NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = C.W.Nestor Found 21 matches. 2008KI07 Nucl.Instrum.Methods Phys.Res. A589, 202 (2008) T.Kibedi, T.W.Burrows, M.B.Trzhaskovskaya, P.M.Davidson, C.W.Nestor, Jr. Evaluation of theoretical conversion coefficients using BrIcc COMPILATION Z=5-110; compiled and evaluated ICC data. BrICC database.
doi: 10.1016/j.nima.2008.02.051
2006RA03 At.Data Nucl.Data Tables 92, 207 (2006) S.Raman, M.Ertugrul, C.W.Nestor, Jr., M.B.Trzhaskovskaya Ratios of internal conversion coefficients COMPILATION Z=26-100; A=57-254; compiled, analyzed ICC ratios, δ. Comparison of experimental data with several model calculations.
doi: 10.1016/j.adt.2005.12.001
2004NI14 Phys.Rev. C 70, 054305 (2004) N.Nica, J.C.Hardy, V.E.Iacob, S.Raman, C.W.Nestor, Jr., M.B.Trzhaskovskaya Precise measurement of αK for the M4 transition from 193Irm: A test of internal-conversion theory RADIOACTIVITY 193mIr(IT) [from 192Os(n, γ) and subsequent decay]; measured Eγ, Iγ, X-ray spectra; deduced conversion coefficient. Comparison with model predictions.
doi: 10.1103/PhysRevC.70.054305
2002BA85 At.Data Nucl.Data Tables 81, 1 (2002) I.M.Band, M.B.Trzhaskovskaya, C.W.Nestor, Jr., P.O.Tikkanen, S.Raman Dirac-Fock Internal Conversion Coefficients NUCLEAR STRUCTURE Z=10-126; A=20-310; calculated ICC. Relativistic self-consistent-field Dirac-Fock approach.
doi: 10.1006/adnd.2002.0884
2002RA45 Phys.Rev. C66, 044312 (2002) S.Raman, C.W.Nestor, Jr., A.Ichihara, M.B.Trzhaskovskaya How good are the internal conversion coefficients now? NUCLEAR STRUCTURE Z=22-94; A=46-240; compiled, analyzed ICC. Comparison of experimental data with several model calculations.
doi: 10.1103/PhysRevC.66.044312
2001RA27 At.Data Nucl.Data Tables 78, 1 (2001) S.Raman, C.W.Nestor, P.Tikkanen Transition Probability from the Ground to the First-Excited 2+ State of Even-Even Nuclides COMPILATION Z=4-100; compiled, evaluated B(E2) for transition from ground to first-excited 2+ states in even-even nuclides.
doi: 10.1006/adnd.2001.0858
1995ME13 Phys.Rev. C52, 1801 (1995) M.P.Metlay, J.L.Johnson, J.D.Canterbury, P.D.Cottle, C.W.Nestor, Jr., S.Raman, V.G.Zelevinsky Are Octupole Vibrations Harmonic ( Question ) NUCLEAR STRUCTURE A ≥ 60; analyzed B(E3) data; deduced octupole vibrations anharmonicity evidence. Data from (p, p'), (d, d'), (α, α') reactions.
doi: 10.1103/PhysRevC.52.1801
1994BH01 Phys.Rev. C49, 808 (1994) K.H.Bhatt, S.Raman, C.W.Nestor, Jr. Symplectic Pseudo-SU(3) Model and B(E2; 0+1 → 2+1) Value of 238U NUCLEAR STRUCTURE 238U; calculated B(λ), electric quadrupole moment; deduced need for effective charges. Symplectric pseudo-SU(3) model.
doi: 10.1103/PhysRevC.49.808
1992BH04 Phys.Rev. C46, 164 (1992) K.H.Bhatt, C.W.Nestor, Jr., S.Raman Do Nucleons in Abnormal-Parity States Contribute to Deformation ( Question ) NUCLEAR STRUCTURE 144Ce, 222Ra, 168Er, 250Cf; calculated quadrupole moments. 222,224,226,228Ra, 238,240,242,244Pu, 226,228,230,232,234Th, 244,246,248Cm, 230,232,234,236,238U, 250,252Cf, 148,150,152,154Sm, 152,154,156,158,160Gd, 154,156,158,160,162,168Dy, 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; calculated B(E2); deduced valence nucleons role. Woods-Saxon model.
doi: 10.1103/PhysRevC.46.164
1991RA02 Phys.Rev. C43, 556 (1991) S.Raman, C.W.Nestor, Jr., S.Kahane, K.H.Bhatt Low-Lying Collective Quadrupole and Octupole Strengths in Even-Even Nuclei NUCLEAR STRUCTURE Z ≥ 50; analyzed B(λ) data; deduced quadrupole, octupole vibrations harmonicity. Model comparisons.
doi: 10.1103/PhysRevC.43.556
1989RA16 At.Data Nucl.Data Tables 42, 1 (1989) S.Raman, C.W.Nestor, Jr., S.Kahane, K.H.Bhatt Predictions of B(E2;01+ → 21+) Values for Even-Even Nuclei COMPILATION Z=2-100; compiled adopted B(E2).
doi: 10.1016/0092-640X(89)90031-4
1988RA07 Phys.Rev. C37, 805 (1988) S.Raman, C.W.Nestor, Jr., K.H.Bhatt Systematics of B(E2; 01+ → 21+) Values for Even-Even Nuclei NUCLEAR STRUCTURE A=4-240; analyzed B(E2) systematics; deduced applicable structure models.
doi: 10.1103/PhysRevC.37.805
1988RA33 Phys.Rev.Lett. 61, 2817 (1988) S.Raman, C.W.Nestor, Jr., S.Kahane, K.H.Bhatt Comment on ' Loss of Collectivity at High Spin in 172W and a Three-Band Interpretation of First Yrast Upbends ' NUCLEAR STRUCTURE 172W; analyzed collectivity effects.
doi: 10.1103/PhysRevLett.61.2817
1987RA01 At.Data Nucl.Data Tables 36, 1 (1987) S.Raman, C.H.Malarkey, W.T.Milner, C.W.Nestor, Jr., P.H.Stelson Transition Probability, B(E2), from the Ground to the First-Excited 2+ State of Even-Even Nuclides COMPILATION A=6-254; compiled, evaluated 2+ level energies, B(E2), T1/2, β2, β2/β2(sp), EWSR, intrinsic quadrupole moments.
doi: 10.1016/0092-640X(87)90016-7
1977CA31 At.Data Nucl.Data Tables 19, 153 (1977) Calculation of K and L x rays for elements of Z = 95 to 130 ATOMIC PHYSICS Z=95-130; calculated relativistic Dirac-Fock Eigenvalues, K and L X-ray energies. Comparison with experimental binding energies.
doi: 10.1016/0092-640X(77)90012-2
1971LU14 At.Data 3, 1 (1971) C.C.Lu, T.A.Carlson, F.B.Malik, T.C.Tucker, C.W.Nestor, Jr. Relativistic Hartree-Fock-Slater Eigenvalues, Radial Expectation Values, and Potentials for Atoms, 2 < Z < 126
doi: 10.1016/S0092-640X(71)80002-5
1969CA10 Nucl.Phys. A135, 57 (1969) T.A.Carlson, C.W.Nestor, Jr., F.B.Malik, T.C.Tucker Calculation of K, L, M and N Binding Energies and K X-Rays for Elements From Z = 96-120
doi: 10.1016/0375-9474(69)90147-X
1969TU02 Phys.Rev. 178, 998 (1969) T.C.Tucker, L.D.Roberts, C.W.Nestor, Jr., T.A.Carlson, F.B.Malik Relativistic Self-Consistent-Field Calculation of the Wave Functions, Eigenvalues, Isotope Shifts, and the 6S Hyperfine-Structure Coupling Constant as a Function of Pressure for Metallic Gold in the Wigner-Seitz Model ATOMIC PHYSICS Au; calculated wave functions, eigenvalues, isotope shift , hfs coupling constant.
doi: 10.1103/PhysRev.178.998
1968CA29 Phys.Rev. 169, 27 (1968) T.A.Carlson, C.W.Nestor, Jr., T.C.Tucker, F.B.Malik Calculation of Electron Shake-Off for Elements from Z = 2 to 92 with the Use of Self-Consistent-Field Wave Functions ATOMIC PHYSICS Z=2-92; calculated electron shake-off.
doi: 10.1103/PhysRev.169.27
1968TU03 Phys.Rev. 174, 118 (1968) T.C.Tucker, L.D.Roberts, C.W.Nestor, Jr., T.A.Carlson, F.B.Malik Calculation of the Electron Binding Energies and X-Ray Energies for the Superheavy Elements 114, 126, and 140 Using Relativistic Self-Consistent-Field Atomic Wave Functions ATOMIC PHYSICS Au, U; Z=114, 116, 140; calculated electron binding energies, X-ray energies.
doi: 10.1103/PhysRev.174.118
1966NE10 ORNL-4027 (1966) C.W.Nestor, T.C.Tucker, T.A.Carlson, L.D.Roberts, F.B.Malik, C.Froese Relativistic and Non-Relativistic scf Wave Functions for Atoms and Ions from Z = 2 to 80, Together with Calculations of Binding Energies, Mean Radii, Screening Constants, Charge Distributions, and Electron Shake-Off Probabilities
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