NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = F.Knapp Found 48 matches. 2023BY03 Phys.Rev. C 108, 024615 (2023) P.Bydzovsky, D.Denisova, D.Petrellis, D.Skoupil, P.Vesely, G.De Gregorio, F.Knapp, N.Lo Iudice Self-consistent many-body approach to the electroproduction of hypernuclei NUCLEAR REACTIONS 12C(e, eK+)12B, 16O(e, eK+)16N, 40Ca(e, eK+)40K, 48Ca(e, eK+)48K, E*<31 MeV; calculated differential σ(θ) for hypernuclei electroproduction, excitation spectrum, σ of electroproduction for selected hypernucleus states. Microscopic self-consistent many-body mean field approach, known as Tamm-Dancoff for hypernuclei extended by equation of motion phonon method (EMPM). Comparison to available experimental data and empirical shell-model calculations. Relevance to the preparation of planned E12-15-008 experiment at JLab. NUCLEAR STRUCTURE 12B, 16N, 28Al, 40K, 48K; calculated Λ binding energy for hypernuclei. 40K, 48K; calculated levels of hypernuclei, J, π, proton and Λ single particle states. Tamm-Dancoff formalism with the NF YNG interaction and elementary amplitudes - SLA and BS3.
doi: 10.1103/PhysRevC.108.024615
2023DE21 Phys.Rev. C 108, 024316 (2023) G.De Gregorio, F.Knapp, P.Vesely, N.Lo Iudice Survey of the 8He properties within a microscopic multiphonon approach NUCLEAR STRUCTURE 8He; calculated levels, J, π, ground-state energy, proton and neutron radii, charge radii, proton and neutron single-particle energies, neutron and proton densities, B(E1) strength distribution, E1 isovector and isoscalar transition strengths, dipole polarizability, proton and neutron transition densities. Equation of motion phonon method (EMPM) which constructs and solves iteratively a set of equations of motion and yields states composed of an arbitrary number (n=2, 3, ...) of particle-hole (p-h) or two-quasiparticle Tamm-Dancoff (TD) phonons. Comparison to available experimental data. NUCLEAR REACTIONS 8He(γ, X), E<40 MeV; calculated E1 σ(E).
doi: 10.1103/PhysRevC.108.024316
2023KN01 Phys.Rev. C 107, 014305 (2023) F.Knapp, P.Papakonstantinou, P.Vesely, G.De Gregorio, J.Herko, N.Lo Iudice Comparative analysis of formalisms and performances of three different beyond-mean-field approaches NUCLEAR STRUCTURE 40Ca; calculated E1 and E2 responses, B(E1) and B(E2) distributions. 16O, 40,48Ca; calculated isovector and isoscalar E1 (dipole) strength functions, E2 (quadrupole) strength functions, E3 (octupole) strength functions, monopole strength function, energy weighted running sums of strength functions. Calculations using equation of motion phonon method (EMPM), second Tamm-Dancoff and random-phase approximations (STDA and SRPA).
doi: 10.1103/PhysRevC.107.014305
2022DE04 Phys.Rev. C 105, 024326 (2022) G.De Gregorio, F.Knapp, N.Lo Iudice, P.Vesely Spectroscopic properties of 4He within a multiphonon approach NUCLEAR STRUCTURE 4He; calculated levels, J, π, charge radii, ground state energy, B(E1) distribution. Equation of motion phonon method (EMPM). Comparison to experimental data. NUCLEAR REACTIONS 4He(γ, X), E=18-48 MeV; calculated σ of Giant Dipole Resonance excitation. Equation of motion phonon method (EMPM) calculations performed with up to 3 phonons. Comparison to experimental data.
doi: 10.1103/PhysRevC.105.024326
2021DE30 Phys.Lett. B 821, 136636 (2021) G.De Gregorio, F.Knapp, N.Lo Iudice, P.Vesely Removal of the center of mass in nuclei and its effects on 4He NUCLEAR STRUCTURE 4He; calculated excitation energies, J, π, n-phonon compositions, B(E1) using an equation of motion method for solving the nuclear eigenvalue problem.
doi: 10.1016/j.physletb.2021.136636
2020DE03 Phys.Rev. C 101, 024308 (2020) G.De Gregorio, F.Knapp, N.Lo Iudice, P.Vesely Proper treatment of the Pauli principle in mirror nuclei within the microscopic particle(hole)-phonon scheme NUCLEAR STRUCTURE 15,17O, 15N, 17F, 39Ca, 39K; calculated levels, J, π, magnetic dipole and electric quadrupole moments, log ft values for β decays, B(M1), B(E1), B(E2), B(E3) using the space spanned by states composed of a particle (hole) coupled to Tamm-Dancoff approximation (TDA) phonons with NNLOsat chiral potential, and with and without the proton-neutron potential. Comparison with experimental data.
doi: 10.1103/PhysRevC.101.024308
2020PO04 Acta Phys.Pol. B51, 617 (2020) J.Pokorny, G.De Gregorio, F.Knapp, N.Lo Iudice, P.Vesely Effect of Λ Particle Phonon Coupling on the Energy Spectra of 5ΛHe and 17ΛO*
doi: 10.5506/APhysPolB.51.617
2019DE02 Phys.Rev. C 99, 014316 (2019) G.De Gregorio, F.Knapp, N.Lo Iudice, P.Vesely Microscopic multiphonon approach to nuclei with a valence hole in the oxygen region NUCLEAR STRUCTURE 15,16,21,22O, 15,21N; calculated levels, J, π, B(E1), B(M1), B(E2), B(E3), magnetic moments, β-decay logft values, and pygmy and giant dipole resonance (GDR) cross sections, and Phonon composition of selected states using microscopic multiphonon equation of motion method (EMPM) for odd nuclei with a valence hole. Comparison with experimental data. RADIOACTIVITY 21N(β-); calculated logft and B(GT) using microscopic multiphonon equation of motion method (EMPM). Comparison with available experimental data.
doi: 10.1103/PhysRevC.99.014316
2019KN03 Acta Phys.Pol. B50, 541 (2019) F.Knapp, T.Dytrych, D.Langr, T.Oberhuber Importance Basis Truncation in the Symmetry-adapted No-core Shell Model NUCLEAR STRUCTURE 12C; calculated ground-state energy, low-lying levels energies, B(E2). Ab-initio symmetry-adapted no-core shell model approach (SA-NCSM).
doi: 10.5506/aphyspolb.50.541
2018DE11 Phys.Rev. C 97, 034311 (2018) G.De Gregorio, F.Knapp, N.Lo Iudice, P.Vesely Microscopic multiphonon approach to spectroscopy in the neutron-rich oxygen region NUCLEAR STRUCTURE 22,23O, 23F; calculated levels, J, π, phonon composition of the low-lying states, weights of two-phonon components, E1 reduced strength distributions, E1 cross section, transition densities for low-lying 1- states, isoscalar versus isovector B(E1), Hartree-Fock levels for 23O and 23F. Equation of motion phonon method (EMPM), Tamm-Dancoff approximation (TDA), and Hartree-Fock method. Comparison with experimental data. RADIOACTIVITY 23O(β-); calculated logft, B(GT) and B(F) strengths, using equation of motion phonon method (EMPM), Tamm-Dancoff approximation (TDA), and Hartree-Fock method. Comparison with experimental data.
doi: 10.1103/PhysRevC.97.034311
2017DE07 Phys.Rev. C 95, 024306 (2017) G.De Gregorio, J.Herko, F.Knapp, N.Lo Iudice, P.Vesely Ground-state correlations within a nonperturbative approach NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated ground-state energies, binding energies/nucleon, point proton radii, ground state correlations, two-phonon components of the ground state in 16O; investigated convergence properties versus the harmonic oscillator frequency and space dimensions. 4He, 16,24O, 34Si, 40,48Ca, 48,56,78Ni, 88Sr, 90Zr, 100,114,132Sn, 146Gd, 208Pb; calculated root-mean-square point proton radii, and compared with experimental values. Nonperturbative calculations using Hartree-Fock basis within an equation-of-motion phonon method with a nucleon-nucleon optimized chiral potential.
doi: 10.1103/PhysRevC.95.024306
2017DE08 Phys.Rev. C 95, 034327 (2017) G.De Gregorio, F.Knapp, N.Lo Iudice, P.Vesely Low- and high-energy spectroscopy of 17O and 17F within a microscopic multiphonon approach NUCLEAR STRUCTURE 17O, 17F; calculated complete set of levels, J, π, phonon amplitudes for selected states, B(E1), B(E2), quadrupole moments, magnetic dipole moments, log ft value for β decay of 17F ground-state. 16,17O, 17F; calculated cross sections for pygmy and giant dipole resonances. Microscopic multiphonon equation of motion method for odd nuclei, using TammDancoff phonons. Comparison with experimental data.
doi: 10.1103/PhysRevC.95.034327
2017DE16 Phys.Scr. 92, 074003 (2017) G.De Gregorio, F.Knapp, N.Lo Iudice, P.Vesely A microscopic multiphonon approach to even and odd nuclei NUCLEAR REACTIONS 132Sn, 208Pb, 16,17O, 17F(γ, X), E not given; calculated electric dipole σ. Comparison with experimental data.
doi: 10.1088/1402-4896/aa6fa2
2016DE10 Phys.Rev. C 93, 044314 (2016) G.De Gregorio, F.Knapp, N.Lo Iudice, P.Vesely Self-consistent quasiparticle formulation of a multiphonon method and its application to the neutron-rich 20O nucleus NUCLEAR STRUCTURE 20O; calculated energy levels, J, π, B(E2), B(E1), E1 cross section, pygmy and giant dipole resonances, 2-qp compositions of the first 2+ state, and two 1- TDA phonons. Bogoliubov quasiparticle formulation of an equation-of-motion multiphonon method (EMPM) with phonons obtained in Tamm-Dancoff approximation (TDA). Comparison with experimental values.
doi: 10.1103/PhysRevC.93.044314
2016DE38 Phys.Rev. C 94, 061301 (2016) G.De Gregorio, F.Knapp, N.Lo Iudice, P.Vesely Microscopic multiphonon method for odd nuclei and its application to 17O NUCLEAR STRUCTURE 17O; calculated energy levels, J, π, B(E2), electric quadrupole moment, magnetic dipole moment, pygmy and giant dipole resonance cross sections. New equation of motion phonon method for odd-A nuclei. Comparison with experimental data.
doi: 10.1103/PhysRevC.94.061301
2015KN01 Phys.Rev. C 92, 054315 (2015) F.Knapp, N.Lo Iudice, P.Vesely, F.Andreozzi, G.De Gregorio, A.Porrino Dipole response in 208Pb within a self-consistent multiphonon approach NUCLEAR STRUCTURE 208Pb; calculated pygmy and giant-dipole resonance cross sections, energy levels, B(E1), neutron skin radius using self-consistent multiphonon, equation of motion phonon method (EMPM). Comparison with experimental data.
doi: 10.1103/PhysRevC.92.054315
2014BI01 J.Phys.(London) G41, 025109 (2014) D.Bianco, F.Knapp, N.Lo Iudice, P.Vesely, F.Andreozzi, G.De Gregorio, A.Porrino A self-consistent study of multipole response in neutron-rich nuclei using a modified realistic potential NUCLEAR STRUCTURE 16,18,20,22O, 116,124,130,132Sn; calculated neutron single-particle spectra, B(E1), strength functions. HFB, comparison with available data.
doi: 10.1088/0954-3899/41/2/025109
2014KN01 Phys.Rev. C 90, 014310 (2014) F.Knapp, N.Lo Iudice, P.Vesely, F.Andreozzi, G.De Gregorio, A.Porrino Dipole response in 132Sn within a self-consistent multiphonon approach NUCLEAR STRUCTURE 132Sn; calculated neutron and proton single-particle levels, pygmy resonances, dipole response, isovector and isoscalar E1 strengths, neutron particle-hole phonon composition, E1 transition density; strength fragmentation enhanced. Equation of motion phonon method and Tamm-Dancoff approximation with Hartree-Fock basis. Comparison with experimental results.
doi: 10.1103/PhysRevC.90.014310
2013BI08 Phys.Rev. C 88, 024303 (2013) D.Bianco, N.Lo Iudice, F.Andreozzi, A.Porrino, F.Knapp Spectroscopy of neutron-rich Te and Xe isotopes within a new shell model context NUCLEAR STRUCTURE 134Sn, 134,136,138,140Te, 136,138,140Xe; calculated levels, J, π, B(E2), B(M1); deduced collectivity, neutron-proton symmetry. Large-scale shell model calculation based on an iterative matrix diagonalization algorithm. Comparison with experimental data. Systematics of energies and B(E2) values of first 2+ states in even-even A=126-140 Te and A=132-140 Xe nuclei.
doi: 10.1103/PhysRevC.88.024303
2012BI01 Phys.Rev. C 85, 014313 (2012) D.Bianco, F.Knapp, N.Lo Iudice, F.Andreozzi, A.Porrino Upgraded formulation of the nuclear eigenvalue problem in a microscopic multiphonon basis NUCLEAR STRUCTURE 16O; calculated E1 strength function and cross section, isoscalar E2 reduced strength, phonon structure of 0+, 1- and 2+ states. Equation of motion method; eigenvalue problem in multiphonon space in terms of Tamm-Dancoff phonons, and Nilsson or Hartree-Fock basis. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.014313
2012BI04 Phys.Rev. C 85, 034332 (2012) D.Bianco, F.Andreozzi, N.Lo Iudice, A.Porrino, F.Knapp Importance-sampling diagonalization algorithm for large-scale shell model calculations on N=80 isotones NUCLEAR STRUCTURE 132Te, 134Xe, 136Ba, 138Ce, 140Nd, 142Sm; calculated levels, J, π, B(E2), B(M1), mixed symmetry states. Iterative matrix diagonalization algorithm with an importance sampling, convergence properties. Comparison with experimental data, other shell-model calculations, and systematics of lowest 2+ states in N=80 isotones.
doi: 10.1103/PhysRevC.85.034332
2012BI11 Phys.Rev. C 86, 044325 (2012) D.Bianco, N.Lo Iudice, F.Andreozzi, A.Porrino, F.Knapp Mixed-symmetry states in Te isotopes within a large-scale shell model approach NUCLEAR STRUCTURE 126,128,130,132Te; calculated levels, B(E2), B(M1), using large-scale shell model calculations with a new diagonalization algorithm. Mixed symmetry states. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.044325
2012BI12 Phys.Rev. C 86, 044327 (2012) D.Bianco, F.Knapp, N.Lo Iudice, F.Andreozzi, A.Porrino, P.Vesely Electric dipole response in 208Pb within a new microscopic multiphonon approach NUCLEAR STRUCTURE 208Pb; calculated dipole resonances, E1 σ(ω), B(E1) for giant and pygmy dipole resonances (GDR and PDR) using the microscopic multiphonon approach with a new equation of motion phonon method. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.044327
2012BI17 J.Phys.:Conf.Ser. 366, 012004 (2012) D.Bianco, F.Andreozzi, N.Lo Iudice, A.Porrino, F.Knapp Complex nuclear spectra in a large scale shell model approach NUCLEAR STRUCTURE 130,131,132,133,134Xe; calculated level energy, B(E2), B(M1). 132,133,134Xe calculated low-energy states energy, J, π, γ transitions. 130Xe calculated energy spectrum. Compared to data.
doi: 10.1088/1742-6596/366/1/012004
2012KN03 J.Phys.:Conf.Ser. 337, 012028 (2012) F.Knapp, D.Bianco, N.Lo Iudice, F.Andreozzi, A.Porrino Multiphonon nuclear response in 16O: A microscopic treatment equivalent to shell model NUCLEAR STRUCTURE 16O; calculated energy levels, γ E1 strength distribution using multiphonon states built on Tamm-Dancoff phonons.
doi: 10.1088/1742-6596/337/1/012028
2012LO17 J.Phys.:Conf.Ser. 366, 012031 (2012) N.Lo Iudice, D.Bianco, F.Knapp, F.Andreozzi, A.Porrino, P.Vesely Multiphonon Approaches to Complex Spectroscopy
doi: 10.1088/1742-6596/366/1/012031
2011BI07 Phys.Rev. C 84, 024310 (2011) D.Bianco, F.Andreozzi, N.Lo Iudice, A.Porrino, F.Knapp Matrix diagonalization algorithm and its applicability to the nuclear shell model NUCLEAR STRUCTURE 130,132,134Xe; calculated levels, J, B(E2), B(M1). New matrix diagonalization algorithm, shell model calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.024310
2011BI11 J.Phys.:Conf.Ser. 312, 092018 (2011) D.Bianco, F.Andreozzi, N.Lo Iudice, A.Porrino, F.Knapp A new algorithm for large scale shell model calculations and its applicability to medium-heavy and neutron rich nuclei NUCLEAR STRUCTURE 128Te; calculated low-lying states E, J, π, B(E2) using large-scale shell model.
doi: 10.1088/1742-6596/312/9/092018
2010LO13 J.Phys.:Conf.Ser. 205, 012008 (2010) N.Lo Iudice, F.Andreozzi, F.Knapp, A.Porrino, J.Kvasil Role of multiphonon configurations in nuclear spectra and responses: A new approach NUCLEAR STRUCTURE 16O; calculated levels, J, π, Eλ distributions using EMPM (Equation of Motion Phonon Method), Tamm-Dancoff approximation, RPA. Compared with data.
doi: 10.1088/1742-6596/205/1/012008
2009AN13 Int.J.Mod.Phys. E18, 944 (2009) F.Andreozzi, F.Knapp, N.Lo Iudice, A.Porrino, J.Kvasil A new equation of motion method for multiphonon nuclear spectra NUCLEAR STRUCTURE 16O; calculated level properties: J, π, multi-phonon states.
doi: 10.1142/S0218301309013087
2009PO05 Appl.Radiat.Isot. 67, 1158 (2009) B.Ponsard, S.C.Srivastava, L.F.Mausner, F.F.Knapp, M.A.Garland, S.Mirzadeh Production of Sn-117m in the BR2 high-flux reactor NUCLEAR REACTIONS 117Sn(n, nγ), E=fast; Measured yield. BR2 reactor, Inductively Coupled Plasma Mass Spectrometry (ICPMS).
doi: 10.1016/j.apradiso.2009.02.023
2008AN12 Phys.Rev. C 78, 054308 (2008) F.Andreozzi, F.Knapp, N.Lo Iudice, A.Porrino, J.Kvasil Multiphonon nuclear response in 16O: A microscopic treatment equivalent to the shell model NUCLEAR STRUCTURE 16O; calculated E1, E2, E3 transition strengths, level energies.
doi: 10.1103/PhysRevC.78.054308
2008KV01 Int.J.Mod.Phys. E17, 196 (2008) J.Kvasil, N.Lo Iudice, F.Andreozzi, A.Porrino, F.Knapp Collective bands in superdeformed nuclei NUCLEAR STRUCTURE 152Dy, 190Hg; analyzed superdeformed bands, and strength of E1 transitions using Cranked Nilsson + QRPA Model.
doi: 10.1142/S0218301308009690
2007AN05 Int.J.Mod.Phys. E16, 580 (2007) F.Andreozzi, N.Lo Iudice, A.Porrino, F.Knapp, J.Kvasil An exact microscopic multiphonon approach to nuclear collective excitations NUCLEAR STRUCTURE 16O; calculated E1 and E2 strength distributions.
doi: 10.1142/S0218301307006022
2007AN13 Phys.Rev. C 75, 044312 (2007) F.Andreozzi, F.Knapp, N.Lo Iudice, A.Porrino, J.Kvasil Exact formulation and solution of the nuclear eigenvalue problem in a microscopic multiphonon space NUCLEAR STRUCTURE 16O; calculated levels, J, π, E3 strength distribution. Tamm-Dancoff phonons.
doi: 10.1103/PhysRevC.75.044312
2007AN15 Prog.Part.Nucl.Phys. 59, 259 (2007) F.Andreozzi, F.Knapp, N.Lo Iudice, A.Porrino, J.Kvasil A new exact microscopic multiphonon approach to the nuclear eigenvalue problem NUCLEAR STRUCTURE 16O; calculated E2 reduced strength, Isovector E1 strength and Isoscalar dipole strength distributions using an exact microscopic multiphonon approach to the nuclear eigenvalue problem.
doi: 10.1016/j.ppnp.2006.12.007
2007AN24 Nucl.Phys. A788, 20c (2007) F.Andreozzi, N.Lo Iudice, A.Porrino, F.Knapp, J.Kvasil An exact microscopic multiphonon approach to collective modes in nuclei NUCLEAR STRUCTURE 16O; calculated E1 strength distribution. Tamm-Dancoff phonons.
doi: 10.1016/j.nuclphysa.2007.01.003
2007KV02 Phys.Rev. C 75, 034306 (2007) J.Kvasil, N.Lo Iudice, F.Andreozzi, F.Knapp, A.Porrino Microscopic structure of deformed and superdeformed collective bands in rotating nuclei NUCLEAR STRUCTURE 190,192,194Hg, 152Dy; calculated deformed and superdeformed rotational bands energies, configurations, strength distributions for linking transitions. Cranked Nilsson plus quasiparticle RPA approach.
doi: 10.1103/PhysRevC.75.034306
2006KV02 Phys.Rev. C 73, 034302 (2006) J.Kvasil, N.Lo Iudice, F.Andreozzi, F.Knapp, A.Porrino Shape transitions and collective excitations in 152Dy NUCLEAR STRUCTURE 152Dy; calculated deformation, superdeformation, rotational bands moments of inertia, B(E1), B(E0), B(M1) distributions; deduced scissors mode. Self-consistent cranked Nilsson plus quasiparticle RPA approach.
doi: 10.1103/PhysRevC.73.034302
2004KV02 Phys.Rev. C 69, 064308 (2004) J.Kvasil, N.Lo Iudice, R.G.Nazmitdinov, A.Porrino, F.Knapp Collective magnetic excitations and backbending in fast rotating nuclei NUCLEAR STRUCTURE 156Dy, 158Er; calculated deformation vs spin, electromagnetic strength functions, collective magnetic dipole excitations, rotational band backbending features. Cranked Nilsson plus RPA approach.
doi: 10.1103/PhysRevC.69.064308
1997MI09 Appl.Radiat.Isot. 48, 441 (1997) S.Mirzadeh, F.F.Knapp, Jr., C.W.Alexander, L.F.Mausner Evaluation of Neutron Inelastic Scattering for Radioisotope Production NUCLEAR REACTIONS 117,119Sn, 195Pt(n, n'), 194Pt, 116Sn(n, γ), 118,120Sn(n, 2n), 196Pt(n, 2n), E=reactor; measured isomer production σ; deduced inelastic scattering, neutron scattering, capture production differences.
doi: 10.1016/S0969-8043(96)00284-9
1997MI27 Radiochim.Acta 77, 99 (1997) S.Mirzadeh, F.F.Knapp, Jr., R.M.Lambrecht Burn-Up Cross-Section of 188W NUCLEAR REACTIONS 188W(n, γ), E=reactor; measured burn-up σ. Radioactive target. RADIOACTIVITY 189W(β-) [from 188W irradiation]; measured Eγ, Iγ, T1/2. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31499. 1996HS01 Appl.Radiat.Isot. 47, 23 (1996) B.-T.Hsieh, A.P.Callahan, A.L.Beets, G.Ting, F.F.R.Knapp, Jr. Ascorbic Acid/Saline Eluant Increases 188Re Yields after ' Wet ' Storage of 188W/188Re Generators RADIOACTIVITY 188W(β-) [from 186W neutron irradiation]; measured 188Re eluant yields; deduced yield increase conditions. ' Wet ' storage of 188W/188Re generators.
doi: 10.1016/0969-8043(95)00255-3
1994KN05 Appl.Radiat.Isot. 45, 1123 (1994) F.F.R.Knapp, Jr., A.P.Callahan, A.L.Beets, S.Mirzadeh, B.-T.Hsieh Processing of Reactor-Produced 188W for Fabrication of Clinical Scale Alumina-Based 188W/188Re Generators RADIOACTIVITY 188W(β-) [from double neutron capture on 186W]; measured specific activity vs time for 186W irradiation; deduced clinical scale Alumina-based 188W/188Re generators fabrication implications.
doi: 10.1016/0969-8043(94)90026-4
1994MI30 J.Labelled Compd.Radiopharm. 35, 273 (1994) S.Mirzadeh, E.Hetherington, F.F.Knapp, Jr., R.M.Lambrecht Carrier-Free 166Ho from 166Dy/166Ho Biomedical Generator System NUCLEAR REACTIONS Dy(n, γ), E=reactor; measured 166Dy yields from double neutron capture on 164Dy; deduced 166Ho specific activity following 166Dy decay.
1992CA17 Appl.Radiat.Isot. 43, 801 (1992) A.P.Callahan, D.E.Rice, D.W.McPherson, S.Mirzadeh, F.F.Knapp, Jr. The Use of Alumina ' SepPaks ' as a Simple Method for the Removal and Determination of Tungsten-188 Breakthrough from Tungsten-188/Rhenium-188 Generators RADIOACTIVITY 188W(β-) [from double neutron capture on 186W]; 188Re(β-) [from 188W(β-decay)]; measured Eγ, Iγ. Removal, determination of 188W breakthrough levels, 188W/188Re generators.
doi: 10.1016/0883-2889(92)90245-A
1989BR04 J.Labelled Compd.Radiopharm. 26, 162 (1989) C.Brihaye, M.Guillaume, F.F.Knapp, Jr., S.Dewez, D.E.Rice, A.P.Callahan Neutron Production of Os-191 and Separation from Ir-192 for a Medical Os-191/Ir-191m Generator NUCLEAR REACTIONS 190Os, 191Ir(n, γ), E=reactor; measured residual production σ.
doi: 10.1002/jlcr.2580260170
1989BR12 Appl.Radiat.Isot. 40, 183 (1989) C.Brihaye, S.Dewez, M.Guillaume, A.P.Callahan, D.E.Rice, F.F.Knapp, Jr. Reactor Production and Purification of Osmium-191 for Use in a New 191Os/191mIr Radionuclide Generator System NUCLEAR REACTIONS 190Os(n, γ), E=thermal; measured residual production yield.
doi: 10.1016/0883-2889(89)90196-2
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