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NSR database version of May 30, 2024.

Search: Author = Y.C.Yu

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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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2020LI06      Phys.Rev. C 101, 024305 (2020)

P.F.Liang, L.J.Sun, J.Lee, S.Q.Hou, X.X.Xu, C.J.Lin, C.X.Yuan, J.J.He, Z.H.Li, J.S.Wang, D.X.Wang, H.Y.Wu, Y.Y.Yang, Y.H.Lam, P.Ma, F.F.Duan, 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.Z.Shi, 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.Q.Zhao, H.M.Jia, L.Yang, P.W.Wen, F.Yang, G.L.Zhang, M.Pan, X.Y.Wang, H.H.Sun, Z.G.Hu, R.F.Chen, M.L.Liu, W.Q.Yang, Y.M.Zhao

Simultaneous measurement of β-delayed proton and γ emission of 26P for the 25Al(p, γ)26Si reaction rate

RADIOACTIVITY 26P(β+), (β+p)[from 9Be(32S, X), E=806 MeV/nucleon, followed by in-flight separation by the RIBLL1 fragment separator at HIRFL-Lanzhou]; measured E(p), I(p), Eγ, Iγ, βp- and βγ-coin, half-life of the decay of 26P from correlated events of 26P implants and successive decays using three double-sided silicon strip detectors (DSSDs), five Clover-type HPGe detectors, and five quadrant silicon detectors (Q SDs). 26Si; deduced levels, J, π, Γp and Γγ of 5929, 3+ state. Comparison with previous experimental data, and with shell-model calculations.

NUCLEAR REACTIONS 9Be(32S, X)22Na/23Mg/24Al/25Si/26P, E=806 MeV/nucleon; measured reaction products and TOF-ΔE spectrum using in-flight separation by the RIBLL1 fragment separator at HIRFL-Lanzhou. 25Al(p, γ)26Si, T=0.03-1.1 GK; deduced energies and strengths of resonances, corresponding astrophysical reaction rates, and compared with data in JINA REACLIB database.

doi: 10.1103/PhysRevC.101.024305
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2018YA19      Phys.Rev. C 98, 044608 (2018)

Y.Y.Yang, X.Liu, D.Y.Pang, D.Patel, R.F.Chen, J.S.Wang, P.Ma, J.B.Ma, S.L.Jin, Z.Bai, V.Guimaraes, Q.Wang, W.H.Ma, F.F.Duan, Z.H.Gao, Y.C.Yu, Z.Y.Sun, Z.G.Hu, S.W.Xu, S.T.Wang, D.Yan, Y.Zhou, Y.H.Zhang, X.H.Zhou, H.S.Xu, G.Q.Xiao, W.L.Zhan

Elastic scattering of the proton drip line nuclei 7Be, 8B, and 9C on a lead target at energies around three times the Coulomb barriers

NUCLEAR REACTIONS Pb(7Be, 7Be), E=130 MeV; Pb(8B, 8B), E=178 MeV; Pb(9C, 9C), E=227 MeV; measured scattered particles, elastic scattering σ(θ) using silicon ΔE-E telescopes at RIBLL-HIRFL-Lanzhou accelerator facility. Comparison with continuum discretized coupled channels (CDCC) and optical model calculations.

doi: 10.1103/PhysRevC.98.044608
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0206.


2010HS01      Nucl.Instrum.Methods Phys.Res. B268, 1786 (2010)

J.Y.Hsu, Y.C.Yu, K.M.Chen

Stopping force and straggling of 0.6-4.7 MeV H, He and Li ions in the polyhydroxybutyrate foil

doi: 10.1016/j.nimb.2010.02.074
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1997AZ03      J.Phys.(London) B30, 353 (1997)

A.R.Azordegan, H.L.Sun, Y.C.Yu, J.L.Duggan, F.D.McDaniel, E.K.Lin, C.W.Wang, G.Lapicki

Charge State Dependence of Copper L-Shell X-Ray Production by 4-14 MeV Oxygen Ions

ATOMIC PHYSICS Cu(16O, X), E=4-14 MeV; measured L-shell X-ray production σ; deduced projectile charge state dependence, electron capture contribution.

doi: 10.1088/0953-4075/30/2/026
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1996CH53      Nucl.Instrum.Methods Phys.Res. B118, 408 (1996)

H.S.Cheng, Y.C.Yu, C.W.Wang, E.K.Lin, T.Y.Liu, M.S.Chen, M.S.Chang

Backscattering Studies of 7Li, 12C and 16O Ions at Energies 3-15 MeV

doi: 10.1016/0168-583X(95)01182-X
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1996SU16      Phys.Rev. A53, 4190 (1996)

H.L.Sun, Y.C.Yu, E.K.Lin, C.W.Wang, J.L.Duggan, A.R.Azordegan, F.D.McDaniel, G.Lapicki

Charge-State Dependence of K-Shell X-Ray Production in Aluminum by 2-12 MeV Carbon Ions

NUCLEAR REACTIONS 27Al(C, X), E=2-12 MeV; measured K-shell X-ray production σ; deduced charge state dependence. ECPSSR theory.

ATOMIC PHYSICS 27Al(C, X), E=2-12 MeV; measured K-shell X-ray production σ; deduced charge state dependence. ECPSSR theory.

doi: 10.1103/PhysRevA.53.4190
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1995YU11      Phys.Rev. A52, 3836 (1995)

Y.C.Yu, H.L.Sun, J.L.Duggan, F.D.McDaniel, J.Y.Yin, G.Lapicki

Charge-State Dependence of M-Shell X-Ray Production in 67Ho by 2-12-MeV Carbon Ions

NUCLEAR REACTIONS Ho(12C, X), E=2-12 MeV; measured X-ray production σ; deduced charge state dependence.

ATOMIC PHYSICS Ho(12C, X), E=2-12 MeV; measured X-ray production σ; deduced charge state dependence.

doi: 10.1103/PhysRevA.52.3836
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1994MC10      J.Phys.(London) B27, 5295 (1994)

M.R.McNeir, Y.C.Yu, D.L.Weathers, D.K.Marble, Z.Zhao, J.L.Duggan, F.D.McDaniel, G.Lapicki

L-Shell X-Ray Production Cross Sections in 26Fe, 28Ni, 29Cu, 30Zn, 31Ga and 32Ge by 0.5 to 8.0 MeV He Ions

NUCLEAR REACTIONS Fe, Ni, Cu, Zn, Ga, Ge(α, X), E=0.5-8 MeV; measured L X-ray production σ. Windowless Si(Li) detector. Model comparison.

ATOMIC PHYSICS Fe, Ni, Cu, Zn, Ga, Ge(α, X), E=0.5-8 MeV; measured L X-ray production σ. Windowless Si(Li) detector. Model comparison.

doi: 10.1088/0953-4075/27/21/020
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1994WA11      Nucl.Phys. A570, 363c (1994)

C.W.Wang, E.K.Lin, Y.C.Yu

Nuclear Excitation of 7Li Projectile from 7Li-Ion Bombardment on Thick Cu Target in the Energy Range 4.9-11.9 MeV

NUCLEAR REACTIONS, ICPND Cu(7Li, 7Li'), E=4.9-11.9 MeV; measured Eγ, Iγ, γ yield vs E; deduced 7Li excitation evidence, reaction mechanism.

doi: 10.1016/0375-9474(94)90302-6
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1994YU03      J.Phys.(London) B27, 3967 (1994)

Y.C.Yu, E.K.Lin, C.W.Wang, P.J.Tsai, C.H.Chang

L X-Ray Production in La, Nd, Gd, Er and Lu by 1-5 MeV Protons

NUCLEAR REACTIONS La, Nd, Gd, Er(p, X), E=1-5 MeV; measured L X-ray production σ vs E. Model comparison.

ATOMIC PHYSICS La, Nd, Gd, Er(p, X), E=1-5 MeV; measured L X-ray production σ vs E. Model comparison.

doi: 10.1088/0953-4075/27/17/020
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1993ME16      Nucl.Instrum.Methods Phys.Res. B79, 175 (1993)

R.Mehta, J.L.Duggan, F.D.McDaniel, M.R.McNeir, Y.C.Yu, D.K.Marble, G.Lapicki

L-Shell X-Ray Production Cross Sections for 29Cu, 31Ga, 32Ge, 35Br, 39Y, 60Nd, 64Gd, 67Ho, 70Yb, 79Au, and 82Pb for 2-25 MeV Carbon Ions

NUCLEAR REACTIONS Cu, Ga, Ge, Br, 89Y, Nd, Gd, 165Ho, Yb, 197Au, Pb(C, X), E=2-25 MeV; measured L X-ray production σ; deduced Si(Li) detector efficiency. Multiple normalization techniques.

ATOMIC PHYSICS Cu, Ga, Ge, Br, 89Y, Nd, Gd, 165Ho, Yb, 197Au, Pb(C, X), E=2-25 MeV; measured L X-ray production σ; deduced Si(Li) detector efficiency. Multiple normalization techniques.

doi: 10.1016/0168-583X(93)95318-Y
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1993WA24      Nucl.Instrum.Methods Phys.Res. B79, 190 (1993)

C.W.Wang, E.K.Lin, Y.C.Yu

Atomic K Shell Ionization by 3.0-15 MeV Oxygen Ions for Selected Elements between Ti and In

NUCLEAR REACTIONS Ti, Cu, 89Y, In(O, X), E=3-15 MeV; measured K shell X-ray production σ. Model comparison.

ATOMIC PHYSICS Ti, Cu, 89Y, In(O, X), E=3-15 MeV; measured K shell X-ray production σ. Model comparison.

doi: 10.1016/0168-583X(93)95322-V
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1993YU05      Nucl.Instrum.Methods Phys.Res. B79, 179 (1993)

Y.C.Yu

Charged Particle Innershell Ionization in K-Shell Excitation for Target Binding Energies Less than 1 keV

NUCLEAR REACTIONS C, O, 19F(p, X), (α, X), (7Li, X), E=0.5-5 MeV; measured K X-ray production σ. Windowless Si(Li) detector.

ATOMIC PHYSICS C, O, 19F(p, X), (α, X), (7Li, X), E=0.5-5 MeV; measured K X-ray production σ. Windowless Si(Li) detector.

doi: 10.1016/0168-583X(93)95319-Z
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1993YU06      Nucl.Instrum.Methods Phys.Res. B79, 199 (1993)

Y.C.Yu, C.W.Wang, E.K.Lin

Lithium-7 Ion Induced K X-Ray Production Cross Sections of Ti, Cu, Se, and Ag in the Energy Range 3.0-10.0 MeV

NUCLEAR REACTIONS Ti, Cu, Se, Ag(7Li, X), E=3-10 MeV; measured K X-ray production σ. Model comparison.

ATOMIC PHYSICS Ti, Cu, Se, Ag(7Li, X), E=3-10 MeV; measured K X-ray production σ. Model comparison.

doi: 10.1016/0168-583X(93)95324-X
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1992LI16      Phys.Scr. 46, 522 (1992)

E.K.Lin, C.W.Wang, Y.C.Yu, F.T.Chuang, Y.M.Huang

Cross Sections for K-Shell Ionization of Atoms Induced by 1.5-6.0 MeV 4He Ions

NUCLEAR REACTIONS Ti, 55Mn, 59Co, Ni, Cu, Zn, Ga(α, X), E=1.5-6 MeV; measured K X-ray production σ; deduced K(β)/K(α) X-ray yield ratio. Model comparison.

doi: 10.1088/0031-8949/46/6/006
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1992LI28      J.Phys.(London) B25, 5413 (1992)

E.K.Lin, C.W.Wang, Y.C.Yu, P.K.Teng

Ionization of the Cobalt K Shell by Low-Energy Protons, Deuterons and Helium-3 Ions

NUCLEAR REACTIONS Cr(p, X), (d, X), (3He, X), E=0.7-2 MeV/nucleon; measured K X-ray intensity ratios, production σ(E). Perturbed stationary state with energy loss model analysis.

ATOMIC PHYSICS Cr(p, X), (d, X), (3He, X), E=0.7-2 MeV/nucleon; measured K X-ray intensity ratios, production σ(E). Perturbed stationary state with energy loss model analysis.

doi: 10.1088/0953-4075/25/24/019
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1992WA23      J.Phys.(London) B25, 1385 (1992)

C.W.Wang, Y.C.Yu, E.K.Lin, C.H.Lee, F.T.Chuang

3He Ion-Induced K X-Ray Emission Cross Section of Elements between Mn and Zn

NUCLEAR REACTIONS Mn, Fe, Ni, Cu, Zn(3He, X), E=1.5-6 MeV; measured K X-ray production σ. Model comparison.

ATOMIC PHYSICS Mn, Fe, Ni, Cu, Zn(3He, X), E=1.5-6 MeV; measured K X-ray production σ. Model comparison.

doi: 10.1088/0953-4075/25/7/010
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1992YU03      J.Phys.Soc.Jpn. 61, 1939 (1992)

Y.C.Yu, E.K.Lin, C.W.Wang, Y.M.Huang, C.H.Lee

K-Shell Vacancy Production Cross Sections for Se, Br, Rb and Y Induced by 1.5 to 9.0 MeV 3He Ions

NUCLEAR REACTIONS Se, Br, Rb, 89Y(3He, X), E=1.5-9 MeV; measured K X-ray production σ; deduced I(K(β))/I(K(α)). Model comparison.

ATOMIC PHYSICS Se, Br, Rb, 89Y(3He, X), E=1.5-9 MeV; measured K X-ray production σ; deduced I(K(β))/I(K(α)). Model comparison.


1991MA66      Nucl.Instrum.Methods Phys.Res. B56/57, 33 (1991)

D.K.Marble, F.D.McDaniel, M.R.McNeir, Y.C.Yu, Z.Y.Zhao, D.K.Wilson, D.L.Weathers, J.L.Duggan, R.M.Wheeler, R.P.Chaturvedi, G.Lapicki, V.Zoran

Direct Ionization in K-Shell X-Ray Production in Fluorine by Highly-Charged Lithium, Boron, and Oxygen Ions

NUCLEAR REACTIONS 19F(7Li, X), E=1.5-4 MeV; 19F(10B, X), E=2-10 MeV; 19F(16O, X), E=3-12 MeV; measured K-shell X-ray production σ(E). Solid YF3 target. Model comparison.

ATOMIC PHYSICS 19F(7Li, X), E=1.5-4 MeV; 19F(10B, X), E=2-10 MeV; 19F(16O, X), E=3-12 MeV; measured K-shell X-ray production σ(E). Solid YF3 target. Model comparison.

doi: 10.1016/0168-583X(91)95964-F
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1991MC02      Nucl.Instrum.Methods Phys.Res. B54, 531 (1991)

F.D.McDaniel, D.K.Marble, J.L.Duggan, M.R.McNeir, Y.C.Yu, Z.Y.Zhao, D.L.Weathers, P.S.Elliott, R.M.Wheeler, R.P.Chaturvedi, G.Lapicki

X-Ray Production in Fluorine by Highly Charged Boron, Carbon, and Oxygen Ions

NUCLEAR REACTIONS 19F(B, X), (C, X), E=10 MeV; 19F(O, X), E=8, 10, 12 MeV; measured K X-ray production σ; deduced direct ionization, electron capture contributions.

ATOMIC PHYSICS 19F(B, X), (C, X), E=10 MeV; 19F(O, X), E=8, 10, 12 MeV; measured K X-ray production σ; deduced direct ionization, electron capture contributions.

doi: 10.1016/0168-583X(91)95433-E
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1991MC09      Phys.Rev. A44, 4372 (1991)

M.R.McNeir, Y.C.Yu, D.L.Weathers, J.L.Duggan, F.D.McDaniel, G.Lapicki

L-Shell X-Ray Production Cross Sections in 26Fe, 28Ni, 29Cu, 30Zn, 31Ga, and 32Ge by 0.5- to 5.0-MeV Protons

NUCLEAR REACTIONS Fe, Ni, Cu, Zn, Ga, Ge(p, X), E=0.5-5 MeV; measured L-shell X-ray production σ. Model comparison.

ATOMIC PHYSICS Fe, Ni, Cu, Zn, Ga, Ge(p, X), E=0.5-5 MeV; measured L-shell X-ray production σ. Model comparison.

doi: 10.1103/PhysRevA.44.4372
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1991MC11      Nucl.Instrum.Methods Phys.Res. B56/57, 26 (1991)

M.R.McNeir, Y.C.Yu, D.L.Weathers, D.K.Marble, J.L.Duggan, F.D.McDaniel, G.Lapicki

L-Shell X-Ray Production Cross Sections in 20Ca, 26Fe, 28Ni, 29 and 32Ge by 0.75 to 4.5 MeV 7Li+ Ions

NUCLEAR REACTIONS Ge, Cu, Ni, Fe, Ca(7Li, X), E=0.75-4.5 MeV; measured L-subshell X-ray production σ(E); deduced detector efficiency. Windowless Si(Li), high purity Ge detectors. Model comparison.

ATOMIC PHYSICS Ge, Cu, Ni, Fe, Ca(7Li, X), E=0.75-4.5 MeV; measured L-subshell X-ray production σ(E); deduced detector efficiency. Windowless Si(Li), high purity Ge detectors. Model comparison.

doi: 10.1016/0168-583X(91)95962-D
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1991WE20      Nucl.Instrum.Methods Phys.Res. B56/57, 964 (1991)

D.L.Weathers, J.L.Duggan, M.R.McNeir, Y.C.Yu, F.D.McDaniel, C.A.Quarles, H.Lehtihet, D.Kahler

Efficiency Determination for a Windowless Si(Li) X-Ray Detector for Photon Energies Below 5 keV Using Atomic-Field Bremsstrahlung

NUCLEAR REACTIONS 197Au, Ag, 27Al(γ, X), E=0.6 keV; measured X-ray spectra; deduced detector efficiency. Windowless Si(Li) X-ray detector.

ATOMIC PHYSICS 197Au, Ag, 27Al(γ, X), E=0.6 keV; measured X-ray spectra; deduced detector efficiency. Windowless Si(Li) X-ray detector.

doi: 10.1016/0168-583X(91)95072-L
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1991YU03      Phys.Rev. A44, 5702 (1991)

Y.C.Yu, M.R.McNeir, D.L.Weathers, J.L.Duggan, F.D.McDaniel, G.Lapicki

K-Shell X-Ray-Production Cross Sections in 6C, 8O, 9F, 11Na, 12Mg, and 13Al by 0.75- to 4.5-MeV Protons

NUCLEAR REACTIONS C, O, 19F, 23Na, Mg, 27Al(p, X), E=0.75-4.5 MeV; measured K-Shell X-ray production σ. Model comparison.

ATOMIC PHYSICS C, O, 19F, 23Na, Mg, 27Al(p, X), E=0.75-4.5 MeV; measured K-shell X-ray production σ. Model comparison.

doi: 10.1103/PhysRevA.44.5702
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1991YU04      Nucl.Instrum.Methods Phys.Res. B56/57, 1188 (1991); see 1991Yu06

Y.C.Yu, M.R.McNeir, D.L.Weathers, D.K.Marble, J.L.Duggan, F.D.McDaniel, G.Lapicki

K-Shell X-Ray Production Cross Sections in 6C, 8O, 11Na, 12Mg and 13Al by 0.75 to 5.0 MeV 7Li+ Ions

doi: 10.1016/0168-583X(91)95128-Z
Citations: PlumX Metrics


1991YU05      Phys.Rev. A44, 7252 (1991)

Y.C.Yu, M.R.McNeir, D.L.Weathers, J.L.Duggan, F.D.McDaniel, D.K.Marble, Z.Y.Zhao, G.Lapicki

K-Shell X-Ray Production in 6C, 8O, 9F, 11Na, 12Mg, and 13Al by 0.5-8.0-MeV Helium Ions

NUCLEAR REACTIONS C, O, 19F, 23Na, Mg, 27Al(α, X), E=0.5-8 MeV; measured K-shell X-ray production σ.

ATOMIC PHYSICS C, O, 19F, 23Na, Mg, 27Al(α, X), E=0.5-8 MeV; measured K-shell X-ray production σ.

doi: 10.1103/PhysRevA.44.7252
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1991YU06      Nucl.Instrum.Methods Phys.Res. B56/57, 1188 (1991)

Y.C.Yu, M.R.McNeir, D.L.Weathers, D.K.Marble, J.L.Duggan, F.D.McDaniel, G.Lapicki

K-Shell X-Ray Production Cross Section in 6C, 8O, 11Na, 12Mg and 13Al by 0.75 to 5.0 MeV 7Li+ Ions

NUCLEAR REACTIONS C, O, 23Na, Mg, 27Al(7Li, X), E=0.75-5 MeV; measured K-shell X-ray production σ(E). Analytical windowless Si(Li) detector.

ATOMIC PHYSICS C, O, 23Na, Mg, 27Al(7Li, X), E=0.75-5 MeV; measured K-shell X-ray production σ(E). Analytical windowless Si(Li) detector.

doi: 10.1016/0168-583X(91)95128-Z
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