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NSR database version of April 25, 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, Γ_p and Γ_γ 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
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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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