camalich, M.J. Vicente Vacas.
[arXiv:0907.0631 [hep-ph]].
10.1103/PhysRevD.80.034027.
Phys.Rev. D80 (2009) 034027.
112)Study of the J/psi ---> phi(omega) f(2)(1270), J/psi ---> phi (omega) f-prime(2)(1525) and J/psi ---> K*0(892) anti-K*0(2) (1430) decays.
By A. Martinez Torres, L.S. Geng, L.R. Dai, Bao Xi Sun, E. Oset, B.S. Zou.
[arXiv:0906.2963 [nucl-th]].
10.1016/j.physletb.2009.09.003.
Phys.Lett. B680 (2009) 310-315.
113)Dynamically generated resonances from vector meson-vector meson interaction based on a hidden-gauge unitary approach.
By L.S. Geng, E. Oset, R. Molina, D. Nicmorus.
[arXiv:0905.0419 [hep-ph]].
10.22323/1.069.0040.
PoS EFT09 (2009) 040.
114)SU(3)-breaking corrections to the baryon-octet magnetic moments in chiral perturbation theory.
By J. Martin Camalich, L. Alvarez-Ruso, L.S. Geng, M.J. Vicente Vacas.
[arXiv:0904.4894 [hep-ph]].
10.22323/1.069.0024.
PoS EFT09 (2009) 024.
115)Recent developments in chiral unitary theory of mesons and baryons.
By E. Oset, D. Gamermann, K. Khemchandani, A. Martinez Torres, L.S. Geng, M. Napsuciale.
10.1063/1.**.
AIP Conf.Proc. 1116 (2009) no.1, 81-92.
116)SU(3)-breaking corrections to the hyperon vector coupling f(1)(0) in covariant baryon chiral perturbation theory.
By L.S. Geng, J. Martin Camalich, M.J. Vicente Vacas.
[arXiv:0903.4869 [hep-ph]].
10.1103/PhysRevD.79.094022.
Phys.Rev. D79 (2009) 094022.
117)Leading-order decuplet contributions to the baryon magnetic moments in Chiral Perturbation Theory.
By L.S. Geng, J. Martin Camalich, M.J. Vicente Vacas.
[arXiv:0903.0779 [hep-ph]].
10.1016/j.physletb.2009.04.061.
Phys.Lett. B676 (2009) 63-68.
118)Meson and Baryon resonances.
By E. Oset et al..
[arXiv:0901.1972 [hep-ph]].
10.1016/j.nuclphysa.2009.05.050.
Nucl.Phys. A827 (2009) 255C-260C.
119)Vector meson-vector meson interaction in a hidden gauge unitary approach.
By L.S. Geng, E. Oset.
[arXiv:0812.1199 [hep-ph]].
10.1103/PhysRevD.79.074009.
Phys.Rev. D79 (2009) 074009.
120)Nature of the axial-vector mesons from their N(c) behavior within the chiral unitary approach.
By L.S. Geng, E. Oset, J.R. Pelaez, L. Roca.
[arXiv:0811.1941 [hep-ph]].
10.1140/epja/i2008-10689-y.
Eur.Phys.J. A39 (2009) 81-87.
121)Exploring three-meson systems using chiral dynamics.
By K.P. Khemchandani, A. Martinez Torres, L.S. Geng, M. Napsuciale, E. Oset.
122)Testing the nature of the Lambda(1520) in the J / psi ---> anti-Lambda K- p and J / psi ---> anti-Lambda pi+ pi- Lambda reactions.
By L.S. Geng, E. Oset, B.S. Zou.
[arXiv:0807.4798 [hep-ph]].
10.1140/epja/i2008-10673-7.
Eur.Phys.J. A38 (2008) 239-245.
123)The Role of the N*(1535) in the J/psi ---> anti-p eta p and J/psi ---> anti-p K+ Lambda reactions.
By L.S. Geng, E. Oset, B.S. Zou, M. Doring.
[arXiv:0807.2913 [hep-ph]].
10.1103/PhysRevC.79.025203.
Phys.Rev. C79 (2009) 025203.
124)Chiral Unitary Dynamics of Hadrons and Hadrons in a Nuclear Medium.
By E. Oset et al..
[arXiv:0806.0340 [nucl-th]].
10.1142/S**3610.
Int.J.Mod.Phys. E18 (2009) 1389-1403.
125)Leading SU(3)-breaking corrections to the baryon magnetic moments in Chiral Perturbation Theory.
By L.S. Geng, J. Martin Camalich, L. Alvarez-Ruso, M.J. Vicente Vacas.
[arXiv:0805.1419 [hep-ph]].
10.1103/PhysRevLett.101.222002.
Phys.Rev.Lett. 101 (2008) 222002.
126)Chiral perturbation theory study of the axial N ---> Delta(1232) transition.
By L.S. Geng, J. Martin Camalich, L. Alvarez-Ruso, M.J. Vicente Vacas.
[arXiv:0802.1834 [hep-ph]].
10.1142/S**9125.
Mod.Phys.Lett. A23 (2008) 2246-2249.
127)Nuclear effects in neutrino induced reactions.
By M.J. Vicente Vacas, L. Alvarez-Ruso, L.S. Geng, J. Nieves, M. Valverde, S. Hirenzaki.
[arXiv:0802.1128 [nucl-th]].
10.1142/S**9290.
Mod.Phys.Lett. A23 (2008) 2321-2324.
128)Nucleon-to-Delta axial transition form factors in relativistic baryon chiral perturbation theory.
By L.S. Geng, J. Martin Camalich, L. Alvarez-Ruso, M.J. Vicente Vacas.
[arXiv:0801.4495 [hep-ph]].
10.1103/PhysRevD.78.014011.
Phys.Rev. D78 (2008) 014011.
129)The X(2175) as a resonant state of the phi K anti-K system.
By A. Martinez Torres, K.P. Khemchandani, L.S. Geng, M. Napsuciale, E. Oset.
[arXiv:0801.3635 [nucl-th]].
10.1103/PhysRevD.78.074031.
Phys.Rev. D78 (2008) 074031.
130)Recent Developments in Chiral Unitary Dynamics of Resonances.
By E. Oset et al..
[arXiv:0712.3013 [nucl-th]].
10.1142/S**9046.
Mod.Phys.Lett. A23 (2008) 2201-2208.
131)The WA3 data and the two K(1)(1270) resonances.
By L.S. Geng, E. Oset, L. Roca, J.A. Oller.
[arXiv:0711.4778 [hep-ph]].
132)Application of the RMF mass model to the r-process and the influence of mass uncertainties.
By B. Sun, F. Montes, L.S. Geng, H. Geissel, Yu.A. Litvinov, Jie Meng.
[arXiv:0710.2332 [astro-ph]].
10.1103/PhysRevC.78.025806.
Phys.Rev. C78 (2008) 025806.
133)The Nature of the Lambda(1405).
By E. Oset, L.S. Geng, M. Doring.
[arXiv:0710.5925 [nucl-th]].
10.1007/978-3-540-85144-8_19.
134)Neutrino-induced coherent pion production.
By L. Alvarez-Ruso, L.S. Geng, S. Hirenzaki, M.J. Vicente Vacas, T. Leitner, U. Mosel.
[arXiv:0709.3019 [nucl-th]].
10.1063/1.**.
AIP Conf.Proc. 967 (2007) no.1, 201-204.
135)Coherent pion production in neutrino-nucleus collisions.
By L. Alvarez-Ruso, L.S. Geng, S. Hirenzaki, M.J. Vicente Vacas.
[arXiv:0709.0728 [nucl-th]].
136)The Role of the Lambda(1405) in the pp ---> p K+ Lambda(1405) reaction.
By L.S. Geng, E. Oset.
[arXiv:0707.3343 [hep-ph]].
10.1140/epja/i2008-10518-5.
Eur.Phys.J. A34 (2007) 405-412.
137)Neutral current coherent pion production.
By L. Alvarez-Ruso, L.S. Geng, M.J. Vicente Vacas.
[arXiv:0707.2172 [nucl-th]].
10.1103/PhysRevC.80.029904,10.1103/PhysRevC.76.068501.
Phys.Rev. C76 (2007) 068501, Erratum: Phys.Rev. C80 (2009) 029904.
138)Reflection asymmetric relativistic mean field approach and its application to the octupole deformed nucleus Ra-226.
By L.S. Geng, J. Meng, H. Toki.
[arXiv:0706.0491 [nucl-th]].
10.1088/0256-307X/24/7/021.
Chin.Phys.Lett. 24 (2007) 1865-1868.
139)The Radiative decay of the Lambda(1405) and its two-pole structure.
By L.S. Geng, E. Oset, M. Doring.
[hep-ph/**].
10.1140/epja/i2007-10371-0.
Eur.Phys.J. A32 (2007) 201-211.
140)Charged current neutrino induced coherent pion production.
By L. Alvarez-Ruso, L.S. Geng, S. Hirenzaki, M.J. Vicente Vacas.
[nucl-th/**].
10.1103/PhysRevC.80.019906,10.1103/PhysRevC.75.055501.
Phys.Rev. C75 (2007) 055501, Erratum: Phys.Rev. C80 (2009) 019906.
141)Structure of nuclei far from the stability in relativistic approach.
By S.F. Ban, L.S. Geng, W.H. Long, J. Meng, J. Peng, J.M. Yao, S.Q. Zhang, S.G. Zhou.
10.1140/epjst/e2007-00288-2.
Eur.Phys.J.ST 150 (2007) 139-144.
142)Clues for the existence of two K(1)(1270) resonances.
By L.S. Geng, E. Oset, L. Roca, J.A. Oller.
[hep-ph/**].
10.1103/PhysRevD.75.014017.
Phys.Rev. D75 (2007) 014017.
143)Recent progress in relativistic many-body approach.
By S.F. Ban et al..
10.1142/S**5010.
Int.J.Mod.Phys. E15 (2006) 1447-1464.
144)Fission barrier for Pu-240 in the quadrupole constrained relativistic mean field approach.
By H.F. Lu, L.S. Geng, J. Meng.
10.1088/0256-307X/23/11/016.
Chin.Phys.Lett. 23 (2006) 2940-2943.
145)Spurious shell closures in the relativistic mean field model.
By L.S. Geng, J. Meng, H. Toki, W.H. Long, G. Shen.
[nucl-th/**].
10.1088/0256-307X/23/5/021.
Chin.Phys.Lett. 23 (2006) 1139-1141.
146)The Stability and the shape of the heaviest nuclei.
By L.S. Geng, H. Toki, E.G. Zhao.
[nucl-th/**].
10.1088/0954-3899/32/4/013.
J.Phys. G32 (2006) 573-582.
147)Diabatic constrained relativistic mean field approach.
By H.F. Lu, L.S. Geng, J. Meng.
[nucl-th/**].
10.1140/epja/i2006-10224-4.
Eur.Phys.J. A31 (2007) 273-278.
148)Relativistic Continuum Hartree Bogoliubov theory for ground state properties of exotic nuclei.
By J. Meng, H. Toki, S.G. Zhou, S.Q. Zhang, W.H. Long, L.S. Geng.
[nucl-th/**].
10.1016/j.ppnp.2005.06.001.
Prog.Part.Nucl.Phys. 57 (2006) 470-563.
149)Masses, deformations and charge radii: Nuclear ground-state properties in the relativistic mean field model.
By Li-Sheng Geng, Hiroshi Toki, Jie Meng.
[nucl-th/**].
10.1143/PTP.113.785.
Prog.Theor.Phys. 113 (2005) 785-800.
150)Magic numbers for superheavy nuclei in relativistic continuum Hartree-Bogolyubov theory.
By W. Zhang, J. Meng, S.Q. Zhang, L.S. Geng, H. Toki.
[nucl-th/**].
10.1016/j.nuclphysa.2005.02.086.
Nucl.Phys. A753 (2005) 106-135.
151)A Systematic study of neutron magic nuclei with N=8, N=20, N=28, N=50, N=82, and N=126 in the relativistic mean field theory.
By L.S. Geng, H. Toki, J. Meng.
[nucl-th/**].
10.1088/0954-3899/30/12/011.
J.Phys. G30 (2004) 1915-1928.
152)First order shape transition and critical point nuclei in Sm isotopes from relativistic mean field approach.
By J. Meng, W. Zhang, S.G. Zhou, H. Toki, L.S. Geng.
[nucl-th/**].
10.1140/epja/i2005-10066-6.
Eur.Phys.J. A25 (2005) 23-27.
153)A Full calculation of Zr and Sn isotopes in the relativistic mean field theory.
By L.S. Geng, H. Toki, J. Meng.
[nucl-th/**].
10.1142/S**5543.
Mod.Phys.Lett. A19 (2004) 2171-2190.
154)Alpha decay chains of 115-288-173 and 115-287-172 in the relativistic mean field theory.
By L.S. Geng, H. Toki, J. Meng.
[nucl-th/**].
10.1103/PhysRevC.68.061303.
Phys.Rev. C68 (2003) 061303.
155)Proton rich nuclei at and beyond the proton drip line in the relativistic mean field theory.
By L.S. Geng, H. Toki, J. Meng.
[nucl-th/**].
10.1143/PTP.112.603.
Prog.Theor.Phys. 112 (2004) 603-617.
156)Proton and neutron skins of light nuclei within the relativistic mean field theory.
By L.S. Geng, H. Toki, A. Ozawa, J. Meng.
[nucl-th/**].
10.1016/j.nuclphysa.2003.10.014.
Nucl.Phys. A730 (2004) 80-94.
157)Relativistic mean field theory for deformed nuclei with the pairing correlations.
By Li-sheng Geng, Hiroshi Toki, Satoru Sugimoto, Jie Meng.
[nucl-th/**].
10.1143/PTP.110.921.
Prog.Theor.Phys. 110 (2003) 921-936.
158)Pairing correlations and resonant states in the relativistic mean field theory.
By N. Sandulescu, L.S. Geng, H. Toki, G. Hillhouse.
[nucl-th/**].
10.1103/PhysRevC.68.054323.
Phys.Rev. C68 (2003) 054323.
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2019.03.10 年会合影
组内春游：香山小分队
组内秋游：登长城
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