NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = S.Agbemava Found 22 matches. 2024LA06 Phys.Rev. C 109, 044306 (2024) D.Lay, E.Flynn, S.Agbemava, K.Godbey, W.Nazarewicz, S.A.Giuliani, Jh.Sadhukhan Multimodal fission from self-consistent calculations
doi: 10.1103/PhysRevC.109.044306
2023SP02 Phys.Lett. B 841, 137932 (2023) M.Spieker, S.E.Agbemava, D.Bazin, S.Biswas, P.D.Cottle, P.J.Farris, A.Gade, T.Ginter, S.Giraud, K.W.Kemper, J.Li, W.Nazarewicz, S.Noji, J.Pereira, L.A.Riley, M.Smith, D.Weisshaar, R.G.T.Zegers Hexadecapole strength in the rare isotopes 74, 76Kr NUCLEAR REACTIONS 1H(74Kr, 74Kr'), (76Kr, 76Kr'), E(cm)=100 MeV, [secondary 74,76Kr beams from 9Be(78Kr, X), E=150 MeV/nucleon primary reaction, followed by separation of fragments using A1900 separator]; measured Doppler-corrected Eγ, Iγ, (particle)γ-coin using NSCL-MSU using NSCL/Ursinus Liquid Hydrogen (LH2) Target, eight GRETINA modules of 36-fold segmented HPGe detectors for γ radiation, and S800 spectrograph for projectile-like reaction residues. 74,76Kr; deduced levels, Jπ, β2 for the first 2+ state and β4 and B(E4)(W.u.) for the first 4+ state from inelastic proton scattering experiments in inverse kinematics. Comparison to coupled-channels calculations, and nuclear density functional theory (DFT) calculations using the Skyrme SkM* and UNEDF1 energy density functionals, covariant NL3* and DD-PC1 energy density functionals. Systematics and theoretical predictions of β2, β4 and B(E4)(W.u.) for 74,76,78,80,82,84,86Kr.
doi: 10.1016/j.physletb.2023.137932
2022FL03 Phys.Rev. C 105, 054302 (2022) E.Flynn, D.Lay, S.Agbemava, P.Giuliani, K.Godbey, W.Nazarewicz, J.Sadhukhan Nudged elastic band approach to nuclear fission pathways RADIOACTIVITY 240Pu, 235U(SF); calculated potential energy surfaces in (Q20, Q30) coordinates, action integrals, fission paths. Nudged elastic band method (NEB), grid-based methods, and the Euler-Lagrange approach.
doi: 10.1103/PhysRevC.105.054302
2021AG03 Phys.Rev. C 103, 034323 (2021) Hyperheavy spherical and toroidal nuclei: The role of shell structure NUCLEAR STRUCTURE 456156; calculated binding energy as function of β2 deformation parameter. Z=1-200, N=1-440; calculated distribution of ellipsoidal and toroidal shapes in the nuclear landscape using RHB with CEDF DD-PC1. 58Ni, 100,132Sn, 208Pb, 304120, 366138, 462154, 592186; calculated proton and neutron shell gaps, fission barrier heights as functions of proton and neutron numbers using NL1, NL3, NL3*, FSUGold, DD-ME2, DD-MEδ, DD-PC1, PC-PK1, PC-F1, and TM1 covariant energy density functionals. 592186; calculated potential energy surfaces in (β2, β3) and (β2cos(γ+30°), β3sin(γ+30°))plane. 348138, 466156, 584174, 592186; calculated proton and neutron densities. 348138, 466156; calculated proton and neutron single-particle energies, deformation energy curves and dominant components Nilsson wave functions, Z=126-144, N=206-228; Z=128-144, N=204-228; Z=126-144; calculated S(2n), S(2p) for even-even nuclei. Investigation of the properties of spherical and toroidal hyperheavy even-even nuclei and their underlying shell structures using covariant density functional theory (CDFT).
doi: 10.1103/PhysRevC.103.034323
2020AL10 Phys.Rev. C 102, 024326 (2020) S.O.Allehabi, V.A.Dzuba, V.V.Flambaum, A.V.Afanasjev, S.E.Agbemava Using isotope shift for testing nuclear theory: The case of nobelium isotopes NUCLEAR STRUCTURE 252,254No; calculated nuclear charge distributions, rms charge radii for five nuclear models using covariant density functional theory (CDFT) with state-of-the-art covariant energy density functionals, isotope shifts and field isotope shifts for four electric dipole atomic transitions using CI+MBPT method. Comparison with experimental data. 254No, 286No; calculated difference in charge radii, isotope shifts between 254No and hypothetical 286No in different nuclear models for four electric dipole transitions from the ground state.
doi: 10.1103/PhysRevC.102.024326
2020CA18 Phys.Rev. C 102, 024311 (2020) Y.Cao, S.E.Agbemava, A.V.Afanasjev, W.Nazarewicz, E.Olsen Landscape of pear-shaped even-even nuclei NUCLEAR STRUCTURE Z=40-100, N=40-200; calculated ground state octupole deformations β3 and octupole deformation energies of even-even nuclei in the (Z, N) plane using the Skyrme energy density functionals (SEDFs): UNEDF0, UNEDF1, UNEDF2, SLy4, and SV-min. 80Zr, 112,146Ba, 224Ra, 286Th; calculated Single-particle energy splitting between the unusual-parity intruder shell and the normal-parity shell using (SEDFs): UNEDF0, UNEDF1, UNEDF2, SLy4, SV-min, DD-ME2, NL3*, DD-PC1 and PC-PK1. 212,214,216,218,220,222,224,226,228,230Rn, 214,216,218,220,222,224,226,228,230,232Ra, 216,218,220,222,224,226,228,230,232,234Th, 216,218,220,222,224,226,228,230,232,234U, 138,140,142,144,146,148,150,152Ba, 140,142,144,146,148,150,152,154Ce, 142,144,146,148,150,152,154,156Nd; calculated deformation parameters β2, β3, and octupole deformation energies using the Skyrme energy density functionals models. 112,114,144,146,148Ba, 144,146,148Ce, 146,148,196,198Nd, 150,194,196,198Sm, 196,198,200Gd, 198,200,202Dy, 200,202Er, 218,220,222,224,278,280,282Rn, 218,220,222,224,226,228,280,282,284,286,288Ra, 220,222,224,226,228,282,284,286,288,290Th, 222,224,226,228,230,282,284,286,288,290U, 224,226,228,230,232,284,286,288,290,292Pu, 224,226,228,230,284,286,288,290,292,294Cm, 226,228,230,284,286,288,290,292,294,296Cf, 226,228,230,232,284,286,288,290,292,294,296,298Fm, 230,286,288,290,292,294,296,298No, 288,290,292,294,296,300Rf, 290,292,294Sg; calculated β3 deformation parameter, octupole deformation energies, proton moments Q20 and Q30 for octupole-deformed nuclei obtained in five Skyrme energy density functionals, and four covariant energy density functionals. Comparison between Skyrme and covariant models, and with relevant experimental data. See also supplemental material.
doi: 10.1103/PhysRevC.102.024311
2020TA21 Phys.Rev. C 102, 054330 (2020) A.Taninah, S.E.Agbemava, A.V.Afanasjev Covariant density functional theory input for r-process simulations in actinides and superheavy nuclei: The ground state and fission properties NUCLEAR STRUCTURE 206,208,210,212,214,216,218,220,220,220,220,220,230,232,234,236,238,240,242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290,292,294,296,298,300Th, 264,266,258,270,272,274,276,278,280,282,284,286,288,290,292,294,296,298,300,302,304,306,308,310,312,314,316,318,320,322,324,326,328,330,332,334,336,338,340,342,344,346,348,350,352,354,356,358,360,362,364,366,368Ds; calculated binding energies as function of deformation β2. 240,242,326,328Cf, 246,330,332Fm, 248,250,334,336No, 250,252,254Rf, 254,256Sg; calculated superdeformed minima, β2, β3, second fission barriers, deformation energy curves and potential energy surface in (β2, β3) plane for 240Cf. 202,204,308,346Th, 210,214,316,350U, 216,220,326,352Pu, 222,224,348,354Cm, 228,354,356Cf, 232,358Fm, 236,238,360No, 242,244,362Rf, 248,250,364Sg, 254,256,366,396Hs, 260,264,368,402Ds, 266,270,370,410Cn, 272,276,376,416Fl, 278,282,402,428Lv, 284,288,412,436Og, 290,294,418,434120; predicted two-proton and two-neutron drip lines. 298,302,306,308,310,312,316,318,320,322,326,328,330,332,336,340Og; calculated potential-energy surfaces in (β2cos(γ+30), β2sin(γ+30)) plane. Z=90-120, N=110-320; calculated proton quadrupole deformations β2, binding-energies, S(2n), Q(α), α-decay half-lives, heights of primary fission barriers. Covariant density functional theory (CDFT) using state-of-the-art DD-PC1, DD-ME2, NL3*, and PC-PK1 CEDFs. Comparison to available data. Relevance to r-process modeling in heavy nuclei, and for the study of fission cycling.
doi: 10.1103/PhysRevC.102.054330
2019AG03 Phys.Rev. C 99, 014318 (2019) S.E.Agbemava, A.V.Afanasjev, A.Taninah Propagation of statistical uncertainties in covariant density functional theory: Ground state observables and single-particle properties NUCLEAR STRUCTURE 34,36,38,40,42,44,46,48,50,52,54,56,58,60,62,64,66,68,70,72,74,76Ca, 50,52,54,56,58,60,62,64,66,68,70,72,74,76,78,80,82,84,86,88,90,92,94,96Ni, 98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172Sn, 176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218,220,222,224,226,228,230,232,234,236,238,240,242,244,246,248,250,252,254,256,258,260,262,264,266Pb, 304120; calculated range of variations of parameters and statistical uncertainties in total binding energy, charge radii, S(2n), and neutron skins using covariant energy density functional theory (CDFT) with only the covariant energy density functionals (CEDFs) with nonlinear density dependency. 208,266Pb, 304120; calculated neutron and proton single-particle states, and relative energies of the pairs of neutron and proton single-particle states. Z=2-112, N=2-172; deduced differences between theoretical and experimental binding energies for several CEDFs for even-even nuclei; calculated charge quadrupole deformations β2 of ground states in even-even nuclei using the RHB calculations. Z=2-96, N=2-152; deduced differences between theoretical and experimental charge radii for several CEDFs.
doi: 10.1103/PhysRevC.99.014318
2019AG06 Phys.Rev. C 99, 034316 (2019) S.E.Agbemava, A.V.Afanasjev, A.Taninah, A.Gyawali Extension of the nuclear landscape to hyperheavy nuclei NUCLEAR STRUCTURE 208Pb, 466156; calculated binding energies versus β2. 366138, 466156, 580174; calculated neutron and proton single-particle energies, potential energy surfaces (PES) in (β2, β3) and (β2, γ) planes. 466156; calculated neutron density distribution versus β2, neutron and proton pairing energies and pairing gaps as a function of the β2 and γ deformations. 208Pb, 292120, 368138, 466156, 584174; calculated proton and neutron densities, charge radii, neutron skins. 296,300122, 316,320124; calculated deformation energy curves as function of β2, potential energy surfaces (PES) in (β2, β3) plane. 324,328,332,336,340,344,348,352,356,360,364,368,372,376,380,384,388,392,396,400,404,408,412,416,420,424,428,432,436,440,444,448,452,456,460,464138; calculated deformation energy curves, and proton and neutron chemical potentials as function of β2. 268Sg, 332Ds, 360130, 354,432134, 348138; calculated three-dimensional potential energy surfaces in (β2, β4, γ) plane. 258,268,278,288,298,308,318,328,338,348,358Sg, 272,282,292,302,312,322,332,342,352,362Ds, 276,286,296,306,316,326,336,346,356,366Fl, 290,300,310,320,330,340,350,360,370,380,390Og; calculated heights of fission barriers along the fission paths for quadrupole and triaxial deformations, inner fission barrier heights. 208Pb, 354134, 466156, 426176; calculated Coulomb energies as function of β2. Z=140-180, N=192-420; calculated proton β2 values of the lowest in energy solutions of the Z=140-180 nuclei. Z=132-176, N=292-324; calculated S(2n), S(2p), neutron and proton pairing energies for spherical minima. Z=2-170, N=2-440; calculated proton quadrupole deformations β2 of the lowest in energy minima for axial symmetry with ellipsoidal-like shapes, for nuclei with fission barriers > 2 MeV, and nuclei with two-proton and two-neutron drip lines. Covariant density functional theory with DD-ME2, PC-PK1, DD-PC1 and NL3* functionals, based on axial reflection symmetric and reflection asymmetric relativistic Hartree-Bogoliubov (RHB) calculations, and treating triaxiality within the triaxial RHB and triaxial relativistic mean field+BCS frameworks.
doi: 10.1103/PhysRevC.99.034316
2018AF01 Phys.Scr. 93, 034002 (2018) A.V.Afanasjev, H.Abusara, S.E.Agbemava Octupole deformation in neutron-rich actinides and superheavy nuclei and the role of nodal structure of single-particle wavefunctions in extremely deformed structures of light nuclei NUCLEAR STRUCTURE 292Cm, 36Ar; calculated octupole deformed shapes in neutron-rich actinides; deduced the presence of new region of octupole deformation in neutron-rich actinides, lack of octupole deformation in the ground states of superheavy for Z>108.
doi: 10.1088/1402-4896/aaa3d0
2017AG05 Phys.Rev. C 95, 054324 (2017) S.E.Agbemava, A.V.Afanasjev, D.Ray, P.Ring Assessing theoretical uncertainties in fission barriers of superheavy nuclei NUCLEAR STRUCTURE 276,278,280,282,284,286,288,290,292,294,296Cn, 280,282,284,286,288,294,296,298Fl, 284,286,288,290,292,294,296,298,300Lv, 288,290,294,296,298,300,302,304,306Og, 292,294,296,298,300,302,304,306,308120; calculated heights of inner fission barriers. Z=96-126, N=140-196; calculated heights of inner fission barriers, binding energies of ground states, energies of saddle points. 296Cn; calculated deformation energy curves as function of β2. 284Cn, 300120; calculated potential energy surface contours in (β2cos(γ+30), β2sin(γ+30)) plane, with systematic and statistical uncertainties quantified, and benchmarking of the functionals to the experimental data on fission barriers. Covariant energy density functional (CEDF) theory based on the state-of-the-art functionals NL3*, DD-ME2, DD-MEd, DD-PC1, and PC-PK1, in the axially symmetric and triaxial relativistic Hartree-Bogoliubov (RHB) frameworks.
doi: 10.1103/PhysRevC.95.054324
2017AG08 Phys.Rev. C 96, 024301 (2017) Octupole deformation in the ground states of even-even Z ∼ 96, N ∼ 196 actinides and superheavy nuclei NUCLEAR STRUCTURE 278,280,282,284,286,288,290,292,294,296,298Th, 282,284,286,288,290,292,294,296,298,300U, 280,282,284,286,288,290,292,294,296,298,300,302Pu, 280,282,284,286,288,290,292,294,296,298,300,302,304Cm, 282,284,286,288,290,292,294,296,298,300,302,304,306Cf, 284,286,288,290,292,294,296,298,300,302,304,306,308Fm, 282,284,286,288,290,292,294,296,298,300,302,304,306,308,310No, 284,286,288,290,292,294,296,298,300,302,304,306,308,310,312Rf, 286,288,290,292,294,296,298,300,302,304,306,308,310,312,314Sg; calculated equilibrium quadrupole β2, octupole β3 deformations, and ΔE(octupole). 286,288,290,292,294,296,298,300Cm, 288Th, 290U, 292Pu, 296Cf, 298Fm, 300No, 302Rf; calculated potential energy surfaces of even-A Cm isotopes and N=118 isotones in the (β2, β3) plane. State-of-the-art covariant energy density functionals (CDFT) using DD-PC1, DD-ME2, NL3*, and PC-PK1 functionals. Comparison with Skyrme DFT, Gogny DFT, and microscopic+macroscopic calculations.
doi: 10.1103/PhysRevC.96.024301
2016AF01 Phys.Rev. C 93, 054310 (2016) Covariant energy density functionals: Nuclear matter constraints and global ground state properties NUCLEAR STRUCTURE Z<100, N<160; calculated binding energies and charge radii of ground states using state-of-the-art covariant energy density functionals; deduced that density functionals with good description of global binding energies and properties of other ground and excited state not necessarily obtained from strict enforcement of constraints on nuclear matter properties (NMP). Detailed comparisons with experimental data.
doi: 10.1103/PhysRevC.93.054310
2016AG06 Phys.Rev. C 93, 044304 (2016) S.E.Agbemava, A.V.Afanasjev, P.Ring Octupole deformation in the ground states of even-even nuclei: A global analysis within the covariant density functional theory NUCLEAR STRUCTURE 56,60Ca, 78Sr, 78,80,108,110,112Zr, 82Mo, 90Cd, 108,110,112,142,144Xe, 108,110,112,114,116,142,144,146,148,150Ba, 114,144,146,148,150Ce, 146,148,150Nd, 150Sm, 196,198,200,202Gd, 200,202,204Dy, 198,200,202,204Er, 204Yb, 210Os, 214Pt, 216,218Hg, 180,182,184,216,218,220,222Pb, 218,220,222Po, 218,220,222,224,226,232Rn, 218,220,222,224,226,228,230Ra, 220,222,224,226,228,230,232,236,288,290,292,294Th, 220,222,224,226,228,230,232,234,238,290,292,294,296U, 222,224,226,228,230,232,234,240,288,290,292,294,296Pu, 224,226,228,230,232,234,236,242,286,288,290,292,294,296,298Cm, 224,226,228,230,232,234,236,238,288,290,292,294,296,298,300Cf, 226,228,232,234,236,238,240,290,292,294,296,298,300,302Fm, 236,238,240,242,284,286,288,290,292,294,296,298,300,302,304,306No, 242,244,246,288,290,292,294,296,298,300,304,306,308Rf, 248,250,288,290,292,294,300,302,304,306Sg; calculated equilibrium β2, β3 deformation parameters for ground states using DD-PC1 and NL3* density functional models and ϵ2, ϵ3 parameters by mic-mac (MM) approach, potential energy surfaces in (β2, β3) plane using CEDF DD-PC1 theory. Covariant energy density functionals (CEDF) of different types, with a nonlinear meson coupling, with density-dependent meson couplings, and pairing correlations within relativistic Hartree-Bogoliubov theory. Predicted a new region of octupole deformation around Z=98 and N=196. Comparison with available experimental data.
doi: 10.1103/PhysRevC.93.044304
2015AF01 Phys.Rev. C 91, 014324 (2015) A.V.Afanasjev, S.E.Agbemava, D.Ray, P.Ring Neutron drip line: Single-particle degrees of freedom and pairing properties as sources of theoretical uncertainties NUCLEAR STRUCTURE Z=4-110, N=4-260; Z=70, N=78-180; calculated neutron pairing energies, neutron δ(2n)(Z, N) quantities between two-proton and two-neutron drip lines. Z=86, N=184-206; calculated neutron chemical potential, neutron quadrupole deformation β2, neutron pairing gap, neutron pairing energy, and neutron single-particle energies. 114Ge, 180Xe, 266Pb, 270Rn, 366Hs; calculated neutron single-particle states at spherical shape, neutron shell gaps at the 2n-drip lines, spread of theoretical predictions for the single-particle energies. 56Ni, 100,132Sn, 208Pb; calculated spread of theoretical predictions for the single-particle energies for doubly magic nuclei. Analyzed theoretical uncertainties in the prediction of the two-neutron drip line using covariant density functional theory (CEDFs) and several interactions.
doi: 10.1103/PhysRevC.91.014324
2015AF02 Acta Phys.Pol. B46, 405 (2015) Nuclear Structure Theory of the Heaviest Nuclei NUCLEAR STRUCTURE 292,304120; analyzed available data; calculated single-particle states, J, π.
doi: 10.5506/APhysPolB.46.405
2015AG09 Phys.Rev. C 92, 054310 (2015) S.E.Agbemava, A.V.Afanasjev, T.Nakatsukasa, P.Ring Covariant density functional theory: Reexamining the structure of superheavy nuclei NUCLEAR STRUCTURE 236,238,240,242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290,292Cm, 238,240,242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290,292,294Cf, 240,242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290,292,294,296Fm, 242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290,292,294,296,298No, 246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290,292,294,296,298,300Rf, 250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290,292,294,296,298,300,302Sg, 258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290,292,294,296,298,300,302,304Hs, 264,266,268,270,272,274,276,278,280,282,284,286,288,290,292,294,296,298,300,302,304,306Ds, 270,272,274,276,278,280,282,284,286,288,290,292,294,296,298,300,302,304,306,308Cn, 276,278,280,282,284,286,288,290,292,294,296,298,300,302,304,306,308,310Fl, 282,284,286,288,290,292,294,296,298,300,302,304,306,308,310,312Lv, 290,292,294,296,298,300,302,304,306,308,310,312,314Og, 292,294,296,298,300,302,304,306,308,310,312,314,316120, 298,300,302,304,306,308,310,312,314,316,318122, 304,306,308,310,312,314,316,318,320124, 312,314,316,318,320,322126, 318,320,322,324128, 324,326130; calculated binding energies, proton and neutron quadrupole deformations, charge radii, root-mean square (rms) proton radii, neutron skin thicknesses, S(2n), S(2p), Q(α) and T1/2(α) using Viola-Seaborg formula. 292,304120; calculated neutron and proton single-particle states, shell gaps. Relativistic Hartree-Bogoliubov theory with DD-PC1 and PC-PK1 interactions, and five most up-to-date covariant energy density functionals of different types.
doi: 10.1103/PhysRevC.92.054310
2014AG08 Phys.Rev. C 89, 054320 (2014) S.E.Agbemava, A.V.Afanasjev, D.Ray, P.Ring Global performance of covariant energy density functionals: Ground state observables of even-even nuclei and the estimate of theoretical uncertainties NUCLEAR STRUCTURE Z=2-120, N=2-280; calculated properties of ground states of even-even nuclei between the two-proton and two-neutron drip lines, binding energies, S(2n), S(2p), charge quadrupole-, hexadecapole- and isovector β2 deformations, charge radii, neutron skin thickness, positions of two-proton and two-neutron drip line, neutron and proton three-point indicators and pairing gaps, density, energy per particle, incompressibility, effective masses. Large-scale axial relativistic Hartree-Bogoliubov calculations with four modern covariant energy density functionals (CEDF) such as NL3*, DD-ME2, DD-MEd, and DD-PC1. Comparison with other calculations and experimental data. Also supplemental information available. ATOMIC MASSES A=10-300; calculated masses, binding energies of 835 even-even nuclei and compared with experimental values. Large-scale axial relativistic Hartree-Bogoliubov calculations with four modern covariant energy density functionals (CEDFs).
doi: 10.1103/PhysRevC.89.054320
2013AF02 Phys.Lett. B 726, 680 (2013) A.V.Afanasjev, S.E.Agbemava, D.Ray, P.Ring Nuclear landscape in covariant density functional theory NUCLEAR STRUCTURE Z=1-120, N=1-300; calculated two-proton and neutron separation energies and dripline, neutron chemical potentials, quadrupole deformations. Skyrme density and covariant density functional theory calculations.
doi: 10.1016/j.physletb.2013.09.017
2011AG01 Ann.Nucl.Energy 38, 379 (2011) S.E.Agbemava, R.B.M.Sogbadji, B.J.B.Nyarko, R.Della Measurement of thermal neutron capture cross section and resonance integral of the 138Ba(n, γ)139Ba reaction using 55Mn(n, γ)56Mn as a monitor NUCLEAR REACTIONS 55Mn, 138Ba(n, γ), E=thermal; measured Eγ, Iγ; deduced thermal σ, resonance integral.
doi: 10.1016/j.anucene.2010.10.005
2011AG07 Ann.Nucl.Energy 38, 1616 (2011) S.E.Agbemava, B.J.B.Nyarko, J.J.Fletcher, R.B.M.Sogbadji, E.Mensimah, M.Asamoah Measurement of thermal neutron and resonance integral cross sections of the reaction 51V(N, γ)52V using a 20 Ci Am-Be isotopic neutron source NUCLEAR REACTIONS 51V, 55Mn(n, γ), E=thermal; measured Eγ, Iγ; deduced thermal and resonance integral σ. Comparison with experimental data and JENDL-3.2 evaluated nuclear library.
doi: 10.1016/j.anucene.2011.02.019
2011AG09 Ann.Nucl.Energy 38, 1737 (2011) S.E.Agbemava, B.J.B.Nyarko, J.J.Fletcher, R.B.M.Sogbadji, E.Mensimah, M.Asamoah Thermal neutron cross section determination of short-to-medium lived nuclides using a 20 Ci Am-Be neutron source NUCLEAR REACTIONS 55Mn, 127I, 152,154Sm, 238U(n, γ), E=thermal; measured Eγ, Iγ; deduced thermal neutron σ and uncertainties. Activation technique.
doi: 10.1016/j.anucene.2011.04.004
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