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NSR database version of April 11, 2024.

Search: Author = J.Lin

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2024LI03      Eur.Phys.J. A 60, 15 (2024)

J.-X.Lin, H.-X.Chen, W.-H.Liang, W.-Y.Liu, D.Zhou

Molecular pentaquark states with open charm and bottom flavors

doi: 10.1140/epja/s10050-024-01240-7
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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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Data from this article have been entered in the XUNDL database. For more information, click here.


2023ZH51      Chin.Phys.C 47, 114102 (2023)

Z.Zhang, Sh.Li, N.Yu, J.Lin, Sh.Li, S.Tang, D.Zhou

Study of neutron density fluctuation and neutron-proton correlation in Au+Au collisions using PYTHIA8/Angantyr

doi: 10.1088/1674-1137/acf65c
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2022LU01      Phys.Rev. C 105, 024305 (2022)

D.W.Luo, C.Xu, Y.K.Wang, Z.H.Li, R.A.Bark, S.Q.Zhang, H.Hua, S.Y.Wang, J.Peng, X.Q.Li, H.Y.Wu, X.Wang, C.G.Wu, Q.T.Li, J.Lin, Y.Jin, W.Z.Xu, L.Mu, J.Meng, F.R.Xu, Y.L.Ye, D.X.Jiang, P.Jones, E.A.Lawrie, P.Papka, M.F.Nkalanga, T.D.Bucher, M.V.Chisapi, L.Msebi, S.Jongile, S.Ntshangase, B.R.Zikhali, S.H.Mthembu, T.Seakamela, M.A.Sithole, O.Shirihda, A.A.Aava, L.Mdletshe, K.L.Malatji, S.Mhlongo, L.Makhathini

Collective structures in 62Cu

NUCLEAR REACTIONS 54Cr(12C, 3np), E=67 MeV; measured Eγ, Iγ, γ(θ), γγ-coin. 62Cu; deduced levels, J, π, high-spin levels, B(M1)/B(E2), configurations, γγ(linear polarization). Comparison with calculations using the self-consistent tilted axis cranking covariant density functional theory (TAC-C DFT). Comparison with level structures in 60,64Ca. AFRODITE array at the iThemba LABS accelerator facility.

doi: 10.1103/PhysRevC.105.024305
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2021AK04      Phys.Rev. C 104, 065501 (2021)

D.S.Akerib, A.K.Al Musalhi, S.K.Alsum, C.S.Amarasinghe, A.Ames, T.J.Anderson, N.Angelides, H.M.Araujo, J.E.Armstrong, M.Arthurs, X.Bai, J.Balajthy, S.Balashov, J.Bang, J.W.Bargemann, D.Bauer, A.Baxter, P.Beltrame, E.P.Bernard, A.Bernstein, A.Bhatti, A.Biekert, T.P.Biesiadzinski, H.J.Birch, G.M.Blockinger, E.Bodnia, B.Boxer, C.A.J.Brew, P.Bras, S.Burdin, J.K.Busenitz, M.Buuck, R.Cabrita, M.C.Carmona-Benitez, M.Cascella, C.Chan, N.I.Chott, A.Cole, M.V.Converse, A.Cottle, G.Cox, O.Creaner, J.E.Cutter, C.E.Dahl, L.de Viveiros, J.E.Y.Dobson, E.Druszkiewicz, S.R.Eriksen, A.Fan, S.Fayer, N.M.Fearon, S.Fiorucci, H.Flaecher, E.D.Fraser, T.Fruth, R.J.Gaitskell, J.Genovesi, C.Ghag, E.Gibson, S.Gokhale, M.G.D.van der Grinten, C.B.Gwilliam, C.R.Hall, S.J.Haselschwardt, S.A.Hertel, M.Horn, D.Q.Huang, M.C.I.gnarra, O.Jahangir, R.S.James, W.Ji, J.Johnson, A.C.Kaboth, A.C.Kamaha, K.Kamdin, K.Kazkaz, D.Khaitan, A.Khazov, I.Khurana, D.Kodroff, L.Korley, E.V.Korolkova, H.Kraus, S.Kravitz, L.Kreczko, B.Krikler, V.A.Kudryavtsev, E.A.Leason, J.Lee, D.S.Leonard, K.T.Lesko, C.Levy, J.Liao, J.Lin, A.Lindote, R.Linehan, W.H.Lippincott, X.Liu, M.I.Lopes, E.Lopez Asamar, B.Lopez Paredes, W.Lorenzon, S.Luitz, P.A.Majewski, A.Manalaysay, L.Manenti, R.L.Mannino, N.Marangou, M.E.McCarthy, D.N.McKinsey, J.McLaughlin, E.H.Miller, E.Mizrachi, A.Monte, M.E.Monzani, J.A.Morad, J.D.Morales Mendoza, E.Morrison, B.J.Mount, A.St.J.Murphy, D.Naim, A.Naylor, C.Nedlik, H.N.Nelson, F.Neves, J.A.Nikoleyczik, A.Nilima, I.Olcina, K.C.Oliver-Mallory, S.Pal, K.J.Palladino, J.Palmer, S.Patton, N.Parveen, E.K.Pease, B.Penning, G.Pereira, A.Piepke, Y.Qie, J.Reichenbacher, C.A.Rhyne, A.Richards, Q.Riffard, G.R.C.Rischbieter, R.Rosero, P.Rossiter, D.Santone, A.B.M.R.Sazzad, R.W.Schnee, P.R.Scovell, S.Shaw, T.A.Shutt, J.J.Silk, C.Silva, R.Smith, M.Solmaz, V.N.Solovov, P.Sorensen, J.Soria, I.Stancu, A.Stevens, K.Stifter, B.Suerfu, T.J.Sumner, N.Swanson, M.Szydagis, W.C.Taylor, R.Taylor, D.J.Temples, P.A.Terman, D.R.Tiedt, M.Timalsina, W.H.To, D.R.Tovey, M.Tripathi, D.R.Tronstad, W.Turner, U.Utku, A.Vaitkus, B.Wang, J.J.Wang, W.Wang, J.R.Watson, R.C.Webb, R.G.White, T.J.Whitis, M.Williams, F.L.H.Wolfs, D.Woodward, C.J.Wright, X.Xiang, J.Xu, M.Yeh, P.Zarzhitsky

Projected sensitivity of the LUX-ZEPLIN experiment to the two-neutrino and neutrinoless double β decays of 134Xe

RADIOACTIVITY 134Xe(2β-); measured recoiling nuclei and electrons, decay energy spectra using LUX-ZEPLIN (LZ) detector of liquid xenon (LXe), with scintillation and electro-luminescence light detected using 494 photomultipliers at Sanford Underground Research Facility (SURF) in South Dakota; deduced lower limits of T1/2 values for 2νββ and 0νββ decay modes.

doi: 10.1103/PhysRevC.104.065501
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2020WA16      Nucl.Instrum.Methods Phys.Res. A971, 164068 (2020)

X.Wang, Z.H.Li, Z.Liu, J.Li, H.Hua, H.Y.Lu, W.Q.Zhang, T.H.Huang, M.D.Sun, J.G.Wang, X.Y.Liu, B.Ding, Z.G.Gan, L.Ma, H.B.Yang, Z.Y.Zhang, L.Yu, J.Jiang, K.L.Wang, Y.S.Wang, M.L.Liu, C.J.Lin, L.J.Sun, N.R.Ma, H.S.Xu, X.H.Zhou, G.Q.Xiao, H.Y.Wu, C.Xu, S.Q.Zhang, X.Q.Li, R.Han, Z.Q.Chen, C.G.Wu, D.W.Luo, Y.Jin, J.Lin, D.X.Jiang, Y.L.Ye, F.S.Zhang

An effective digital pulse processing method for pile-up pulses in decay studies of short-lived nuclei

RADIOACTIVITY 219Th(α), 210,211Ra(IT) [from 175Lu, 186W, 187Re(40Ar, X), E=188 MeV]; measured decay products, Eα, Iα; deduced α spectra, proper baseline correction, standard pulse construction and plateau-region fitting, spectroscopic information of overlapping signals.

doi: 10.1016/j.nima.2020.164068
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2014LI43      Nucl.Data Sheets 118, 588 (2014)

R.Liu, T.H.Zhu, X.S.Yan, X.X.Lu, L.Jiang, M.Wang, Z.J.Han, Z.W.Wen, J.F.Lin, Y.W.Yang

Progress of Integral Experiments in Benchmark Fission Assemblies for a Blanket of Hybrid Reactor

doi: 10.1016/j.nds.2014.04.143
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1995JI14      Chin.J.Nucl.Phys. 17, No 3, 223 (1995)

D.-X.Jiang, X.Qian, T.Qian, H.Hua, J.-S.Lin, E.-J.Wu, J.-W.Zheng, G.-M.Jing, S.-Z.Yin, J.-L.Tan, W.-Y.Jing, M.-T.Song, Z.-Y.Li, Z.-Y.He

Emission of Intermediate-mass Fragments from Hot-Nuclei Produced in the Reaction 40Ar - (nat)Ag at 25 MeV/u

NUCLEAR REACTIONS Ag(40Ar, X), E=25 MeV/nucleon; measured intermediate mass fragment σ(θ), energy spectra for Li-F. Thermal model analysis.


1995QI03      Chin.J.Nucl.Phys. 17, No 2, 118 (1995)

X.Qian, D.-X.Jiang, J.-S.Lin, D.-M.Liu, Z.Li

Average Angular Momentum for the 12C + 93Nb System at Near-and Sub-Barrier Energies

NUCLEAR REACTIONS, ICPND 93Nb(12C, 2n), (12C, 3n), E(cm)=25-40.5 MeV; calculated residuals production σ(E); deduced fusion σ(E). Statistical evaporation model.


1985LE10      Phys.Rev. C32, 277 (1985)

R.S.Lee, J.H.Hamilton, A.V.Ramayya, A.P.de Lima, D.L.Sastry, K.S.R.Sastry, E.H.Spejewski, R.L.Mlekodaj, H.K.Carter, W.-D.Schmidt-Ott, J.Lin, C.R.Bingham, L.L.Riedinger, E.F.Zganjar, J.L.Weil, B.D.Kern, A.C.Xenoulis, R.W.Fink, Sun Xi-jun, Guo Jun-sheng, Cho Chi-cheng, Pan Zong-you, Guo Ying-xian

Decay of 117Xe → 117I → 117Te

NUCLEAR REACTIONS 107,109Ag(12C, xn), E=50-70 MeV; measured γ yields. 117I deduced transition.

RADIOACTIVITY 117Xe(EC), (β+) [from 104Pd(16O, xn), E=86 MeV]; 117I(EC), (β+) [from 117Xe β-decay]; 117Te(β+), (EC) [from 117I β-decay]; measured Eγ, Iγ, E X-ray, I X-ray, T1/2, γγ-coin. 117I, 117Te deduced levels, relative Iγ. 117Sb(EC), (β+) [from 117Te decay]; measured T1/2. 117Xe, 117I deduced mass difference, Q(EC).

doi: 10.1103/PhysRevC.32.277
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1985PI08      Phys.Rev. C32, 625 (1985)

R.B.Piercey, A.C.Rester, J.H.Hamilton, A.V.Ramayya, H.K.Carter, R.L.Robinson, H.J.Kim, J.C.Wells, J.Lin

Near-Spherical Band in 76Kr Observed in the β Decay of Mass Separated 76Rb

RADIOACTIVITY 76Rb(β+) [from Ni(20Ne, xn), E=112 MeV]; measured Eγ, Iγ, γγ-coin. 76Kr deduced levels, J, π, γ-branching.

NUCLEAR REACTIONS Ni(20Ne, xn), E=112 MeV; measured Eγ, Iγ, γγ-coin following 76Rb β+-decay. 76Kr deduced levels, J, π, γ-branching.

doi: 10.1103/PhysRevC.32.625
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1984ME04      Phys.Rev. C29, 1839 (1984)

R.A.Meyer, J.Lin, G.Molnar, B.Fazekas, A.Veres, M.Sambataro

Influence of Cross Subshell Excitations on the Collective States of 98Mo Observed by β Decay and (n, n'γ) Reaction Spectroscopy

RADIOACTIVITY 98mNb(β-) [from 98Mo(n, p), E=14 MeV]; measured Eγ, Iγ, γγ(t), γγ-coin; deduced log ft. 98Mo deduced levels, J, π, γ-branching, Iβ, absolute Iγ, δ. Compton suppression.

NUCLEAR REACTIONS 98Mo(n, n'γ), E=14 MeV; measured γ(θ), Eγ, Iγ, γγ-coin, γγ(θ). 98Mo deduced levels, δ, J, π. Enriched target.

NUCLEAR STRUCTURE 98Mo; calculated levels, γ-branching ratios, cross subshell excitations. Interacting boson model.

doi: 10.1103/PhysRevC.29.1839
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1983KE08      Phys.Rev. C28, 2168 (1983)

B.D.Kern, K.S.Toth, D.M.Moltz, J.Lin, F.T.Avignone III, H.Noma, G.A.Leander

Beta Decay of 75Rb to Low-Lying Levels in 75Kr

RADIOACTIVITY 75Rb(β+) [from 58Ni(20Ne, p2n)]; measured T1/2, Eγ, Iγ, γγ-coin. 75Kr deduced levels, J, π. Mass separated samples.

doi: 10.1103/PhysRevC.28.2168
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1983KO01      Phys.Rev. C27, 158 (1983)

R.L.Kozub, J.Lin, J.F.Mateja, C.J.Lister, D.J.Millener, J.W.Olness, E.K.Warburton

Lifetimes of Levels in 20,21F, 22Ne, and 16N

NUCLEAR REACTIONS 7Li(18O, α), (18O, nα), (18O, t), E=10-60 MeV; 7Li(11B, np), E=7-35 MeV; measured Eγ, Iγ, recoil. 21F, 22Ne levels deduced T1/2. 16N, 20F levels deduced T1/2, B(λ). Shell model.

doi: 10.1103/PhysRevC.27.158
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1982LI09      Radiochem.Radioanal.Lett. 50, 399 (1982)

J.Lin, K.Rengan, R.A.Meyer

Ground-State Decay Branchings for 85,86,87,88Se Isotopes with a Gas-Phase Rapid Chemistry System

RADIOACTIVITY 85,86,87,88Se [from fission]; measured Eγ, Iγ following β-decay. 85,86,87,88Br, 85,86,87,88Kr levels deduced γ-branching, absolute Iγ.


1982RE08      Nucl.Instrum.Methods 197, 427 (1982)

K.Rengan, J.Lin, M.Zendel, R.A.Meyer

On-Line System for the Isolation and Study of 0.5 to 30 Second Selenium Fission Products with Simulataneous Suppression of Daughter Bromine Activity

RADIOACTIVITY 85,86,87,88,89Se [from 235U(n, F)]; measured Eγ, Iγ, T1/2. 89Se deduced transition. On-line, fast gas jet systems.

doi: 10.1016/0167-5087(82)90338-6
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1982RE10      Radiochem.Radioanal.Lett. 51, 339 (1982)

K.Rengan, J.Lin, R.A.Meyer

Measurement of Yields of Fission Products with Half Lives of 1 to 30 Sec by Continuous Chemistry Techniques

RADIOACTIVITY 85,86,87,88Se [from fission]; measured Eγ, Iγ; deduced cumulative yields. Gas jet system.


1981HS04      Phys.Rev. C24, 523 (1981)

S.S.Hsu, J.T.Lin, C.M.Yang, Y.W.Yu

Yields and Isomeric Ratio of Xenon and Krypton Isotopes from Thermal Neutron Fission of 235U

NUCLEAR REACTIONS, Fission 235U(n, F), E=thermal; measured cumulative yield for 85m,87,88Kr, 133,135m,135Xe, independent, isomeric yield ratios for 133m,133,135m,135Xe. Activation technique.

doi: 10.1103/PhysRevC.24.523
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30666.


1981KO08      Phys.Rev. C23, 1571 (1981)

R.L.Kozub, J.Lin, J.F.Mateja, C.J.Lister, D.J.Millener, E.K.Warburton

Electromagnetic Transitions in 14C and 14N

NUCLEAR REACTIONS 7Li(9Be, pn), E=5.5 MeV; 9Be(7Li, pn), (7Li, 2n), E=3.8-7.8 MeV; measured Eγ, Iγ, recoil. 14C, 14N levels deduced T1/2. Shell model, SU(3) basis.

NUCLEAR STRUCTURE 14C, 14N; calculated levels, B(λ), δ, Γγ, T1/2, γ-branching. Shell model, SU(3) basis.

doi: 10.1103/PhysRevC.23.1571
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1981PI12      Phys.Rev.Lett. 47, 1514 (1981)

R.B.Piercey, J.H.Hamilton, R.Soundranayagam, A.V.Ramayya, C.F.Maguire, X.-J.Sun, Z.Z.Zhao, R.L.Robinson, H.J.Kim, S.Frauendorf, J.Doring, L.Funke, G.Winter, J.Roth, L.Cleemann, J.Eberth, W.Neumann, J.C.Wells, J.Lin, A.C.Rester, H.K.Carter

Evidence for Deformed Ground States in Light Kr Isotopes

RADIOACTIVITY 76Rb [from Ni(20Ne, xn), E=112 MeV]; measured γγ-coin. 76Kr deduced levels.

NUCLEAR REACTIONS 60Ni(16O, 2n), E=45 MeV; 66Zn(12C, 2n), E=39 MeV; 58Ni(19F, 2np), E=68 MeV; measured DSA, in-beam γ-spectroscopy. 74,76Kr deduced levels, yrast cascade B(E2), moments of inertia, shape coexistence. 76Kr levels deduced T1/2.

doi: 10.1103/PhysRevLett.47.1514
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1977SC03      Phys.Lett. 66B, 133 (1977)

A.G.Schmidt, R.L.Mlekodaj, E.L.Robinson, F.T.Avignone, J.Lin, G.M.Gowdy, J.L.Wood, R.W.Fink

New Isomers of 185,187Tl and the Departure of the h9/2 Intruder State

doi: 10.1016/0370-2693(77)90158-7
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1976BI09      Phys.Rev. C14, 1586 (1976)

C.R.Bingham, L.L.Riedinger, F.E.Turner, B.D.Kern, J.L.Weil, K.J.Hofstetter, J.Lin, E.F.Zganjar, A.V.Ramayya, J.H.Hamilton, J.L.Wood, G.M.Gowdy, R.W.Fink, E.H.Spejewski, W.D.Schmidt-Ott, R.L.Mlekodaj, H.K.Carter, K.S.R.Sastry

Decay of Mass-Separated 190Tl and 190Hg

RADIOACTIVITY 190,190mTl, 190Hg [from Ta, W(16O, X)]; measured Eγ, Iγ, I(ce), Eβ, γX-ray-coin, γγ-coin, T1/2; deduced log ft, Q, ICC. 190Hg, 190Au deduced levels, J, π, λ.

doi: 10.1103/PhysRevC.14.1586
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1976CO24      Phys.Rev.Lett. 37, 1185 (1976)

J.D.Cole, J.H.Hamilton, A.V.Ramayya, W.G.Nettles, H.Kawakami, E.H.Spejewski, M.A.Ijaz, K.S.Toth, E.L.Robinson, K.S.R.Sastry, J.Lin, F.T.Avignone, W.H.Brantley, P.V.G.Rao

Behavior of the Excited Deformed Band and Search for Shape Isomerism in 184Hg

RADIOACTIVITY 184Tl [from 180W+14N]; measured Eγ, Iγ, Eα, Iα, γce-, γγ-coin, γ(t), T1/2. 184Hg deduced levels, J, π, λ, T1/2.

doi: 10.1103/PhysRevLett.37.1185
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1976GO02      Phys.Rev. C13, 1601 (1976)

G.M.Gowdy, A.C.Xenoulis, J.L.Wood, K.R.Baker, R.W.Fink, J.L.Weil, B.D.Kern, K.J.Hofstetter, E.H.Spejewski, R.L.Mlekodaj, H.K.Carter, W.D.Schmidt-Ott, J.Lin, C.R.Bingham, L.L.Riedinger, E.F.Zganjar, K.S.R.Sastry, A.V.Ramayya, J.H.Hamilton

On-Line Mass Separator Investigation of the New Isotope 2.9-sec 116I

RADIOACTIVITY 116I, 116Xe; measured Eγ, Iγ, T1/2, βγ(t); deduced Q, log ft. 116I deduced J, π. 116Te, 116Xe deduced levels, J, π.

doi: 10.1103/PhysRevC.13.1601
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1976IJ01      Phys.Rev. C14, 264 (1976); Erratum Phys.Rev. C14, 2346 (1976)

M.A.Ijaz, J.Lin, E.L.Robinson, K.S.Toth

α Decay of 186Tl

RADIOACTIVITY 186Tl; measured T1/2, Eα, Iα, Eγ, Iγ; deduced α-branching. 183,184,185,186Hg; measured Eα. α decay systematics for 100 ≤ n ≤ 114.

doi: 10.1103/PhysRevC.14.264
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1976RA26      Phys.Rev. C14, 1381 (1976)

S.Raman, R.L.Auble, J.B.Ball, E.Newman, J.C.Wells, Jr., J.Lin

Levels in 144Nd from the 143Nd(d, p) and 146Nd(p, t) Reactions

NUCLEAR REACTIONS 143Nd(d, p), E=25 MeV; measured σ(θ). 146Nd(p, t), E=31 MeV; measured σ(θ). 144Nd deduced levels, L, S. DWBA analysis.

doi: 10.1103/PhysRevC.14.1381
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1976RO06      Phys.Rev. C13, 1922 (1976)

R.L.Robinson, H.J.Kim, J.B.McGrory, G.J.Smith, W.T.Milner, R.O.Sayer, J.C.Wells, Jr., J.Lin

High-Spin States in 42Ca

NUCLEAR REACTIONS 28Si(16O, 2p), E=36-42 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ), γ(θ). 42Ca deduced levels, J, π, δ, γ-branching, B(E2).

doi: 10.1103/PhysRevC.13.1922
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1976TO06      Phys.Lett. 63B, 150 (1976)

K.S.Toth, M.A.Ijaz, J.Lin, E.L.Robinson, B.O.Hannah, E.H.Spejewski, J.D.Cole, J.H.Hamilton, A.V.Ramayya

Observation of α-Decay in Thallium Nuclei, Including the New Isotopes 184Tl and 185Tl

RADIOACTIVITY 184,185,186,187Tl; measured Eα, T1/2. 184,186Tl deduced α-branching.

doi: 10.1016/0370-2693(76)90636-5
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1974HA10      Izv.Akad.Nauk SSSR, Ser.Fiz. 38, 2036 (1974); Bull.Acad.Sci.USSR, Phys.Ser. 38, No.10, 22 (1974)

J.H.Hamilton, E.H.Spejewski, R.L.Mlekodaj, W.-D.Schmidt-Ott, R.W.Fink, A.Xenoulis, K.R.Baker, J.L.Wood, G.Gowdy, H.K.Carter, B.D.Kern, K.J.Hofstetter, J.L.Weil, E.F.Zganjar, K.S.R.Sastry, F.T.Avignone, C.R.Bingham, L.L.Riedinger, L.Harwood, F.Turner, I.A.Sellin, D.J.Pegg, J.Lin, A.V.Ramayya, S.Lee, G.Garcia-Bermudez, E.Bosworth, K.S.Toth, N.R.Johnson

Initial UNISOR Research: New Isotopes 186Tl, 188Tl, 116I; Decays of 189,190Tl, 117Xe, and 117I; and Off-Line Atomic and Nuclear Studies

RADIOACTIVITY 116,117Xe, 116,117I, 186,188,189,190Tl; measured T1/2, Eγ, Iγ, γγ, Eβ; deduced Q(β). 126I measured γγ(θ, H). 117I, 116Te, 188,190Hg deduced levels, J, π. 126Xe level deduced g. On-line isotope separator UNISOR.


1973CA03      Priv.Comm. (February 1973)

H.K.Carter, F.K.Wohn, W.L.Talbert, Jr., J.R.McConnell, J.Lin


1973CO19      Phys.Lett. 45B, 321 (1973)

W.R.Coker, J.Lin, J.L.Duggan, P.D.Miller

Multistep Contributions to 11B(h, α)10B from 8.0 to 12.0 MeV

NUCLEAR REACTIONS 11B(3He, α), E=8.0, 10.0, 12.0 MeV; measured σ(θ). 10B level deduced S.

doi: 10.1016/0370-2693(73)90044-0
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0447.


1973WU01      Nucl.Phys. A199, 23 (1973)

R.R.Wu, R.L.Dangle, M.M.Duncan, J.L.Duggan, P.D.Miller, Jung Lin

A Study of the 11B(3He, p)13C Reaction at 12, 10, 8, 6 and 4 MeV

NUCLEAR REACTIONS 11B(3He, p), E=4, 6, 8, 10, 12 MeV; measured σ(θ). Enriched target.

doi: 10.1016/0375-9474(73)90331-X
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1971CO14      Nucl.Phys. A168, 307 (1971)

W.R.Coker, P.D.Miller, J.L.Duggan, M.M.Duncan, R.L.Dangle, J.Lin

The 14C(t, α0)13C Reaction at 6.0, 8.0 and 10.0 MeV

NUCLEAR REACTIONS 14C(3He, α), 14C(3He, 3He), E=6.0, 8.0, 10.0 MeV; 13C(α, α), E=15, 18, 20 MeV; measured σ(θ); deduced optical model parameters. Enriched targets.

doi: 10.1016/0375-9474(71)90795-0
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1970DU07      Nucl.Phys. A151, 107 (1970)

J.L.Duggan, J.Y.Park, S.D.Danielopoulos, P.D.Miller, J.Lin, M.M.Duncan, R.L.Dangle

3He Elastic Scattering from 10B and 14C in the Range 4 to 18 MeV

NUCLEAR REACTIONS 10B(3He, 3He)10B, 14C(3He, 3He)14C, E = 4-18 MeV; measured σ(E;θ); deduced optical potential parameters.

doi: 10.1016/0375-9474(70)90971-1
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1970TA01      Phys.Rev. C2, 160 (1970)

S.Tanaka, P.H.Stelson, W.T.Bass, J.Lin

Levels in 53Mn, 58Co, 63Zn, and 70Ga from the (p, n) Reaction

NUCLEAR REACTIONS 53Cr, 58Fe, 63Cu, 70Zn(p, n), E=2.74-6.35 MeV; measured σ(E;En). 53Mn, 58Co, 63Zn, 70Ga deduced levels.

doi: 10.1103/PhysRevC.2.160
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1969MI15      Nucl.Phys. A136, 229 (1969)

P.D.Miller, J.L.Duggan, M.M.Duncan, R.L.Dangle, W.R.Coker, J.Lin

11B(3He, d)12C Spectroscopic Factors

NUCLEAR REACTIONS 11B(3He, d), (3He, 3He); E = 10, 12, 18 MeV; measured σ(Ed, θ). 12C levels deduced S. Enriched target.

doi: 10.1016/0375-9474(69)90050-5
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1963WE15      Bull.Am.Phys.Soc.Southeastern Section, p.18, S7, (November 1963); Bull.Am.Phys.Soc. 9 No.3, 351, S7 (1963)

V.N.Webb, M.M.Duncan, J.Lin, J.L.Duggan, L.E.Akers, H.E.Banta

The C14(He3, p)N16, C14(He3, d)N15 and C14(He3, α)C13 Reactions

NUCLEAR STRUCTURE 14C; measured not abstracted; deduced nuclear properties.


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Note: The following list of authors and aliases matches the search parameter J.Lin: , J.C.LIN, J.F.LIN, J.S.LIN, J.T.LIN, J.X.LIN