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NSR database version of April 27, 2024.

Search: Author = C.L.Wu

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2014CU01      Phys.Rev. C 90, 014321 (2014)

J.-W.Cui, X.-R.Zhou, F.-Q.Chen, Y.Sun, C.-L.Wu, Z.-C.Gao

Description of collective and quasiparticle excitations in deformed actinide nuclei: The first application of the multishell shell model for heavy nuclei

NUCLEAR STRUCTURE ^230,232Th, ^232,234,236U, ²⁴⁰Pu; calculated levels, J, π, ground-, β-, γ-, and K=0 to K=7 bands, 2-quasiparticle configurations, B(E2), staggering parameter. Heavy shell model (HSM), an extension of projected shell model (PSM). Comparison with experimental data.

doi: 10.1103/PhysRevC.90.014321
Citations: PlumX Metrics

2012CU01      Chin.Phys.Lett. 29, 022101 (2012)

J.-W.Cui, X.-R.Zhou, F.-Q.Chen, Y.Sun, C.-L.Wu

Analyses of β-Bands of ^{230, 232}Th and ^{232, 234}U by the Projected Shell Model

NUCLEAR STRUCTURE ^230,232Th, ^232,234U; calculated ground and β-bands, deformation parameters, energy schemes. Projected shell model, comparison with experimental data.

doi: 10.1088/0256-307X/29/2/022101
Citations: PlumX Metrics

2008SU25      Int.J.Mod.Phys. E17, Supplement 1, 159 (2008)

Y.Sun, C.-Li.Wu

Multi-major-shell shell model for heavy nuclei - an extended projected shell model

NUCLEAR STRUCTURE ¹⁷⁸Hf; calculated rotational bands, B(E2), J, π.deduced low-energy collective vibrations.

doi: 10.1142/S0218301308011835
Citations: PlumX Metrics

2003SU11      Phys.Rev. C 68, 024315 (2003)

Y.Sun, C.-L.Wu

Multishell shell model for heavy nuclei

doi: 10.1103/PhysRevC.68.024315
Citations: PlumX Metrics

2002LE09      Phys.Rev. C65, 041301 (2002)

C.-T.Lee, Y.Sun, J.-Y.Zhang, M.Guidry, C.-L.Wu

Microscopic Description of Band Structure at Very Extended Shapes in the A ∼ 110 Mass Region

NUCLEAR STRUCTURE ¹⁰⁸Cd; calculated rotational bands energy vs spin, transition quadrupole moments, g factors. Projected shell model, comparison with data.

doi: 10.1103/PhysRevC.65.041301
Citations: PlumX Metrics

2002SU06      Nucl.Phys. A703, 130 (2002)

Y.Sun, C.-L.Wu, K.Bhatt, M.Guidry

SU(3) Symmetry and Scissors Mode Vibrations in Nuclei

NUCLEAR STRUCTURE ¹⁶⁸Er; calculated rotational bands energy vs spin, transitions B(E2); deduced SU(3) symmetry, scissors mode vibrations. Extended projected shell model.

doi: 10.1016/S0375-9474(01)01457-9
Citations: PlumX Metrics

2000PA50      J.Phys.(London) G26, 1569 (2000)

S.K.Patra, C.-L.Wu, W.Greiner, R.K.Gupta

α-Decay Chain of the ²⁸⁹114 Nucleus

NUCLEAR STRUCTURE ²⁸⁹Fl, ²⁸⁵Cn, ²⁸¹Ds, ²⁷⁷Hs, ²⁷³Sg, ²⁶⁹Rf, ²⁶⁵No, ²⁶¹Fm; calculated quadrupole deformation, binding energies, Qα, α-decay T_1/2. Fermion dynamical symmetry model, deformed relativistic mean field, other models compared.

doi: 10.1088/0954-3899/26/10/310
Citations: PlumX Metrics

1999HA56      At.Data Nucl.Data Tables 73, 43 (1999)

X.-L.Han, C.L.Wu

Nuclear Superdeformation Data Tables

COMPILATION ⁵⁸Cu, ^60,62Zn, ^80,81,82,83Sr, ⁸²Y, ^83,84,86Zr, ⁸⁷Nb, ¹³⁰La, ^{129,130,131,132,133}Ce, ^{130,131,132,133}Pr, ^{132,133,134,135,136,137}Nd, ^133,136Pm, ^{133,135,136,137,142,145}Sm, ^{142,143,144,147,148}Eu, ^{139,144,145,146,147,148,149,150}Gd, ^{145,147,149,150,151,152}Tb, ^{151,152,153,154,155}Dy, ¹⁵³Ho, ¹⁵⁴Er, ^163,165,167Lu, ¹⁹¹Au, ^{189,190,191,192,193,194,195}Hg, ^{189,191,192,193,194,195}Tl, ^{192,193,194,195,196,197,198}Pb, ^195,196,197Bi, ¹⁹⁸Po; compiled, analyzed superdeformed bands transitions, moments of inertia, transition quadrupole moments.

doi: 10.1006/adnd.1999.0817
Citations: PlumX Metrics

1999PA11      J.Phys.(London) G25, 501 (1999)

S.K.Patra, C.-L.Wu, C.R.Praharaj, G.K.Khamari

Oscillations in Deformation Properties of Heavy Rare-Earth Nuclei

NUCLEAR STRUCTURE Yb, Hf; calculated binding energy, deformation parameters, charge radii for A=160-230. Relativistic mean-field theory.

doi: 10.1088/0954-3899/25/3/003
Citations: PlumX Metrics

1999PA21      Nucl.Phys. A651, 117 (1999)

S.K.Patra, C.-L.Wu, C.R.Praharaj, R.K.Gupta

A Systematic Study of Superheavy Nuclei for Z = 114 and Beyond using the Relativistic Mean Field Approach

NUCLEAR STRUCTURE ^{268,272,274,276,278,282,286,290,294,298,302,306,310,314}Fl, ³⁰⁰Lv, ³⁰²Og, ^{286,290,292,294,296,298,300,302,304,306,308,310,312,314,316,318,320,322}120, ³⁰⁶122, ³⁰⁸124, ³¹⁰126; calculated binding energies, deformations, single particle levels for some nuclides; deduced shell features. Relativistic mean field theory.

doi: 10.1016/S0375-9474(99)00129-3
Citations: PlumX Metrics

1999SU10      Phys.Rev.Lett. 83, 686 (1999)

Y.Sun, J.-Y.Zhang, M.Guidry, C.-L.Wu

Theoretical Constraints for Observation of Superdeformed Bands in the Mass-60 Region

NUCLEAR STRUCTURE ^60,62,64,66Zn; calculated superdeformed bands transition energies, moments of inertia; deduced role of pair alignment. Projected shell model.

doi: 10.1103/PhysRevLett.83.686
Citations: PlumX Metrics

1998CH32      Phys.Rev. C58, 2133 (1998)

H.-Y.Chang, S.K.Patra, C.-L.Wu

Coefficients of Fractional Parentage in the k-i Basis Shell Model

doi: 10.1103/PhysRevC.58.2133
Citations: PlumX Metrics

1998LE04      Phys.Rev. C57, 637 (1998)

M.-T.Lee, W.-M.Zhang, C.-L.Wu

Influence of Dynamical Pauli Effect and Dynamical Symmetry Breaking on Quantum Chaos

doi: 10.1103/PhysRevC.57.637
Citations: PlumX Metrics

1998PA46      Mod.Phys.Lett. A 13, 2743 (1998)

S.K.Patra, C.-L.Wu, C.R.Praharaj

Proton-Skin in ⁸B-Nucleus

NUCLEAR STRUCTURE ⁷Be, ^8,9,10B; calculated single-particle levels, radii, quadrupole moments, deformations. ⁸B deduced thick proton-skin. Relativistic mean-field approach.

doi: 10.1142/S0217732398002916
Citations: PlumX Metrics

1998SU02      Phys.Rev.Lett. 80, 672 (1998)

Y.Sun, C.-L.Wu, K.Bhatt, M.Guidry, D.H.Feng

Scissors-Mode Vibrations and the Emergence of SU(3) Symmetry from the Projected Deformed Mean Field

NUCLEAR STRUCTURE ¹⁶⁸Er; calculated levels, J, π; deduced 1⁺ band collective scissors mode characterization. Nilsson+BCS, exact angular momentum projection.

doi: 10.1103/PhysRevLett.80.672
Citations: PlumX Metrics

1996CH08      Phys.Lett. 366B, 1 (1996)

H.-T.Chen, C.L.Wu, D.H.Feng, A.Arima

The Quadrupole-Quadrupole Interaction and the Inverted Pairing

doi: 10.1016/0370-2693(95)01322-9
Citations: PlumX Metrics

1996GU10      J.Phys.(London) G22, 425 (1996)

M.W.Guidry, D.H.Feng, X.-W.Pan, C.-L.Wu

Solution of the Nuclear Shell Model by Symmetry-Dictated Truncation

doi: 10.1088/0954-3899/22/4/004
Citations: PlumX Metrics

1996HA18      At.Data Nucl.Data Tables 63, 117 (1996)

X.-L.Han, C.-L.Wu

Nuclear Superdeformation Data Tables

NUCLEAR STRUCTURE ^83,82Sr, ¹³⁰La, ^131,132,133Ce, ¹³³Pr, ^{133,134,135,136,137}Nd, ^135,137,142Sm, ^144,143,142Eu, ^{139,144,146,147,148,149,150}Gd, ^150,151,152Tb, ^{151,152,153,154}Dy, ¹⁹¹Au, ^{189,190,191,192,193,194}Hg, ^{191,192,193,194,195}Tl, ^{192,193,194,195,196,198}Pb, ¹⁹⁷Bi; compiled superdeformed features related data.

COMPILATION ^83,82Sr, ¹³⁰La, ^131,132,133Ce, ¹³³Pr, ^{133,134,135,136,137}Nd, ^135,137,142Sm, ^144,143,142Eu, ^{139,144,146,147,148,149,150}Gd, ^150,151,152Tb, ^{151,152,153,154}Dy, ¹⁹¹Au, ^{189,190,191,192,193,194}Hg, ^{191,192,193,194,195}Tl, ^{192,193,194,195,196,198}Pb, ¹⁹⁷Bi; compiled superdeformed features related data.

doi: 10.1006/adnd.1996.0011
Citations: PlumX Metrics

1996PA03      Phys.Rev. C53, 715 (1996)

X.-W.Pan, J.-L.Ping, D.H.Feng, J.-Q.Chen, C.-L.Wu, M.W.Guidry

Fermion Dynamical Symmetry Model for the Even-Even and Even-Odd Nuclei in the Xe-Ba Region

NUCLEAR STRUCTURE ^{120,122,124,127,129,131,133,126,128,130,132}Xe, ^{131,133,135,137}Ba; calculated levels, B(λ), relative B(λ) in some cases. Fermion dynamical symmetry.

doi: 10.1103/PhysRevC.53.715
Citations: PlumX Metrics

1996SU03      Phys.Rev. C53, 2227 (1996)

Y.Sun, C.-L.Wu, D.H.Feng, J.L.Egido, M.Guidry

Identical Bands at Normal Deformation: Necessity of going beyond the mean-field approach

NUCLEAR STRUCTURE ¹⁷⁰Yb, ¹⁷¹Lu; analyzed identical band data; deduced need to go beyond mean field approach. Projected shell model.

doi: 10.1103/PhysRevC.53.2227
Citations: PlumX Metrics

1996WU09      Phys.Lett. 387B, 449 (1996)

C.-L.Wu, M.Guidry, D.H.Feng

Z = 110-111 Elements and the Stability of Heavy and Superheavy Elements

NUCLEAR STRUCTURE ²⁵⁶Rf, ²⁵⁸Db, ²⁶⁰Sg, ²⁶²Bh, ²⁶⁴Hs, ²⁶⁶Mt, ²⁶⁹Ds, ²⁷²Rg; calculated mass excess.

ATOMIC MASSES ²⁵⁶Rf, ²⁵⁸Db, ²⁶⁰Sg, ²⁶²Bh, ²⁶⁴Hs, ²⁶⁶Mt, ²⁶⁹Ds, ²⁷²Rg; calculated mass excess.

doi: 10.1016/0370-2693(96)01072-6
Citations: PlumX Metrics

1995GU25      Ann.Phys.(New York) 242, 135 (1995)

M.W.Guidry, C.-L.Wu, D.H.Feng

The Dynamical Pauli Effect

NUCLEAR STRUCTURE ¹⁶²Dy; calculated 2n-transfer probability to ¹⁶⁰Dy ground state. N=84-108; calculated single particle energy. Fermi dynamical symmetry model, dynamical Pauli effect.

doi: 10.1006/aphy.1995.1077
Citations: PlumX Metrics

1995WU03      Phys.Rev. C51, R1086 (1995)

C.-L.Wu, D.H.Feng, M.W.Guidry, H.-T.Chen, X.-W.Pan

Single-Particle Nondegeneracy and SU(3) Fermion Dynamical Symmetry

doi: 10.1103/PhysRevC.51.R1086
Citations: PlumX Metrics

1994GU11      Nucl.Phys. A579, 163 (1994)

M.Guidry, C.-L.Wu, D.H.Feng

Comments on the Origin of Gaps in Deformed Single-Particle Spectra

doi: 10.1016/0375-9474(94)90799-4
Citations: PlumX Metrics

1994LI67      Int.J.Mod.Phys. E3, 1119 (1994)

Z.-P.Li, M.W.Guidry, C.-L.Wu, D.H.Feng

New Microscopic View of Nuclear Deformation

NUCLEAR STRUCTURE N=60-150; analyzed B(E2) systematics, calculations; N=82-126; calculated energy surface primary, secondary minima deformation vs particle number in Sm isotopes, superdeformation discussed. Fermi dynamical symmetry model.

doi: 10.1142/S0218301394000334
Citations: PlumX Metrics

1994WU02      Nucl.Phys. A570, 377c (1994)

C.-L.Wu, H.-T.Chen

A Generalized Pair Field Approach to the Shell Model

doi: 10.1016/0375-9474(94)90304-2
Citations: PlumX Metrics

1993FE07      Phys.Rev. C48, R1488 (1993)

D.H.Feng, M.W.Guidry, X.-W.Pan, C.-L.Wu, I.Zlatev

Effective Fermion SO(6) Dynamical Symmetry in the Platinum Nuclei

NUCLEAR STRUCTURE ¹⁹⁶Pt; calculated levels; deduced fermion SO(6) dynamical symmetry evidence.

doi: 10.1103/PhysRevC.48.R1488
Citations: PlumX Metrics

1993GU08      Phys.Rev. C48, 1739 (1993)

M.W.Guidry, M.R.Strayer, C.-L.Wu, D.H.Feng

Some General Constraints on Identical Band Symmetries

NUCLEAR STRUCTURE ^192,194,196Hg, ^234,236,238U, ^{238,240,242,244}Pu, ^246,248Cm, ^248,250Cf; analyzed band structure; deduced normal, superdeformed identical bands related features.

doi: 10.1103/PhysRevC.48.1739
Citations: PlumX Metrics

1993WU05      Nucl.Phys. A565, 455 (1993)

L.-A.Wu, C.-L.Wu, M.W.Guidry, D.H.Feng

The Polarization Effect of SO(6) in the Fermion Dynamical Symmetry Model

NUCLEAR STRUCTURE ¹³³La; calculated levels; deduced band structure. Fermion dynamical symmetry model, SO(6) polarization effect.

doi: 10.1016/0375-9474(93)90221-I
Citations: PlumX Metrics

1993WU06      Ann.Phys.(New York) 222, 187 (1993)

C.-L.Wu, D.H.Feng, M.W.Guidry

Nuclear Superdeformation and the Supershell Fermion Dynamical Symmetry Model

NUCLEAR STRUCTURE Z=60-110; N=60-150; calculated regions favorable for superdeformation. Other aspects related to superdeformation discussed. Supershell fermion dynamical symmetry model.

doi: 10.1006/aphy.1993.1021
Citations: PlumX Metrics

1992HA06      Phys.Rev. C45, 1127 (1992)

X.-L.Han, C.-L.Wu, D.H.Feng, M.W.Guidry

Nuclear Masses in the Fermion Dynamical Symmetry Model

NUCLEAR STRUCTURE Z ≥ 82; N ≥ 126; calculated neutron, proton separation pairing gap energies. Z=98, 114; calculated mass shell corrections components. Fermion dynamical symmetry model.

doi: 10.1103/PhysRevC.45.1127
Citations: PlumX Metrics

1992HA35      At.Data Nucl.Data Tables 52, 43 (1992)

X.-L.Han, C.-L.Wu

Nuclear Superdeformation Data Tables

COMPILATION A=130, 150, 190; compiled Iγ for transitions in superdeformed bands.

doi: 10.1016/0092-640X(92)90009-7
Citations: PlumX Metrics

1992WA16      Phys.Lett. 284B, 196 (1992)

R.-P.Wang, F.-K.Thielemann, D.H.Feng, C.-L.Wu

Microscopic Nuclear Masses and Their Astrophysical Implications

NUCLEAR STRUCTURE A ≈ 210-260; calculated masses; deduced accurate level densities. Microscopic fermion dynamical symmetry model.

doi: 10.1016/0370-2693(92)90419-5
Citations: PlumX Metrics

1992WU06      Phys.Rev. C46, 1339 (1992)

C.-L.Wu, D.H.Feng, M.Guidry

Is There Objective Evidence for Quantized Spin Alignment in Superdeformed Nuclei ( Question )

NUCLEAR STRUCTURE ^{192,191,193,194}Hg, ¹⁹⁴Pb, ¹⁹⁴Tl; analyzed superdeformed band γ-transition energy analyses for spin determination; deduced quantized spin alignment related characteristics.

doi: 10.1103/PhysRevC.46.1339
Citations: PlumX Metrics

1991CH17      Phys.Rev. C44, 559 (1991)

J.-Q.Chen, D.H.Feng, M.W.Guidry, C.-L.Wu

Comment on ' Comparison of Realistic and Symmetry-Determined S and D Pairs of ¹⁵⁶Gd '

NUCLEAR STRUCTURE ¹⁵⁶Gd; analyzed S-, D-pair determination criteria.

doi: 10.1103/PhysRevC.44.559
Citations: PlumX Metrics

1991PI05      Phys.Rev. C43, 2224 (1991)

J.-L.Pin, J.-Q.Chen, C.-L.Wu, D.H.Feng

Nuclear Stretching

NUCLEAR STRUCTURE ¹⁵²Sm, ¹⁵⁸Gd, ¹⁶⁰Dy, ¹⁶⁶Er, ¹⁶⁶Yb, ¹⁷⁰Hf, ¹⁸⁸W; calculated B(λ). ^{162,164,166,168,170,172}Er, ^{168,170,172,174,176,178,180}Yb, ^{230,232,234,236,238,240}U, ^{238,240,242,244,246}Cm; calculated levels. Fermion dynamical symmetry model, stretching.

doi: 10.1103/PhysRevC.43.2224
Citations: PlumX Metrics

1991WA11      Phys.Rev. C43, 2268 (1991)

K.-X.Wang, G.-Z.Liu, D.F.Collinson, D.H.Feng, C.-L.Wu

Test of the Composite Particle Representation Theory

NUCLEAR STRUCTURE ²⁰O, ²⁰F, ²⁰Ne; calculated levels. Composite particle representation theory.

doi: 10.1103/PhysRevC.43.2268
Citations: PlumX Metrics

1991WU01      Nucl.Phys. A522, 31c (1991)

C.-L.Wu

Superdeformations and Fermion Dynamical Symmetries

NUCLEAR STRUCTURE ¹⁵⁰Gd, ¹⁹⁴Hg; calculated levels, band features, decay characteristics, superdeformation effects. Other nuclei discussed. Fermion dynamical symmetry model.

doi: 10.1016/0375-9474(91)90050-G
Citations: PlumX Metrics

1991WU04      Phys.Rev.Lett. 66, 1377 (1991)

C.-L.Wu, D.H.Feng, M.W.Guidry

Comment on ' Spin Alignment in Superdeformed Hg Nuclei '

NUCLEAR STRUCTURE ^192,194Hg; analyzed superdeformed band data; deduced spin alignment features.

doi: 10.1103/PhysRevLett.66.1377
Citations: PlumX Metrics

1990WU04      Nucl.Phys. A520, 459c (1990)

C.-L.Wu

Finite Particle Number Effect in High Spin B(E2)'s

NUCLEAR STRUCTURE ¹⁵²Dy, ^174,176,160Yb, ^168,172W, ¹⁶⁸Hf; calculated B(λ), ratios. Fermion dynamical symmetry model.

doi: 10.1016/0375-9474(90)91168-Q
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1990WU05      Fizika(Zagreb) 22, 123 (1990)

C.-L.Wu, M.W.Guidry, D.H.Feng, J.Q.Chen

β-γ Vibrations and SU₃ Symmetry in the Fermion Dynamical Symmetry Model

NUCLEAR STRUCTURE A > 228; calculated (β-γ) vibrational bandhead energies. Fermion dynamical symmetry model.

1988FE03      Phys.Lett. 205B, 157 (1988)

D.H.Feng, C.-L.Wu, M.W.Guidry, Z.-P.Li

Dynamical Pauli Effects and the Saturation of Nuclear Collectivity

NUCLEAR STRUCTURE Z=52-82; N=52-82; Z=82-126; N=126-184; analyzed B(E2). Fermion dynamical symmetry model.

1987GU06      Phys.Lett. 187B, 210 (1987)

M.W.Guidry, C.-L.Wu, Z.-P.Li, D.H.Feng, J.N.Ginocchio

An Algerbraic Fermion Description of Band Termination and Loss of Collectivity in Heavy Nuclei

NUCLEAR STRUCTURE ¹⁶²Dy, ^{160,166,174,176}Yb, ^168,172W; calculated B(E2) ratio relative to rigid rotor value. Algebraic fermion model.

doi: 10.1016/0370-2693(87)91082-3
Citations: PlumX Metrics

1987HA18      Phys.Lett. 192B, 253 (1987)

X.-L.Han, M.W.Guidry, D.H.Feng, K.-X.Wang, C.-L.Wu

Evidence for Nuclear Shell Symmetries

NUCLEAR STRUCTURE Z=36-100; calculated even-even nuclei B(E2) ratios; deduced shell symmetry evidence. Fermion dynamical symmetry model.

doi: 10.1016/0370-2693(87)90100-6
Citations: PlumX Metrics

1987WU06      Phys.Lett. 194B, 447 (1987)

C.-L.Wu, X.-L.Han, Z.-P.Li, M.W.Guidry, D.H.Feng

A Microscopic Formula for Actinide Masses

NUCLEAR STRUCTURE Z=82-126; calculated masses. Dynamical symmetry, microscopic approach.

doi: 10.1016/0370-2693(87)90214-0
Citations: PlumX Metrics

1986CA10      Phys.Rev.Lett. 56, 2578 (1986)

R.F.Casten, C.-L.Wu, Da Hsuan Feng, J.N.Ginocchio, Xiao-Ling Han

Empirical Evidence for an SO(7) Fermion Dynamical Symmetry in Nuclei

NUCLEAR STRUCTURE ^{98,100,102,104,106}Pd, ^{104,106,108,110,112}Pd; calculated levels, B(E2) ratios; deduced dynamical symmetry evidence. Ginocchio model, SO(7) fermion dynamical symmetry.

doi: 10.1103/PhysRevLett.56.2578
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1986GU11      Phys.Lett. 176B, 1 (1986)

M.W.Guidry, C.-L.Wu, D.H.Feng, J.N.Ginocchio, X.-G.Chen, J.-Q.Chen

A Fermion Dynamical Symmetry Model for High-Spin Physics

NUCLEAR STRUCTURE ²³²Th; calculated levels, E2 matrix elements. ¹⁶⁰Yb; calculated levels, alignment. Interacting boson model, dynamical symmetry.

doi: 10.1016/0370-2693(86)90913-5
Citations: PlumX Metrics

1980ZH01      Phys.Scr. 22, 426 (1980)

M.V.Zhukov, D.H.Feng, Cheng-li Wu, J.Bang

Study of the Two-Nucleon Surface Correlation Via a Simple Three Body System

NUCLEAR STRUCTURE ⁶He, ⁶Be, ¹⁸O, ¹⁸Ne, ⁴²Ca, ⁴²Ti; calculated levels. Three-body problem, two-nucleon surface clustering, Pauli effects.

doi: 10.1088/0031-8949/22/5/003
Citations: PlumX Metrics

Note: The following list of authors and aliases matches the search parameter C.L.Wu: , C.L.WU