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NSR database version of April 11, 2024.

Search: Author = S.M.Wang

Found 28 matches.

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2023CH46      Phys.Rev.Lett. 131, 172501 (2023)

R.J.Charity, J.Wylie, S.M.Wang, T.B.Webb, K.W.Brown, G.Cerizza, Z.Chajecki, J.M.Elson, J.Estee, D.E.M.Hoff, S.A.Kuvin, W.G.Lynch, J.Manfredi, N.Michel, D.G.McNeel, P.Morfouace, W.Nazarewicz, C.D.Pruitt, C.Santamaria, S.Sweany, J.Smith, L.G.Sobotka, M.B.Tsang, A.H.Wuosmaa

Strong Evidence for 9N and the Limits of Existence of Atomic Nuclei

RADIOACTIVITY 9N(p), 8C, 6Be(2p) [from 9Be(13O, X)9N, E=69.5 MeV/nucleon]; measured decay products, Ep, Ip. 9N, 8C; deduced invariant-mass spectra, level diagrams, possible single resonancelike peak in the spectrum. R-matrix fits, comparison with the theoretical predictions of an open-quantum-system approach. The National Superconducting Cyclotron Laboratory at Michigan State University.

doi: 10.1103/PhysRevLett.131.172501
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2023DI08      Chin.Phys.C 47, 094101 (2023)

M.-Q.Ding, P.Su, D.-Q.Fang, S.-M.Wang

Investigation of the relationship between mirror proton radii and neutron-skin thickness

NUCLEAR STRUCTURE 18O, 18,19,21,22Ne, 19F, 21,23Na, 22,23Mg, 34,35,37,38Ar, 34,36S, 35,37Cl, 36,37,38Ca, 54Fe, 54Ni; analyzed available data; deduced that neutron-skin thickness of a neutron-rich nucleus is proportional to the difference between the proton radii of mirror nuclei using the axially deformed solutions of the Skyrme-Hartree-Fock-Bogoliubov equations with 132 sets of Skyrme interaction parameters.

doi: 10.1088/1674-1137/ace680
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2023PF02      Prog.Part.Nucl.Phys. 132, 104050 (2023)

M.Pfutzner, I.Mukha, S.M.Wang

Two-proton emission and related phenomena

RADIOACTIVITY 19Mg, 45Fe, 48Ni, 54Zn, 67Kr, 6Be, 11,12O, 15,16,17Ne, 29,30Ar(2p); analyzed available data; deduced T1/2, Q-values, resonance widths, J, π. Comparison with calculations.

doi: 10.1016/j.ppnp.2023.104050
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2023WA15      Phys. Rev. Res. 5, 023183 (2023)

S.M.Wang, W.Nazarewicz, A.Volya, Y.G.Ma

Probing the nonexponential decay regime in open quantum systems

RADIOACTIVITY 6Be(2p), 6He(2n); calculated survival probability; deduced the phenomenon of a nonexponential decay of an open quantum system at long times.

doi: 10.1103/PhysRevResearch.5.023183
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2023YA28      Phys.Rev. C 108, 044307 (2023)

Y.H.Yang, Y.G.Ma, S.M.Wang, B.Zhou, D.Q.Fang

Structure and decay mechanism of the low-lying states in 9Be and 9B

doi: 10.1103/PhysRevC.108.044307
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2022LI15      Phys.Rev. C 105, 034613 (2022)

W.Liu, J.L.Lou, Y.L.Ye, S.M.Wang, Z.W.Tan, Z.H.Li, Q.T.Li, H.Hua, X.F.Yang, J.Y.Xu, H.J.Ong, D.T.Tran, N.Aoi, E.Ideguchi, D.Y.Pang, C.X.Yuan, Y.Jiang, B.Yang, Y.Liu, J.G.Li, Z.Q.Chen, J.X.Han, S.W.Bai, G.Li, K.Ma, H.Y.Zhu, B.L.Xia

New investigation of low-lying states in 12Be via a 2H(13B, 3He) reaction

NUCLEAR REACTIONS 2H(13B, d), (13B, 3He), E=23 MeV/nucleon; measured reaction products, deuteron spectra, 3He spectra, angular distributions; deduced σ(θ), optical potential parameters. 12Be; deduced levels, J, π, spectroscopic factors, resonance widths. DWBA analysis. Comparison to various calculations in particular to one using the shell model with the YSOX interaction and Gamow coupled-channel (GCC) approach (for the resonance widths). Secondary beam from 18O(9Be, X), E=60 MeV/nucleon (RCNP, Osaka).

doi: 10.1103/PhysRevC.105.034613
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2022WA33      J.Phys.(London) G49, 10LT02 (2022)

S.M.Wang, W.Nazarewicz, R.J.Charity, L.G.Sobotka

Nucleon-nucleon correlations in the extreme oxygen isotopes

RADIOACTIVITY 11,12O(2p), 26O(2n); calculated density distributions of two-nucleon decays, asymptotic energy and angular correlations of protons and neutrons, Jacobi-Y correlations of two protons emitted from the broad low-energy structure, two-neutron decay of threshold resonance in 26O. The Gamow coupled-channel (GCC) method.

doi: 10.1088/1361-6471/ac888f
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2022YU02      Phys.Rev. C 105, L061303 (2022)

Q.Yuan, S.Q.Fan, B.S.Hu, J.G.Li, S.Zhang, S.M.Wang, Z.H.Sun, Y.Z.Ma, F.R.Xu

Deformed in-medium similarity renormalization group

NUCLEAR STRUCTURE 6,8,10,12,14,16Be, 10,12,14,16,18,20,22C, 14,16,18,20,22,24,26,28O, 16,18,20,22,24,26,28,30,32,34Ne, 20,22,24,26,28,30,32,34,36,38,40Mg; calculated ground-state energies, and charge radii using deformed ab initio in-medium similarity renormalization group (deformed IMSRG), Hartree-Fock, and angular momentum projection methods for open-shell nuclei; results benchmarked with the no-core shell model and valence-space IMSRG calculations. Comparison with experimental data.

doi: 10.1103/PhysRevC.105.L061303
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2021CH17      Phys.Rev. C 103, L031302 (2021)

J.Chen, S.M.Wang, H.T.Fortune, J.L.Lou, Y.L.Ye, Z.H.Li, N.Michel, J.G.Li, C.X.Yuan, Y.C.Ge, Q.T.Li, H.Hua, D.X.Jiang, X.F.Yang, D.Y.Pang, F.R.Xu, W.Zuo, J.C.Pei, J.Li, W.Jiang, Y.L.Sun, H.L.Zang, N.Aoi, H.J.Ong, E.Ideguchi, Y.Ayyad, K.Hatanaka, D.T.Tran, D.Bazin, J.Lee, Y.N.Zhang, J.Wu, H.N.Liu, C.Wen, T.Yamamoto, M.Tanaka, T.Suzuki

Observation of the near-threshold intruder 0- resonance in 12Be

NUCLEAR REACTIONS 2H(11Be, p)12Be, E=26.9 MeV/nucleon; measured E(p), I(p), σ(θ) using two parallel-plate avalanche counters (PPACs), and a set of annular double-sided silicon detectors (ADSSDs) at the RCNP, Osaka University. 12Be; deduced missing-mass spectra of 12Be unbound states, levels, J, π, a 0- resonance just above S(n), decay width. DWBA analysis. Comparison with Gamow coupled-channel and Gamow shell-model calculations.

doi: 10.1103/PhysRevC.103.L031302
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2690. Data from this article have been entered in the XUNDL database. For more information, click here.


2021DA11      Phys.Rev. C 103, 064327 (2021)

B.Dai, B.S.Hu, Y.Z.Ma, J.G.Li, S.M.Wang, C.W.Johnson, F.R.Xu

Tensor force role in β decays analyzed within the Gogny-interaction shell model

NUCLEAR STRUCTURE 10,11,12,13,14,15C; calculated levels, J, π, ground-state energies. 10,11,12,13,14,15N; calculated ground-state energies. Shell-model calculations with the effective interaction derived from D1S Gogny interaction with and without the tensor force. 15,17O; calculated spectra using the Single-particle energies (SPEs) and two-body matrix elements (TBMEs) from the D1S interaction. Comparison with theoretical calculations using WBP interaction, and with experimental data.

RADIOACTIVITY 10,11C, 12,13N(β+); 14,15C(β-); calculated β spectra, B(GT) using shell model within the p-sd space and the D1S Gogny interaction with different components of tensor force. Comparison with theoretical calculations using WBP interaction, and with experimental data. Relevance to anomalously long half-life of 14C decay, and role of tensor force, cross-shell mixing, and three-body forces in β decay.

doi: 10.1103/PhysRevC.103.064327
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2021JI15      Phys.Rev.Lett. 127, 262502 (2021)

Y.Jin, C.Y.Niu, K.W.Brown, Z.H.Li, H.Hua, A.K.Anthony, J.Barney, R.J.Charity, J.Crosby, D.Dell'Aquila, J.M.Elson, J.Estee, M.Ghazali, G.Jhang, J.G.Li, W.G.Lynch, N.Michel, L.G.Sobotka, S.Sweany, F.C.E.Teh, A.Thomas, C.Y.Tsang, M.B.Tsang, S.M.Wang, H.Y.Wu, C.X.Yuan, K.Zhu

First Observation of the Four-Proton Unbound Nucleus 18Mg

RADIOACTIVITY 18Mg(14O), (2p), (4p) [from 9Be(20Mg, X)18Mg, E=170 MeV/nucleon]; measured decay products, Ep, Ip, 18Mg, 16Ne; deduced decay energy spectra, level scheme, J, π, resonance parameters. Comparison with the Gamow shell model (GSM) calculations.

doi: 10.1103/PhysRevLett.127.262502
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Data from this article have been entered in the XUNDL database. For more information, click here.


2021LI64      Phys.Rev. C 104, 064605 (2021)

W.Liu, J.L.Lou, Y.L.Ye, Z.H.Li, Q.T.Li, H.Hua, X.F.Yang, J.Y.Xu, H.J.Ong, D.T.Tran, N.Aoi, E.Ideguchi, D.Y.Pang, C.X.Yuan, S.M.Wang, Y.Jiang, B.Yang, Y.Liu, J.G.Li, Z.Q.Chen, J.X.Han, S.W.Bai, G.Li, K.Ma, Z.W.Tan, H.Y.Zhu, B.L.Xia

s- and d-wave intruder strengths in 13Bg.s. via the 1H(13B, d)12B reaction

NUCLEAR REACTIONS 1H(13B, p), (13B, d)12B, E=23 MeV/nucleon, [13B secondary beam from 9Be(18O, X), E=58 MeV/nucleon]; measured reaction products, E(d), I(d), E(p), I(p), σ(θ), (particle)(particle)-coin using four sets of charged-particle telescopes of double-sided silicon strip (DSSD) detectors at RCNP-Osaka accelerator facility. 12,13B; analyzed optical potential parameters for low energy elastic scattering and single-neutron transfer reaction. 13B; deduced levels, J, π, L-transfers from σ(θ) distributions relative spectroscopic factors, s- and d-wave intruder strengths in the ground state; calculated p-, s-, and d-wave intensities from the shell model with the YSOX interaction and Gamow coupled-channel (GCC) approach. Comparison with systematics of p-, s-, and d-wave intensities in the ground state of 12Be, 13B and 14C.

doi: 10.1103/PhysRevC.104.064605
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Data from this article have been entered in the XUNDL database. For more information, click here.


2021SH23      Phys.Rev. C 103, L061301 (2021)

G.Z.Shi, J.J.Liu, Z.Y.Lin, H.F.Zhu, X.X.Xu, L.J.Sun, P.F.Liang, C.J.Lin, J.Lee, C.X.Yuan, S.M.Wang, Z.H.Li, H.S.Xu, Z.G.Hu, Y.Y.Yang, R.F.Chen, J.S.Wang, D.X.Wang, H.Y.Wu, K.Wang, F.F.Duan, Y.H.Lam, P.Ma, Z.H.Gao, Q.Hu, Z.Bai, J.B.Ma, J.G.Wang, F.P.Zhong, C.G.Wu, D.W.Luo, Y.Jiang, Y.Liu, D.S.Hou, R.Li, N.R.Ma, W.H.Ma, G.M.Yu, D.Patel, S.Y.Jin, Y.F.Wang, Y.C.Yu, Q.W.Zhou, P.Wang, L.Y.Hu, X.Wang, H.L.Zang, P.J.Li, Q.R.Gao, H.Jian, S.X.Zha, F.C.Dai, R.Fan, Q.Q.Zhao, L.Yang, P.W.Wen, F.Yang, H.M.Jia, G.L.Zhang, M.Pan, X.Y.Wang, H.H.Sun, X.H.Zhou, Y.H.Zhang, M.Wang, M.L.Liu, H.J.Ong, W.Q.Yang

β-delayed two-proton decay of 27S at the proton-drip line

RADIOACTIVITY 27S(β+2p)[from 9Be(32S, X), E=80.6 MeV/nucleon, followed by separation and purification of fragments using RIBLL1 at HIRFL-Lanzhou facility, and implanted into three W1-type double-sided silicon strip detectors (DSSDs)]; measured reaction products, E(p), I(p), pp-coin, p(θ), half-life of 27S decay using Si detectors surrounded by HPGe detectors; deduced branching ratio of β+2p decay, identified as a two-proton transition, dominantly sequential, via the isobaric-analog state (IAS) in 27P to the ground state of 25Al.

doi: 10.1103/PhysRevC.103.L061301
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Data from this article have been entered in the XUNDL database. For more information, click here.


2021WA23      Phys.Rev.Lett. 126, 142501 (2021)

S.M.Wang, W.Nazarewicz

Fermion Pair Dynamics in Open Quantum Systems

NUCLEAR STRUCTURE 6Be, 6He; calculated time evolution of the wave functions, asymptotic energy and angular correlations of emitted nucleons, density and momentum distributions of two-nucleon decays from the g.s., three-body decays.

doi: 10.1103/PhysRevLett.126.142501
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2021WY01      Phys.Rev. C 104, L061301 (2021)

J.Wylie, J.Okolowicz, W.Nazarewicz, M.Ploszajczak, S.M.Wang, X.Mao, N.Michel

Spectroscopic factors in dripline nuclei

NUCLEAR STRUCTURE 9C, 9Li; calculated spectroscopic factors for the knockout of a p3/2 nucleon from the 3/2- g.s. of 9C and 9Li to ground states of 8C, 8He, 8B, and 8Li. 8C, 8He, 8B, 8Li, 9C, 9Li; calculated squared harmonic-oscillator basis shell model HO-SM and Gamow shell model (GCM) amplitudes of shell-model configurations, with details of GSM spectra and dominant configurations in ps-space and psd-space given in the Supplemental Material 13O, 13F; calculated ratio of spectroscopic in shell model embedded in the continuum (SMEC) and HO-SM for neutron and proton removal from the g.s. of 13O to 12O and 12N ground states, and 13F proton resonance to the second 2+ state of 12O.

doi: 10.1103/PhysRevC.104.L061301
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2020HO06      Nature(London) 580, 52 (2020)

D.E.M.Hoff, A.M.Rogers, S.M.Wang, P.C.Bender, K.Brandenburg, K.Childers, J.A.Clark, A.C.Dombos, E.R.Doucet, S.Jin, R.Lewis, S.N.Liddick, C.J.Lister, Z.Meisel, C.Morse, W.Nazarewicz, H.Schatz, K.Schmidt, D.Soltesz, S.K.Subedi, S.Waniganeththi

Mirror-symmetry violation in bound nuclear ground states

RADIOACTIVITY 73Sr(β+p), (β+), (EC) [from Be(92Mo, X), E=140 MeV/nucleon]; measured decay products, Eβ, Iβ, Ep, Ip; deduced T1/2, γ-ray energies, level scheme, J, π, branching ratios, isobaric-analogue state (IAS), log ft. Comparison with calculations, available data.

doi: 10.1038/s41586-020-2123-1
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Data from this article have been entered in the XUNDL database. For more information, click here.


2020HO17      Phys.Rev. C 102, 045810 (2020)

D.E.M.Hoff, A.M.Rogers, Z.Meisel, P.C.Bender, K.Brandenburg, K.Childers, J.A.Clark, A.C.Dombos, E.R.Doucet, S.Jin, R.Lewis, S.N.Liddick, C.J.Lister, C.Morse, H.Schatz, K.Schmidt, D.Soltesz, S.K.Subedi, S.M.Wang, S.Waniganeththi

Influence of 73Rb on the ashes of accreting neutron stars

RADIOACTIVITY 73Sr(β+), (β+p)[from 9Be(92Mo, X), E=140 MeV/nucleon, followed by the separation and purification of 73Sr beam by A1900 and radiofrequency fragment separators at NSCL-MSU, and implanted in double-sided silicon strip detector]; measured Ep, Ip. 73Rb; deduced energy of the isobaric analogue state (IAS), J, π, isospin, S(p), β++ϵ feedings and logft for transitions to the 3/2- g.s. and the IAS, influence of 73Rb S(p) on x-ray bursts, and impact on the products of the rp process. Bayesian analysis of beta-delayed proton spectrum.

ATOMIC MASSES 73Rb, 73Sr; analyzed mass excesses by IMME analysis for A=73 isobars of 73Sr, 73Rb, 73Kr and 73Br; deduced mass excesses for 73Rb and 73Sr, and S(p) for 73Rb. Comparison with data in AME2016.

doi: 10.1103/PhysRevC.102.045810
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2019WA16      Phys.Rev. C 99, 054302 (2019)

S.M.Wang, W.Nazarewicz, R.J.Charity, L.G.Sobotka

Structure and decay of the extremely proton-rich nuclei 11, 12O

NUCLEAR STRUCTURE 10,11N, 11,12O, 11Li, 12Be; calculated levels, J, π, 2p partial decay width of 12O. 11O, 11Li, 12Be, 12O; calculated levels, J, π, two-proton widths and configurations for mirror nuclei. 12C; calculated two-proton angular correlation. 6Be, 12O; calculated 2p density distributions. 11O, 11Li; calculated angular correlations between the valence nucleons in ground and excited states. 10N, 11O; calculated trajectories of the threshold resonances. Deformed core+nucleon+nucleon Gamow coupled channel (GCC) method. Comparison with experimental data.

RADIOACTIVITY 6Be, 11,12O(2p); calculated 2p density distributions, decay widths. Deformed core+nucleon+nucleon Gamow coupled channel (GCC) method.

doi: 10.1103/PhysRevC.99.054302
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2019WE03      Phys.Rev.Lett. 122, 122501 (2019)

T.B.Webb, S.M.Wang, K.W.Brown, R.J.Charity, J.M.Elson, J.Barney, G.Cerizza, Z.Chajecki, J.Estee, D.E.M.Hoff, S.A.Kuvin, W.G.Lynch, J.Manfredi, D.McNeel, P.Morfouace, W.Nazarewicz, C.D.Pruitt, C.Santamaria, J.Smith, L.G.Sobotka, S.Sweany, C.Y.Tsang, M.B.Tsang, A.H.Wuosmaa, Y.Zhang, K.Zhu

first Observation of Unbound 11O, the Mirror of the Halo Nucleus 11Li

RADIOACTIVITY 11,12O(2p) [from 9Be(13O, xn)11O/12O, E<69.5 MeV/nucleon]; measured decay products, Ep, Ip; deduced an invariant-mass spectrum, resonant state widths, two-nucleon density distributions. Comparison with theoretical calculations.

doi: 10.1103/PhysRevLett.122.122501
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2019WE11      Phys.Rev. C 100, 024306 (2019); Erratum Phys.Rev. C 102, 019904 (2020)

T.B.Webb, R.J.Charity, J.M.Elson, D.E.M.Hoff, C.D.Pruitt, L.G.Sobotka, K.W.Brown, J.Barney, G.Cerizza, J.Estee, G.Jhang, W.G.Lynch, J.Manfredi, P.Morfouace, C.Santamaria, S.Sweany, M.B.Tsang, T.Tsang, S.M.Wang, Y.Zhang, K.Zhu, S.A.Kuvin, D.McNeel, J.Smith, A.H.Wuosmaa, Z.Chajecki

Particle decays of levels in 11, 12N and 12O investigated with the invariant-mass method

NUCLEAR REACTIONS 9Be(13O, 12O), (13O, 12N), (13O, 11N), E=69.5 MeV/nucleon, [secondary 13O beam from 9Be(16O, 12O), E=150 MeV/nucleon primary reaction, followed by separation of ion beam using A1900 magnetic separator]; measured charged particles, (particle)(particle)-coin, cross sections using the High Resolution Array (HiRA) of 14 ΔE-E Si-CsI(Tl) telescopes at NSCL, MSU facility. 12,13O, 12N; deduced levels, J, π, 2p-, 3p-, 1p- and 2p+α-decay branches, p+10C, p+11C, 2p+10C invariance mass spectra, widths, total decay energy spectrum and invariant-mass spectra from coincident 4p+2α events. Comparison with Gamow coupled-channel (GCC) calculations, and with previous experimental data in the ENSDF database.

doi: 10.1103/PhysRevC.100.024306
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Data from this article have been entered in the XUNDL database. For more information, click here.


2019ZH46      Phys.Rev. C 100, 044609 (2019)

Y.X.Zhao, Y.Z.Sun, S.T.Wang, Z.Y.Sun, X.H.Zhang, D.Yan, D.Y.Pang, P.Ma, Y.H.Yu, K.Yue, S.W.Tang, S.M.Wang, F.Fang, Y.Sun, Z.H.Cheng, X.M.Liu, H.R.Yang, C.G.Lu, L.M.Duan

One-proton knockout from 16C at around 240 MeV/nucleon

NUCLEAR REACTIONS 12C(16C, 15B), E=239 MeV/nucleon, [secondary16O beam from 9Be(18O, X)8Li/10Be/11Be/13B/16C, E=280 MeV/nucleon primary reaction using RIBLL2 at HRIFL-Lanzhou facility]; measured reaction products by magnetic rigidity (Bρ), time of flight (TOF), and energy loss (ΔE), mass yields. 16C, 15B; deduced σ for one-proton knockout, spectroscopic reduction factor. Comparison to predictions based on the eikonal reaction model with shell-model structure inputs, and with previous experimental data for 9Be(16C, 15B), E=75 MeV/nucleon reaction. Discussed energy dependence of the spectroscopic reduction factor, and the role of surface neutrons as spectators.

doi: 10.1103/PhysRevC.100.044609
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0221.


2018WA10      Phys.Rev.Lett. 120, 212502 (2018)

S.M.Wang, W.Nazarewicz

Puzzling Two-Proton Decay of 67Kr

RADIOACTIVITY 67Kr, 48Ni(2p); analyzed available data; calculated Nilsson levels, partial width, T1/2, two-proton angular correlations.

doi: 10.1103/PhysRevLett.120.212502
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2017WA40      Phys.Rev. C 96, 044307 (2017)

S.M.Wang, N.Michel, W.Nazarewicz, F.R.Xu

Structure and decays of nuclear three-body systems: The Gamow coupled-channel method in Jacobi coordinates

NUCLEAR STRUCTURE 6Be, 6Li, 6He; calculated levels, J, π, decay widths, two-nucleon separation energies and angular densities, S(2n) and two-neutron correlations for 6He. 26O; calculated S(2n), GCC wave function of the g.s. in the Jacobi coordinates, level energies, widths, two-neutron correlations. Gamow shell model (GSM) in the cluster-orbital shell model coordinates, and Gamow coupled-channel (GCC) model in Jacobi coordinates, with the nuclei viewed as a core-plus-two nucleon systems.

doi: 10.1103/PhysRevC.96.044307
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2013WA02      Phys.Rev. C 87, 014311 (2013)

S.M.Wang, J.C.Pei, F.R.Xu

Spectroscopic calculations of cluster nuclei above double shell closures with a new local potential

NUCLEAR STRUCTURE 20,22Ne, 44,46,52,54Ti, 60,62Zn, 136,138Te, 212Po; calculated levels, B(E2), α-decay widths, using binary cluster potential with a new local potential. Comparison with experimental data.

doi: 10.1103/PhysRevC.87.014311
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2012ZH48      J.Phys.:Conf.Ser. 381, 012059 (2012)

S.J.Zheng, S.M.Wang, F.R.Xu

Effect of odd-multipolarity deformations on fission barriers in superheavy nuclei

NUCLEAR STRUCTURE 250No; calculated total Routhian surface energy vs deformation, fission path. 292Og; calculated potential energy surface vs deformation, fission path. 242,244,246,248,250,252,254,256Fm, 248,250,252,254,256,258,260,262No; calculated static energy curves vs β2 deformation.

doi: 10.1088/1742-6596/381/1/012059
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2010XU04      Phys.Rev. C 81, 054319 (2010)

C.Xu, C.Qi, R.J.Liotta, R.Wyss, S.M.Wang, F.R.Xu, D.X.Jiang

Molecular structure of highly excited resonant states in 24Mg and the corresponding 8Be+16O and 12C+12C decays

NUCLEAR REACTIONS 12C(12C, X)24Mg, E not given; calculated excitation energies, J, π, widths, and 8Be+16O decays of 24Mg resonances using cluster model. Comparison with experimental data.

doi: 10.1103/PhysRevC.81.054319
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2006WA24      Phys.Rev. D 74, 057902 (2006)

S.-M.Wang, L.Han, W.-G.Ma, R.-Y.Zhang, Y.Jiang

QCD corrections to the R-parity violating processes p(p-bar)/pp → eμ + X at hadron colliders

NUCLEAR REACTIONS 1H(p, e+μ-X), (p-bar, e+μ-X), E=high; calculated σ, transverse momentum spectra, QCD corrections to the R-parity violating processes.

doi: 10.1103/PhysRevD.74.057902
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1979WA24      Chin.J.Nucl.Phys. 1, 63 (1979)

Wang Xin-Lin, Wang Shu-Mao, Mao Zhen-Lin, Wang Fang-Lin, Cheng Pin-Liu

Deuteron-Induced Reactions on 12C at Bombarding Energy of 9 MeV

NUCLEAR REACTIONS 12C(d, p), (d, α), (d, d), (d, d'), E=9 MeV; measured σ(θ). Optical model, zero-range DWBA, Hauser-Feshbach analyses.


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