NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = B.Buck Found 98 matches. 2019IB01 Phys.Rev. C 99, 064332 (2019) T.T.Ibrahim, A.C.Merchant, S.M.Perez, B.Buck α-cluster structure above double closed shells NUCLEAR STRUCTURE 20Ne, 44Ti, 94Mo, 104,136Te; calculated levels, J, π, B(E2), mean-square separation of the α-core system, α-decay widths using local potential cluster model with a cluster-core nuclear potential parametrized as mixture of Saxon-Woods and cubed Saxon-Woods terms. Comparison with experimental data.
doi: 10.1103/PhysRevC.99.064332
2013BU02 Phys.Rev. C 87, 024304 (2013), Erratum Phys.Rev. C 88, 039903 (2013) B.Buck, A.C.Merchant, S.M.Perez Local potential model of the Hoyle band in 12C NUCLEAR STRUCTURE 12C; calculated level energies, widths, charge radii of Hoyle band using a local potential 8Be+α cluster model. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.024304
2012BU08 Phys.Rev. C 85, 054302 (2012) B.Buck, A.C.Merchant, S.M.Perez Electromagnetic transition strengths in heavy nuclei NUCLEAR STRUCTURE 230,232Th, 234,238U; calculated reduced B(E2), B(M1) for transitions within and between K=0+, 1+ and 2+ bands. Cluster Model for the structure of heavy nuclei. Discussion of beta and gamma bands. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.054302
2012IB02 Phys.Rev. C 85, 044313 (2012) T.T.Ibrahim, S.M.Perez, S.M.Wyngaardt, B.Buck, A.C.Merchant Hybrid potential analysis of exotic clustering in heavy nuclei NUCLEAR STRUCTURE 222,224,226Ra, 228,230Th, 230,232,234,236U, 236,238Pu, 242Cm; calculated levels, J, π, B(E2), T1/2, exotic decay probability. Hybrid potential of a microscopic and a phenomenological core-cluster potential. Cluster model. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.044313
2011BU09 Phys.Rev. C 84, 034310 (2011) B.Buck, A.C.Merchant, S.M.Perez Generation of excited K bands in heavy nuclei NUCLEAR STRUCTURE 222Ra, 228Th, 232U, 236Pu; calculated radial wave functions for various L values and radial overlap integrals from a numerical solution of the Schrodinger equation. Binary cluster model. Schematics of K=0+, 1+, 2+ bands and transitions.
doi: 10.1103/PhysRevC.84.034310
2010BU02 Phys.Rev. C 81, 034322 (2010) B.Buck, A.C.Merchant, S.M.Perez Theory of recursive nuclear band spectra NUCLEAR STRUCTURE 102,104,106Mo, 102,104,106,110,112Ru, 102,110,114,116Pd, 140Xe, 144,146Ba, 146,148Ce, 148,150,152Nd, 150,152,154Sm, 152,154,156,158,160Gd, 154,156,158,160,162,164Dy, 156,158,160,162,164,166,168,170Er, 158,160,162,164,166,168,170,172,174,176Yb, 164,166,168,170,172,174,176,178,180Hf, 168,170,172,174,180,182,186W, 172,174,180,182,184,186,188,192Os, 176,180,184,186,188Pt, 222,224,226Ra, 222,226,228,230,232,234Th, 230,232,234,236,238U, 238,240,242,244Pu, 248Cm; analyzed nuclear band spectra using recursion formula based on a quantum mechanical model.
doi: 10.1103/PhysRevC.81.034322
2009BU09 J.Phys.(London) G36, 085101 (2009) B.Buck, A.C.Merchant, S.M.Perez, T.T.Ibrahim, S.M.Wyngaardt Electromagnetic transition strength ratios in 238U NUCLEAR STRUCTURE 238U; calculated B(E1), B(E2), B(E1)/B(E2). Pb-Ne cluster model, comparison with experiment.
doi: 10.1088/0954-3899/36/8/085101
2008BU03 Phys.Rev. C 77, 017301 (2008) B.Buck, A.C.Merchant, S.M.Perez Core-cluster partitions of rare-earth nuclei NUCLEAR STRUCTURE 142,144,146Ba, 146,148,150Ce, 146,148,150,152Nd, 148,150,152,154Sm, 152,154,156,158,160Gd, 154,156,158,160,162,164Dy, 156,158,160,162,164,166,168,170Er, 158,160,162,164,166,168,170,172,174,176Yb, 166,168,170,172,174,176,178,180Hf, 168,170,172,180,182,184,186W, 182,184,186,188,190,192Os, 184,186,188,190,192,194,196,198Pt; calculated cluster charge, cluster mass, potential radii, B(E2).
doi: 10.1103/PhysRevC.77.017301
2008BU11 J.Phys.(London) G35, 085101 (2008) B.Buck, A.C.Merchant, S.M.Perez Negative parity bands in even-even isotopes of Ra, Th, U and Pu NUCLEAR STRUCTURE 226Ra, 230Th, 234,236,238U, 238,240,242Pu; calculated level energies and B(E3) for negative parity bands using a Pb core plus exotic cluster model.
doi: 10.1088/0954-3899/35/8/085101
2007BU16 Phys.Rev. C 76, 014310 (2007) B.Buck, A.C.Merchant, S.M.Perez, H.E.Seals Core-cluster partitions of actinide nuclei NUCLEAR STRUCTURE Rn, Ra, Th, U, Pu, Cm; calculated level energies and B(E2) using a cluster model.
doi: 10.1103/PhysRevC.76.014310
2007BU20 J.Phys.(London) G34, 1985 (2007) B.Buck, A.C.Merchant, S.M.Perez Negative parity bands in 238U NUCLEAR STRUCTURE 238U; calculated level energies, K, J, π in terms of a Pb-Ne cluster model.
doi: 10.1088/0954-3899/34/9/010
2007BU27 Phys.Rev. C 76, 034326 (2007) B.Buck, A.C.Merchant, S.M.Perez Parameter-free characterization of nuclear band spectra
doi: 10.1103/PhysRevC.76.034326
2005BU03 Phys.Rev. C 71, 014311 (2005) B.Buck, A.C.Merchant, S.M.Perez Evidence of nuclear clustering throughout a major shell NUCLEAR STRUCTURE Z=56-80; analyzed data; deduced cluster model parameters. 166,168,170,172,174,176,178,180Hf; calculated rotational bands level energies, cluster features.
doi: 10.1103/PhysRevC.71.014311
2005BU17 Phys.Rev.Lett. 94, 202501 (2005) B.Buck, A.C.Merchant, S.M.Perez Interpretation of Correlations between Nuclear Observables in Rare-Earth Nuclei NUCLEAR STRUCTURE 170Er, 170Yb, 170Hf, 170W; A=140-200; analyzed levels, B(E2); deduced core-cluster decomposition parameters.
doi: 10.1103/PhysRevLett.94.202501
2005BU38 J.Phys.(London) G31, 1499 (2005) B.Buck, A.C.Merchant, S.M.Perez, H.E.Seals The exotic structure of heavy nuclei RADIOACTIVITY 222,224,226Ra(14C); 228Th(20O); 230Th, 232,234U(24Ne); 230U(22Ne); 234U(26Ne); 234U, 236,238Pu(28Mg); 238Pu(30Mg), (32Si); 242Cm(34Si); calculated decay widths. 212Po(α); calculated T1/2. Binary cluster model. NUCLEAR STRUCTURE 212Po, 222Ra, 228Th, 232U, 236Pu, 242Cm; calculated level energies.
doi: 10.1088/0954-3899/31/12/010
2004BU02 J.Phys.(London) G30, 65 (2004) B.Buck, A.C.Merchant, S.M.Perez Coexistence of very dissimilar cluster bands in 212Po NUCLEAR STRUCTURE 212Po; calculated cluster configuration energies, rotational bands.
doi: 10.1088/0954-3899/30/2/006
2003BU11 Phys.Rev. C 68, 024313 (2003) B.Buck, A.C.Merchant, S.M.Perez Theory of band comparison in even-even nuclei NUCLEAR STRUCTURE 142,144,146Ba, 146,148Ce, 146,148,150,152Nd, 150,152,154Sm, 218,220,222,224,226Ra, 222,224,226,228,230,232,234Th, 230,232,234,236,238U, 236,238,240,242,244Pu; calculated rotational bands relative μ, B(E2). 148,150Gd, 152,154Dy, 190,192,194Hg, 194,196Pb; calculated superdeformed bands relative μ, B(E2). 212Pb, 212Po; calculated superdeformed bands features. Cluster model.
doi: 10.1103/PhysRevC.68.024313
2003BU27 Acta Phys.Hung.N.S. 18, 303 (2003) B.Buck, A.C.Merchant, S.M.Perez Criteria for Comparison of Bands in Even-Even Nuclei NUCLEAR STRUCTURE 142,144,146Ba, 146,148Ce, 146,148,150,152Nd, 150,152,154Sm, 218,222,224,226Ra, 222,226,228,230,232,234Th, 230,232,234,236,238U, 238,240,242,244Pu; analyzed rotational bands, fractional change in transition energies and reduced mass. Cluster model.
doi: 10.1556/APH.18.2003.2-4.31
2002BU13 Yad.Fiz. 65, 701 (2002); Phys.Atomic Nuclei 65, 669 (2002) B.Buck, A.C.Merchant, S.M.Perez Transition Quadrupole Moments in Superdeformed Bands NUCLEAR STRUCTURE 60,62Zn, 80,82Sr, 84,86Zr, 132Ce, 134Nd, 142Sm, 146,148,150Gd, 152,154Dy, 190,192,194Hg, 194,196Pb, 236,238U; calculated superdeformed bands transition quadrupole moments. Binary cluster approach, comparisons with data.
doi: 10.1134/1.1471271
2002BU18 Phys.Rev. C65, 067306 (2002) B.Buck, A.C.Merchant, S.M.Perez Binary Cluster Model of Very Extended Shapes in the A ∼ 110 Region NUCLEAR STRUCTURE 102,104,106,108,110Ru, 104,106,108,110,112Pd, 106,108,110,112,114Cd, 108,110,112,114,116Sn, 110,112,114,116,118Te; calculated binary cluster configuration energies.
doi: 10.1103/PhysRevC.65.067306
2002BU34 Phys.Rev. C 66, 067303 (2002) B.Buck, A.C.Merchant, V.A.McBride, S.M.Perez New relation between B(E2) values and excitation energies NUCLEAR STRUCTURE A=10-252; analyzed B(E2), correlation with excitation energy for even-even nuclides. Binary cluster model.
doi: 10.1103/PhysRevC.66.067303
2001BU02 Phys.Rev. C63, 014312 (2001) B.Buck, A.C.Merchant, S.M.Perez Transition Quadrupole Moments in Superdeformed Bands NUCLEAR STRUCTURE 60,62Zn, 80,82Sr, 84,86Zr, 132Ce, 134Nd, 142Sm, 146,148,150Gd, 152,154Dy, 190,192,194Hg, 194,196Pb, 236,238U; calculated superdeformed bands transition quadrupole moments; deduced cluster configuration features. Binary cluster model, comparisons with data.
doi: 10.1103/PhysRevC.63.014312
2001BU08 Phys.Rev. C63, 037301 (2001) B.Buck, A.C.Merchant, S.M.Perez Magnetic Moments of Mirror Nuclei NUCLEAR MOMENTS A=3-59; compiled, analyzed μ, gyromagnetic ratios for mirror nuclei. 45,47V, 47Cr, 49Mn, 51,53Fe, 53Co, 55Ni, 57,59Cu, 59Zn; deduced predictions for ground-state μ.
doi: 10.1103/PhysRevC.63.037301
2000BU01 Phys.Rev. C61, 014310 (2000) B.Buck, A.C.Merchant, S.M.Perez Cluster Model Interpretation of Normal and Superdeformed Bands in 60Zn NUCLEAR STRUCTURE 60Zn; calculated levels, J, π, superdeformed bands B(E2), deformation. Local potential cluster model. Comparison with data.
doi: 10.1103/PhysRevC.61.014310
2000BU02 Phys.Rev. C61, 024314 (2000) B.Buck, A.C.Merchant, M.J.Horner, S.M.Perez Choosing Cluster and Core in Cluster Models of Nuclei NUCLEAR STRUCTURE 218,222,224,226,228Ra, 222,224,226,228,230,232,234Th, 230,232,234,236,238U; calculated transitions B(E2). Cluster models, method for determining cluster size discussed. Comparison with data.
doi: 10.1103/PhysRevC.61.024314
2000BU16 Nucl.Phys. A673, 157 (2000) B.Buck, A.C.Merchant, M.J.Horner, S.M.Perez Normal and Superdeformed Cluster Bands in Heavy Nuclei NUCLEAR STRUCTURE 194Hg, 236U, 240Pu; calculated rotational bands levels, J, π, superdeformed bands features. Cluster model, comparisons with data.
doi: 10.1016/S0375-9474(00)00130-5
2000BU32 Few-Body Systems 29, 53 (2000) B.Buck, A.C.Merchant, S.M.Perez Cluster Selection in Binary Nuclear Models NUCLEAR STRUCTURE 222,224,226,228,230,232,234Th, 218,222,224,226,228Ra, 230,232,234,236,238U, 238,240,242Pu; calculated transitions B(E2), cluster-core configuration features. Comparisons with data.
doi: 10.1007/s006010070008
1999BU03 Phys.Rev. C59, 750 (1999) B.Buck, A.C.Merchant, S.M.Perez Cluster Structure and γ Transitions in Actinide Nuclei NUCLEAR STRUCTURE 226Ra, 232Th, 234,236,238U; calculated E2, E3 transition matrix elements. Binary cluster model. Comparison with data.
doi: 10.1103/PhysRevC.59.750
1999BU06 Nucl.Phys. A650, 37 (1999) B.Buck, A.C.Merchant, S.M.Perez Cluster Model Investigation of 229Th NUCLEAR STRUCTURE 229Th; calculated levels, J, π, μ, quadrupole moment, B(M1), B(E2), parity-doublet bands. Cluster model.
doi: 10.1016/S0375-9474(99)00096-2
1999BU13 J.Phys.(London) G25, 901 (1999) B.Buck, A.C.Merchant, S.M.Perez Exotic Cluster Model of Band Structure in Actinides NUCLEAR STRUCTURE 232Th, 223Ac; calculated levels, J, π. 226Ra, 232Th, 236U; calculated E2 matrix elements. Binary cluster model. Comparison with data.
doi: 10.1088/0954-3899/25/4/065
1999BU14 Nucl.Phys. A652, 211 (1999) B.Buck, A.C.Merchant, S.M.Perez Possible Clustering in Isotopes of Ba NUCLEAR STRUCTURE 140,146Ba; calculated levels, J, π, B(λ). Cluster-core model. Comparison with data.
doi: 10.1016/S0375-9474(99)00163-3
1999BU27 Nucl.Phys. A657, 267 (1999) B.Buck, A.C.Merchant, S.M.Perez Exotic Clustering in Ce and Nd Isotopes NUCLEAR STRUCTURE 146,148,150Ce, 148,150,152,154Nd; calculated levels, J, π, B(E2), quadrupole moments. Exotic cluster model.
doi: 10.1016/S0375-9474(99)00342-5
1998BU06 Phys.Rev. C57, R2095 (1998) B.Buck, A.C.Merchant, S.M.Perez Alternative View of Collective Bands in Actinide Nuclei NUCLEAR STRUCTURE 223Ra, 234U; calculated levels, J, π, rotational bands. Binary cluster model, other actinide nuclei discussed.
doi: 10.1103/PhysRevC.57.R2095
1998BU08 Nucl.Phys. A634, 15 (1998); Erratum Nucl.Phys. A640, 506 (1998) B.Buck, A.C.Merchant, S.M.Perez Cluster Model Investigation of the Structure of 223Ra NUCLEAR STRUCTURE 223Ra; calculated levels, J, π, deformation, B(Eλ), B(Mλ). Pb+C+n cluster model. Comparison with data. RADIOACTIVITY 223Ra(14C); calculated partial decay T1/2. Pb+C+n cluster model.
doi: 10.1016/S0375-9474(98)00131-6
1998BU18 Phys.Rev. C58, 2049 (1998) B.Buck, A.C.Merchant, S.M.Perez Systematic Study of Exotic Clustering in Even-Even Actinide Nuclei NUCLEAR STRUCTURE 220,222,224,226Ra, 226,228,230,232,234Th, 232,234,236,238U, 236,238,240,242,244Pu, 244Cm; calculated levels, J, π, transitions B(E2), B(E4). Binary cluster model.
doi: 10.1103/PhysRevC.58.2049
1998BU23 Phys.Rev. C58, 2990 (1998) B.Buck, A.C.Merchant, S.M.Perez Cluster Model Investgigation of 223Ac NUCLEAR STRUCTURE 223Ac; calculated levels, J, π. Cluster model with odd proton. Comparison with data.
doi: 10.1103/PhysRevC.58.2990
1998BU27 Nucl.Phys. A644, 306 (1998) B.Buck, A.C.Merchant, S.M.Perez Cluster Model Investigation of 233U NUCLEAR STRUCTURE 233U; calculated ground-state μ, Q, bandhead excitation energies, levels J, π, transitions B(E2), B(M1). Pb-Ne-n cluster model.
doi: 10.1016/S0375-9474(98)00595-8
1997BU05 Nucl.Phys. A614, 129 (1997) B.Buck, A.C.Merchant, S.M.Perez Mass-Symmetric Form for Cluster-Core Potentials NUCLEAR STRUCTURE 44Ti, 24Mg; calculated levels, B(λ). 222Ra; 212Po; calculated levels. Cluster-core potentials, mass-symmetric forms.
doi: 10.1016/S0375-9474(96)00448-4
1997BU07 Nucl.Phys. A617, 195 (1997) B.Buck, A.C.Merchant, S.M.Perez Exotic Clustering in 222,224,226Ra RADIOACTIVITY 222,224,226Ra(14C); calculated T1/2. Mixed Saxon-Woods plus cubed Saxon-Woods cluster-core interaction. NUCLEAR STRUCTURE 222,224,226Ra; calculated levels, B(λ), deformation characteristics, (14C)-decay T1/2. Mixed Saxon-Woods plus cubed Saxon-Woods cluster-core interaction.
doi: 10.1016/S0375-9474(97)00043-2
1997BU20 Nucl.Phys. A625, 554 (1997) B.Buck, A.C.Merchant, S.M.Perez Exotic Clustering in 232,234,236,238U NUCLEAR STRUCTURE 232,234,236,238U; calculated levels, B(λ). Pb-Ne binary cluster model. RADIOACTIVITY 232,234U(24Ne); calculated T1/2. Pb-Ne binary cluster model.
doi: 10.1016/S0375-9474(97)00511-3
1997BU28 Nuovo Cim. 110A, 935 (1997) B.Buck, A.C.Merchant, S.M.Perez Exotic Cluster Model of Octupole Deformed Radium Isotopes NUCLEAR STRUCTURE 223Ra; calculated levels J, π, deformation, μ, Q. 222Ra; calculated levels J, π. 226Ra; calculated transitions B(Eλ). Binary cluster model. RADIOACTIVITY 222,224,226Ra(14C); calculated T1/2.
doi: 10.1007/BF03035929
1996BU05 Phys.Rev.Lett. 76, 380 (1996) B.Buck, A.C.Merchant, S.M.Perez Exotic Cluster States in Actinide Nuclei RADIOACTIVITY 224,226,222Ra(14C); 228Th(20O); 232U(24Ne); 234U, 236Pu(28Mg); 230Th, 232U(24Ne); 238Pu(32Si); calculated exotic decay T1/2. Cluster-core potential. NUCLEAR STRUCTURE 222Ra, 228Th, 232U, 236Pu; calculated exotic cluster spectra, B(λ). Cluster-core potential.
doi: 10.1103/PhysRevLett.76.380
1996BU08 Phys.Rev. C53, 2841 (1996) B.Buck, J.C.Johnston, A.C.Merchant, S.M.Perez Cluster Model of α Decay and 212Po NUCLEAR STRUCTURE 212Po; calculated levels, B(λ), α-decay T1/2. Cluster model. NUCLEAR REACTIONS 208Pb(α, α), E=23.5, 40 MeV; calculated σ(θ). Cluster model wave functions.
doi: 10.1103/PhysRevC.53.2841
1996BU19 Nucl.Phys. A600, 387 (1996) A Simple Expression for the General Oscillator Bracket
doi: 10.1016/0375-9474(96)00035-8
1996BU35 Phys.Rev. C54, 2063 (1996) B.Buck, A.C.Merchant, S.M.Perez Alpha Decays of Neutron Deficient Isotopes in the Region N > 82 > Z RADIOACTIVITY 159,156Hf, 157,160,161,158,159Ta, 158,163,164W, 160,162,161,163,164,166Re, 163,164,170,172Os, 166,167,168,174,170,171,172,173Ir, 169,171Pt, 173,177,178Au, 175,176,177,178,179Hg, 179Tl, 149Tb, 156,155Lu, 172,174,177Au(α); calculated α-decay T1/2. 156Ta(p); calculated p-emission T1/2. Cluster model, three-parameter local potential with cosh geometry.
doi: 10.1103/PhysRevC.54.2063
1995BU03 Phys.Rev. C51, 559 (1995) B.Buck, A.C.Merchant, S.M.Perez Systematics of Alpha-Cluster States Above Double Shell Closures NUCLEAR STRUCTURE 20Ne, 44Ti, 94Mo, 212Po; calculated levels, B(λ), Γγ, Γα, T1/2 in some cases. Alpha-particle cluster models.
doi: 10.1103/PhysRevC.51.559
1995BU24 Nucl.Phys. A593, 80 (1995) B.Buck, A.C.Merchant, S.M.Perez Model-Dependence of Hindrance Factors for Alpha-Decay, and Consequences for the Description of the 45.1 s Isomeric State of 212Po RADIOACTIVITY 212Po(α); calculated α-decay reduced hindrance factors; deduced model dependence, implication for 212Po isomeric state.
doi: 10.1016/0375-9474(95)00335-X
1995BU25 Phys.Rev. C52, 1840 (1995) B.Buck, J.C.Johnston, A.C.Merchant, S.M.Perez Unified Treatment of Scattering and Cluster Structure in α + Closed Shell Nuclei: 20Ne and 44Ti NUCLEAR STRUCTURE 20Ne; 44Ti; calculated levels, B(λ), α-emission widths. Universal α-core interaction. NUCLEAR REACTIONS 16O(α, α), E=22-49.5 MeV; 40Ca(α, α), E=24.1-49.5 MeV; analyzed σ(θ); deduced model parameters. Universal α-core interaction.
doi: 10.1103/PhysRevC.52.1840
1995BU35 Phys.Rev. D51, 1419 (1995) Magnetic Moments and β Decays of Octet Baryons NUCLEAR MOMENTS 1n, 1H; calculated μ. Simple variant of the constituent quark model. Other aspects of octet baryons included.
doi: 10.1103/PhysRevD.51.1419
1995MA62 Nucl.Phys. A591, 85 (1995) The Determination of Nuclear Charge Distributions using a Bayesian Maximum Entropy Method NUCLEAR STRUCTURE 4He, 12C; calculated charge density, form factor. Bayesian maximum entropy method.
doi: 10.1016/0375-9474(95)00125-K
1994BU07 J.Phys.(London) G20, 351 (1994) B.Buck, A.C.Merchant, S.M.Perez, P.Tripe Calculation of Exotic Decay Half-Lives for All Observed Cases RADIOACTIVITY 221Fr, 225Ac, 221,223,222,224,226Ra(14C); 228Th(20O); 233,234,235,237U, 231Pa, 230Th(24Ne); 234U, 238,236Pu(28Mg); 238Pu(32Si), (28Mg); 231Pa(23F); 233,235U(25Ne); 114Ba(12C); calculated T1/2, effective Q. Cluster model.
doi: 10.1088/0954-3899/20/2/013
1994BU12 Phys.Rev. C49, 3357 (1994) B.Buck, A.C.Merchant, S.M.Perez Comment on ' α-Decay Properties of Neutron-Deficient Polonium and Radon Nuclei '
doi: 10.1103/PhysRevC.49.3357
1994BU13 Phys.Rev.Lett. 72, 1326 (1994) B.Buck, A.C.Merchant, S.M.Perez Alpha-Cluster Structure in 212Po NUCLEAR STRUCTURE 212Po; calculated α-, γ-decay widths, T1/2, α-branching ratios, ICC for ground state 'band' levels. α-cluster model.
doi: 10.1103/PhysRevLett.72.1326
1993BU05 Phys.Rev. C47, 1307 (1993) B.Buck, A.C.Merchant, S.M.Perez, P.Tripe Diffuse Well Analysis of Exotic Decay of Heavy Nuclei RADIOACTIVITY 222,224,226Ra(14C); 232U, 230Th(24Ne); 234U, 236Pu(28Mg); 238Pu(32Si); analyzed exotic decay T1/2 data; deduced model parameters. Cluster model, diffuse well.
doi: 10.1103/PhysRevC.47.1307
1993BU09 At.Data Nucl.Data Tables 54, 53 (1993) B.Buck, A.C.Merchant, S.M.Perez Half-Lives of Favored Alpha Decays from Nuclear Ground States RADIOACTIVITY A=106-266; compiled α-decay T1/2 data. Cluster model comparison.
doi: 10.1006/adnd.1993.1009
1993KA13 Nucl.Phys. A556, 1 (1993) Cluster Model for the Mass-22 T = 1 Triplet Nuclei NUCLEAR STRUCTURE 22Ne, 22Na, 22Mg; calculated levels, quadrupole moment, μ, B(λ). Clusters orbiting a subnucleus, Buck-Dover-Vary model.
doi: 10.1016/0375-9474(93)90234-O
1992BU03 J.Phys.(London) G18, 143 (1992) B.Buck, A.C.Merchant, S.M.Perez Favoured Alpha Decays of Odd-Mass Nuclei RADIOACTIVITY A=145-257; calculated α-decay T1/2; deduced preformed α-particle existence evidence. Simple cluster model.
doi: 10.1088/0954-3899/18/1/012
1992BU04 Phys.Rev. C45, 1688 (1992) B.Buck, A.C.Merchant, S.M.Perez Ground State Proton Emission from Heavy Nuclei RADIOACTIVITY 109I, 113Cs, 147Tm, 151,150Lu, 156Ta, 160Re(p); calculated p-decay T1/2. Realistic proton-nucleus potential.
doi: 10.1103/PhysRevC.45.1688
1992BU06 Phys.Rev. C45, 2247 (1992) B.Buck, A.C.Merchant, S.M.Perez α Decay Calculations with a Realistic Potential NUCLEAR STRUCTURE N=80-160; calculated α-decay T1/2; deduced α-particle preformation probability dependence on mass.
doi: 10.1103/PhysRevC.45.2247
1992RA25 Phys.Rev.Lett. 69, 3709 (1992) W.D.M.Rae, A.C.Merchant, B.Buck The Shape Eigenstate: A new kind of resonance NUCLEAR REACTIONS 12C(12C, 12C'), E(cm)=33, 35 MeV; analyzed σ(θ); deduced new type of resonance evidence. Coherence between nearly degenerate resonances.
doi: 10.1103/PhysRevLett.69.3709
1991BU01 J.Phys.(London) G17, L91 (1991) B.Buck, A.C.Merchant, S.M.Perez Unifying Model for Alpha Decay and Exotic Decay of Heavy Nuclei RADIOACTIVITY 222,224,226Ra(14C); 230Th, 232U(24Ne); 234U, 234Pu(28Mg); 238Pu(32Si); analyzed decay data. Extension of α-decay model.
doi: 10.1088/0954-3899/17/6/001
1991BU05 J.Phys.(London) G17, 1223 (1991) B.Buck, A.C.Merchant, S.M.Perez Ground State to Ground State Alpha Decays of Heavy Even-Even Nuclei RADIOACTIVITY A=164-264; analyzed α-decay T1/2 data; deduced Geiger-Nuttal plot discontinuity features. Cluster model.
doi: 10.1088/0954-3899/17/8/012
1991KA23 Nucl.Phys. A533, 215 (1991) Cluster Model of 11B and 11C NUCLEAR STRUCTURE 11C, 11B; calculated levels, B(λ), μ. Cluster model. RADIOACTIVITY 11C; calculated β-decay log ft. Cluster model.
doi: 10.1016/0375-9474(91)90487-Q
1990BU09 J.Phys.(London) G16, L85 (1990) Size Effects in the Theory of Exotic Decay and Alpha Decay from Heavy Nuclei RADIOACTIVITY 222,224,226Ra(12C), 230Th(24Ne), 234U(28Mg), 238Pu(32Si); calculated decay T1/2. Cluster model.
doi: 10.1088/0954-3899/16/5/001
1990BU13 Nucl.Phys. A512, 483 (1990) B.Buck, A.C.Merchant, S.M.Perez Can We Obtain Nuclear Structure Information from Exotic Decays of Heavy Nuclei ( Question ) RADIOACTIVITY 221Fr, 221,222,223,224,226Ra, 225Ac(14C), (α); 230Th, 231Pa, 232,233U(24Ne), (α); calculated exotic, α-decay T1/2. Cluster model.
doi: 10.1016/0375-9474(90)90082-W
1990BU14 Nucl.Phys. A513, 75 (1990) B.Buck, P.D.B.Hopkins, A.C.Merchant A 12C + 12C Cluster Model of 24Mg NUCLEAR STRUCTURE 24Mg; calculated levels, B(λ). Cluster model. NUCLEAR REACTIONS 24Mg(e, e), E not given; calculated form factors. Cluster model.
doi: 10.1016/0375-9474(90)90344-L
1990BU30 Phys.Rev.Lett. 65, 2975 (1990) B.Buck, A.C.Merchant, S.M.Perez New Look at α Decay of Heavy Nuclei RADIOACTIVITY 220,222,224,226,228,230,232Th, 214,216,218,206,204,202,200,198,196,194,192Po, 172,174,176,178,180,182,184,186,188,190Pt(α); analyzed T1/2 data. 200,202,204,206,208Rn, 206,208,210Ra; analyzed T1/2 differences. Z=76-100; analyzed α-decay data. Preformed α-particle model.
doi: 10.1103/PhysRevLett.65.2975
1990KA31 Nucl.Phys. A518, 449 (1990) Cluster Model of 23Na and 23Mg NUCLEAR STRUCTURE 23Na, 23Mg; calculated levels, B(λ). Cluster model.
doi: 10.1016/0375-9474(90)90140-H
1989BU05 J.Phys.(London) G15, 615 (1989) A Consistent Cluster Model Treatment of Exotic Decays and Alpha Decays from Heavy Nuclei RADIOACTIVITY A=106-206; calculated α-decay width. Comparison with data, other decays examined, cluster model.
doi: 10.1088/0954-3899/15/5/015
1989BU06 Phys.Rev. C39, 2097 (1989) Cluster-Model Calculations of Exotic Decays from Heavy Nuclei RADIOACTIVITY 221,222,223,224,226Ra(14C); 231Pa, 232,233U(24Ne); calculated partial width Γ. Cluster model.
doi: 10.1103/PhysRevC.39.2097
1989FA12 Phys.Lett. 231B, 25 (1989) Excitation of 7Li below the Coulomb Barrier NUCLEAR REACTIONS 208Pb(7Li, 7Li'), E ≈ 16-30 MeV; calculated projectile Coulomb excitation probaility.
doi: 10.1016/0370-2693(89)90106-8
1989ME09 Europhys.Lett. 8, 409 (1989) Cluster Model Calculations of Alpha-Decays Across the Periodic Table NUCLEAR STRUCTURE A ≈ 211-230; calculated partial α-decay widths. Cluster model.
doi: 10.1209/0295-5075/8/5/003
1988BU17 J.Phys.(London) G14, L211 (1988) Cluster Model of A = 7 Nuclei Revisited, and the Astrophysical S Factors for 3He(α, γ)7Be and 3H(α, γ)7Li at Zero Energy NUCLEAR REACTIONS, ICPND 3He, 3H(α, γ), E at rest; calculated capture reaction astrophysical S-factor. Cluster model. NUCLEAR STRUCTURE 7Li, 7Be; calculated rms charge radii, B(E2), quadrupole moments, cluster breakup Γ. Cluster model.
doi: 10.1088/0305-4616/14/2/013
1986BA03 J.Phys.(London) G12, L29 (1986) The Cluster Structure of 24Mg NUCLEAR STRUCTURE 24Mg; calculated levels, B(E2). Two 12C nuclei cluster model.
doi: 10.1088/0305-4616/12/1/006
1985BU02 J.Phys.(London) G11, L11 (1985) B.Buck, R.A.Baldock, J.A.Rubio Cluster Model of A = 7 Nuclei and the Astrophysical S Factor for 3He(α, γ)7Be at Zero Energy NUCLEAR REACTIONS, ICPND 3He(α, γ), E ≈ 0; calculated astrophysical σ factor S(E). 4He(3He, 3He), E(cm)=0-15 MeV; calculated phase shifts. Cluster model. NUCLEAR STRUCTURE 7Li; calculated rms radii, quadrupole moment, B(E2), B(M1), μ. 7Be; calculated B(M1), log ft.
doi: 10.1088/0305-4616/11/1/003
1984BA48 Nucl.Phys. A426, 222 (1984) R.A.Baldock, B.Buck, J.A.Rubio Alpha Cluster States in 16O NUCLEAR REACTIONS 12C(α, α), E not given; calculated compound system resonances, Γα, Γγ. Coupled-channels formalism, cluster-core model. NUCLEAR STRUCTURE 16O; calculated levels, B(E2), rotational bands, rms charge radius. Cluster-core model.
doi: 10.1016/0375-9474(84)90106-4
1984BU25 J.Phys.(London) G10, L209 (1984) Revised Calculation of Alpha-Cluster Rotational States in 16O NUCLEAR STRUCTURE 16O; calculated rotational band levels, Γα. Cluster core system.
doi: 10.1088/0305-4616/10/2/012
1983BU07 Phys.Rev.Lett. 50, 1975 (1983); Erratum Phys.Rev.Lett. 51, 1395 (1983) New Look at Magnetic Moments and Beta Decays of Mirror Nuclei NUCLEAR STRUCTURE A=3-43; analyzed μ, β-decay data; deduced axial vector coupling constant quenching, effective orbital nucleon g factors. Model independent method.
doi: 10.1103/PhysRevLett.50.1975
1979BU12 Nucl.Phys. A327, 29 (1979) B.Buck, A.C.Merchant, N.Rowley Semi-Microscopic Calculation of α-Cluster States in 18F NUCLEAR STRUCTURE 18F; calculated α-cluster states; deduced mixing of two-particle shell-model states. Semi-microscopic calculation, spin-orbit, tensor interactions.
doi: 10.1016/0375-9474(79)90316-6
1978BU03 Nucl.Phys. A295, 1 (1978) Trinucleon Cluster States in 18F and 18O NUCLEAR STRUCTURE 18F, 18O; calculated trinucleon cluster levels.
doi: 10.1016/0375-9474(78)90016-7
1977BU01 Nucl.Phys. A275, 246 (1977) B.Buck, H.Friedrich, C.Wheatley Local Potential Models for the Scattering of Complex Nuclei NUCLEAR REACTIONS 3,4He(α, α), 16O(16O, 16O); calculated phase shifts.
doi: 10.1016/0375-9474(77)90287-1
1977BU05 Nucl.Phys. A280, 133 (1977) Alpha-Particle and Triton Cluster States in 19F NUCLEAR STRUCTURE 19F, 19Ne; calculated 3-, 4-particle cluster states, properties.
doi: 10.1016/0375-9474(77)90300-1
1977BU22 Nucl.Phys. A290, 205 (1977) Alpha-Particle Cluster States in 18F and 18O NUCLEAR STRUCTURE 18F, 18O; calculated, predicted levels, K, J, π. 18O, 18,19F, 20Ne; analyzed α-cluster state systematics.
doi: 10.1016/0375-9474(77)90675-3
1975BU03 Phys.Rev. C11, 1803 (1975) Simple Potential Model for Cluster States in Light Nuclei NUCLEAR STRUCTURE 15N, 16O, 20Ne; calculated levels, J, π, B(E2) values, α-widths, radii in cluster model with folded potential.
doi: 10.1103/PhysRevC.11.1803
1974AN36 Phys.Rep. 12, 201 (1974) N.Anyas-Weiss, J.C.Cornell, P.S.Fisher, P.N.Hudson, A.Menchaca-Rocha, D.J.Millener, A.D.Panagiotou, D.K.Scott, D.Strottman, D.M.Brink, B.Buck, P.J.Ellis, T.Engeland Nuclear structure of light nuclei using the selectivity of high energy transfer reactions with heavy ions NUCLEAR REACTIONS 12C, 16O, 40Ca(12C, 11B), (12C, 11C), (12C, 10B), (12C, 10Be), (12C, 10C), (12C, 9Be), E=114 MeV; 12,13C(11B, 9Li), E=114 MeV; 13C(11B, 10B), E=114 MeV; measured particle spectra, σ(E, θ). 13,14C, 13,14,15N, 14,15O deduced levels, J, π, spectroscopic amplitudes.
doi: 10.1016/0370-1573(74)90045-3
1969MA20 Phys.Rev. 178, 1864 (1969) M.A.J.Mariscotti, G.Scharff-Goldhaber, B.Buck Phenomenological Analysis of Ground-State Bands in Even-Even Nuclei NUCLEAR STRUCTURE 208Pb; calculated proton density near nuclear surface.
doi: 10.1103/PhysRev.178.1864
1968ZU02 Phys.Rev.Letters 21, 39 (1968) A.P.Zuker, B.Buck, J.B.McGrory Structure of O16
doi: 10.1103/PhysRevLett.21.39
1967BU05 Nucl.Phys. A95, 271 (1967) Calculation of Photonuclear Resonance Cross Sections by Coupled Channel Reaction Theory
doi: 10.1016/0375-9474(67)90504-0
1964BE07 Phys. Rev. 133, B323 (1964) J.Benveniste, A.C.Mitchell, B.Buck, C.B.Fulmer Proton Scattering of Isobars and Single Isotopes NUCLEAR STRUCTURE 64Zn, 64Ni, 58Ni, 58Fe, 56Fe; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.133.B323
1963BU22 Phys.Rev. 130, 712 (1963) Calculation of Elastic and Inelastic Proton Scattering with a Generalized Optical Model NUCLEAR STRUCTURE 68Zn, 64Zn, 66Zn, 48Ti, 60Ni; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.130.712
1963BU25 Phil.Mag. 8, 1805 (1963) B.Buck, A.P.Stamp, P.E.Hodgson The excitation of collective states by inelastic scattering the extended optical model
doi: 10.1080/14786436308209075
1962BU04 Nuclear Phys. 29, 496 (1962) Optical Model Analysis of Mg24(d, p)Mg25* at 10.1 MeV NUCLEAR STRUCTURE 25Mg; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90199-2
1962BU17 Phys.Rev. 127, 940 (1962) Excitation of Two-Phonon States by Inelastic α-Particle Scattering NUCLEAR STRUCTURE 58Ni; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.127.940
1962BU29 Phys.Rev.Letters 8, 444 (1962) Effect of Nuclear Collective Motions on s- and P- Wave Strength Functions
doi: 10.1103/PhysRevLett.8.444
1962PE27 Nuclear Phys. 32, 353 (1962) A Non-Local Potential Model for the Scattering of Neutrons by Nuclei
doi: 10.1016/0029-5582(62)90345-0
1961BU01 Bull.Am.Phys.Soc. 6, No.1, 38, MA11 (1961) Distorted Wave Analysis of the Reaction Si28(d, p)-Si29 NUCLEAR STRUCTURE 29Si; measured not abstracted; deduced nuclear properties.
1961BU16 Phil.Mag. 6, 1371 (1961) NUCLEAR STRUCTURE 16O, 49Ti, 45Ca, 10B; measured not abstracted; deduced nuclear properties.
doi: 10.1080/14786436108241232
1960BU24 Phil.Mag. 5, 1181 (1960) B.Buck, R.N.Maddison, P.E.Hodgson
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