NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = S.A.Wender Found 69 matches. 2015HA01 Nucl.Data Sheets 123, 130 (2015) R.C.Haight, C.Y.Wu, H.Y.Lee, T.N.Taddeucci, B.A.Perdue, J.M.O'Donnell, N.Fotiades, M.Devlin, J.L.Ullmann, T.A.Bredeweg, M.Jandel, R.O.Nelson, S.A.Wender, D.Neudecker, M.E.Rising, S.Mosby, S.Sjue, M.C.White, B.Bucher, R.Henderson The LANL/LLNL Prompt Fission Neutron Spectrum Program at LANSCE and Approach to Uncertainties NUCLEAR REACTIONS 239Pu(n, F), E<15 MeV; analyzed available data; deduced possible prompt fission neutron spectra σ, yields, correlation matrices.
doi: 10.1016/j.nds.2014.12.023
2015TA03 Nucl.Data Sheets 123, 135 (2015) T.N.Taddeucci, R.C.Haight, H.Y.Lee, D.Neudecker, J.M.O'Donnell, M.C.White, B.A.Perdue, M.Devlin, N.Fotiadis, J.L.Ullmann, R.O.Nelson, T.A.Bredeweg, M.E.Rising, S.K.Sjue, S.A.Wender, C.Y.Wu, R.Henderson Multiple-scattering Corrections to Measurements of the Prompt Fission Neutron Spectrum NUCLEAR REACTIONS 239Pu(n, F), E<15 MeV; analyzed available data; deduced response functions, the shape of the prompt fission neutron spectrum.
doi: 10.1016/j.nds.2014.12.024
2015WA26 Phys.Rev. C 92, 024620 (2015) B.S.Wang, E.B.Norman, N.D.Scielzo, A.R.Smith, K.J.Thomas, S.A.Wender Cosmogenic-neutron activation of TeO2 and implications for neutrinoless double-β decay experiments NUCLEAR REACTIONS Te, O(n, X)7Be/60Co/101Rh/101mRh/102mRh/105Ag/106mAg/110Ag/110mAg/111Ag/111In/114mIn/113Sn/117mSn/118Sb/119Sb/120mSb/122Sb/124Sb/125Sb/126Sb/127Sb/131mXe/118Te/119mTe/121Te/121mTe/123mTe/125mTe/127Te/127mTe/129Te/129mTe/131Te/131mTe, E<800 MeV from LANSCE-LANL facility; measured off-line Eγ, Iγ at Low Background Facility of LBNL; deduced flux-averaged cross sections; estimated cosmogenic-activation background from 110Ag and 60Co in connection with 130Te 0νββ-decay experiments at CUORE and SNO-2. Benchmarking by GEANT4 simulations. Comparison of measured σ with calculations using ACTIVIA code based on Silberberg and Tsao (S and T) semiempirical formulas.
doi: 10.1103/PhysRevC.92.024620
2014HA27 Nucl.Data Sheets 119, 205 (2014) R.C.Haight, H.Y.Lee, T.N.Taddeucci, J.M.O'Donnell, B.A.Perdue, N.Fotiades, M.Devlin, J.L.Ullmann, A.Laptev, T.Bredeweg, M.Jandel, R.O.Nelson, S.A.Wender, M.C.White, C.Y.Wu, E.Kwan, A.Chyzh, R.Henderson, J.Gostic The Prompt Fission Neutron Spectrum (PFNS) Measurement Program at LANSCE
doi: 10.1016/j.nds.2014.08.057
2014KW05 Nucl.Data Sheets 119, 221 (2014) E.Kwan, C.Y.Wu, R.C.Haight, H.Y.Lee, T.A.Bredeweg, A.Chyzh, M.Devlin, N.Fotiades, J.M.Gostic, R.A.Henderson, M.Jandel, A.Laptev, R.O.Nelson, J.M.O'Donnell, B.A.Perdue, T.N.Taddeucci, J.L.Ullmann, S.A.Wender Prompt Fission γ-rays Measured Using Liquid Scintillators NUCLEAR REACTIONS 235U(n, F), E=1-20 MeV; measured prompt Eγ, Iγ, γγ-coin using FIGARO; deduced γ-ray spectrum, unfolded using SVD and iterative Bayesian techniques. Compared to 235Cf(SF). RADIOACTIVITY 235Cf(SF); measured prompt Eγ, Iγ, γγ-coin using FIGARO; deduced γ-ray spectrum, unfolded using SVD and iterative Bayesian techniques. Compared to 235U(n, F).
doi: 10.1016/j.nds.2014.08.061
2014PE14 Nucl.Data Sheets 119, 371 (2014) B.A.Perdue, T.N.Taddeucci, R.C.Haight, T.Bredeweg, M.Devlin, N.Fotiades, M.Jandel, A.Laptev, H.Y.Lee, R.O.Nelson, J.M.O'Donnell, J.L.Ullmann, S.A.Wender, C.Y.Wu, E.Kwan, A.Chyzh, R.A.Henderson, J.M.Gostic Development of an Array of Liquid Scintillators to Measure the Prompt Fission Neutron Spectrum at LANSCE
doi: 10.1016/j.nds.2014.08.102
2013BA03 Nucl.Instrum.Methods Phys.Res. B295, 16 (2013) A.F.Barghouty, C.Brofferio, S.Capelli, M.Clemenza, O.Cremonesi, S.Cebrian, E.Fiorini, R.C.Haight, E.B.Norman, M.Pavan, E.Previtali, B.J.Quiter, M.Sisti, A.R.Smith, S.A.Wender Measurements of proton-induced radionuclide production cross sections to evaluate cosmic-ray activation of tellurium NUCLEAR REACTIONS Te(p, X)54Mn/57Co/60Co/65Zn/75Se/88Y/102Rh/110Ag/113Sn/46Sc/48V/56Co/58Co/59Fe/83Rb/84Rb/85Sr/88Zr/87Y/95Nb/89Zr/92Nb/95Nb/95Tc/100Pd/103Ru/105Ag/111In/114In, E=0.8, 1.4, 23 GeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with calculations and available data.
doi: 10.1016/j.nimb.2012.10.008
2012KW01 Nucl.Instrum.Methods Phys.Res. A688, 55 (2012) E.Kwan, C.Y.Wu, R.C.Haight, H.Y.Lee, T.A.Bredeweg, A.Chyzh, M.Devlin, N.Fotiades, J.M.Gostic, R.A.Henderson, M.Jandel, A.Laptev, R.O.Nelson, J.M.O'Donnell, B.A.Perdue, T.N.Taddeucci, J.L.Ullmann, S.A.Wender Prompt energy distribution of 235U(n, f)γ at bombarding energies of 1-20 MeV NUCLEAR REACTIONS 235U(n, F), E=1-20 MeV; measured reaction products, Eγ, Iγ; deduced prompt γ-rays distribution. Comparison with GEANT4 simulations. RADIOACTIVITY 252Cf(SF); measured decay products, Eγ, Iγ; deduced prompt γ-rays distribution. Comparison with GEANT4 simulations.
doi: 10.1016/j.nima.2012.06.003
2007SA14 Phys.Rev. C 75, 031001 (2007) Y.Safkan, T.Akdogan, W.A.Franklin, J.L.Matthews, W.M.Schmitt, V.V.Zelevinsky, P.A.M.Gram, T.N.Taddeucci, S.A.Wender, S.F.Pate Differential cross section for neutron-proton bremsstrahlung NUCLEAR REACTIONS 1H(n, n'γ), E=175-275 MeV; measured Ep, En, σ(θ(n), θ(p), θ(γ)). Comparison with relativistic soft-photon and nonrelativistic models.
doi: 10.1103/PhysRevC.75.031001
2006RO22 Nucl.Instrum.Methods Phys.Res. A562, 771 (2006) C.Romano, Y.Danon, R.C.Haight, S.A.Wender, D.J.Vieira, E.M.Bond, R.S.Rundberg, J.B.Wilhelmy, J.M.O'Donnell, A.F.Michaudon, T.A.Bredeweg, D.Rochman, T.Granier, T.Ethvignot Measurements of (n, α) cross-section of small samples using a lead-slowing-down-spectrometer NUCLEAR REACTIONS 6Li(n, α), E ≈ 0.1-10000 eV; measured Eα, σ(E). Lead-slowing-down spectrometer.
doi: 10.1016/j.nima.2006.02.052
2006RO28 Nucl.Instrum.Methods Phys.Res. A564, 400 (2006) D.Rochman, R.C.Haight, J.M.O'Donnell, S.A.Wender, D.J.Vieira, E.M.Bond, T.A.Bredeweg, J.B.Wilhelmy, T.Granier, T.Ethvignot, M.Petit, Y.Danon, C.Romano Cross-section measurements for 239Pu(n, f) and 6Li(n, α) with a lead slowing-down spectrometer NUCLEAR REACTIONS 239Pu(n, F), E < 100 keV; measured fission σ. 6Li(n, α), E < 10 keV; measured σ. Lead slowing-down spectrometer.
doi: 10.1016/j.nima.2006.03.032
2005NO04 Nucl.Phys. B(Proc.Supp.) S143, 508 (2005) E.B.Norman, A.R.Smith, A.F.Barghouty, R.C.Haight, S.A.Wender Cosmic-Ray Production of 60Co in Double Beta-Decay Source Materials NUCLEAR REACTIONS Ge, Mo, Te(p, X)60Co, E=0.8, 1.85 GeV; measured production σ. Comparison with model predictions.
doi: 10.1016/j.nuclphysbps.2005.01.173
2005RO30 Nucl.Instrum.Methods Phys.Res. A550, 397 (2005) D.Rochman, R.C.Haight, J.M.O'Donnell, A.Michaudon, S.A.Wender, D.J.Vieira, E.M.Bond, T.A.Bredeweg, A.Kronenberg, J.B.Wilhelmy, T.Ethvignot, T.Granier, M.Petit, Y.Danon Characteristics of a lead slowing-down spectrometer coupled to the LANSCE accelerator NUCLEAR REACTIONS 235U, 239Pu(n, F), E < 100 keV; measured fission σ. Lead slowing-down spectrometer.
doi: 10.1016/j.nima.2005.04.075
1995BR14 Phys.Lett. 349B, 272 (1995) F.P.Brady, J.L.Romero, D.R.Mayo, J.E.Koster, R.O.Nelson, S.A.Wender ' Photon Spectrum of the Neutron-Proton Bremsstrahlung at 170 MeV ': Contributions of np → dγ to inclusive photon energy spectra from np and pd collisions near 200 MeV NUCLEAR REACTIONS 1H(n, γ), E=170 MeV; 2H(p, γ), E=195, 200 MeV; analyzed σ(θ, Eγ) data; deduced capture process role in reaction, implications to free np bremsstrahlung.
doi: 10.1016/0370-2693(95)00209-4
1994VO16 Phys.Rev. C50, 1952 (1994) H.Vonach, A.Pavlik, M.B.Chadwick, R.C.Haight, R.O.Nelson, S.A.Wender, P.G.Young 207,208Pb(n, xnγ) Reactions for Neutron Energies from 3 to 200 MeV NUCLEAR REACTIONS 207,208Pb(n, xn), E=3-200 MeV; measured Eγ, Iγ; calculated γ production σ(E), x ≤ 9; deduced multiple preequilibrium emission role. Exciton, Hauser-Feshbach, coupled-channels models.
doi: 10.1103/PhysRevC.50.1952
1993KO53 Nucl.Instrum.Methods Phys.Res. B79, 297 (1993) J.E.Koster, R.O.Nelson, M.E.Schillaci, S.A.Wender, D.Mayo, F.P.Brady, J.Romero, D.Krofcheck, M.Blann, P.Anthony, V.R.Brown, L.Hansen, B.Pohl, T.C.Sangster, H.Nifenecker, J.A.Pinston Neutron-Proton Bremsstrahlung Experiments NUCLEAR REACTIONS 1H(n, γ), E=138-401 MeV; measured γ rays. Tof techniques.
doi: 10.1016/0168-583X(93)95348-9
1993RO25 Nucl.Instrum.Methods Phys.Res. A326, 549 (1993) N.R.Roberson, C.D.Bowman, J.D.Bowman, P.P.J.Delheij, C.M.Frankle, C.R.Gould, D.G.Haase, J.N.Knudson, G.E.Mitchell, R.N.Mortensen, S.I.Penttila, H.Postma, S.J.Seestrom, J.J.Szymanski, S.A.Wender, S.H.Yoo, V.W.Yuan, X.Zhu An Apparatus and Techniques of Tests for Fundamental Symmetries in Compound-Nucleus Scattering with Epithermal Polarized Neutron Beams NUCLEAR REACTIONS 238U(polarized n, X), E=5-300 eV; measured neutron transmission. 239U resonance deduced average parity violating asymmetry.
doi: 10.1016/0168-9002(93)90858-F
1993WE13 Nucl.Instrum.Methods Phys.Res. A336, 226 (1993) S.A.Wender, S.Balestrini, A.Brown, R.C.Haight, C.M.Laymon, T.M.Lee, P.W.Lisowski, W.McCorkle, R.O.Nelson, W.Parker, N.W.Hill A Fission Ionization Detector for Neutron Flux Measurements at a Spallation Source
doi: 10.1016/0168-9002(93)91102-S
1992CO16 Nucl.Phys. A545, 785 (1992) H.Conde, N.Olsson, E.Ramstrom, T.Ronnqvist, R.Zorro, J.Blomgren, A.Hakansson, G.Tibell, O.Jonsson, L.Nilsson, P.-U.Renberg, M.Osterlund, W.Unkelbach, J.Wambach, S.Y.van der Werf, J.Ullmann, S.A.Wender The 90Zr(n, p)90Y Reaction at E(n) = 98 MeV NUCLEAR REACTIONS 90Zr(n, p), E=98 MeV; measured σ(Ep, θ). 90Y deduced Gamow-Teller, other multipole strengths. Statistical multistep direct, DWBA calculations, multipole decomposition, comparison with RPA-DWIA calculations.
doi: 10.1016/0375-9474(92)90530-W
1992LA20 Phys.Rev. C46, 1880 (1992) C.M.Laymon, R.O.Nelson, S.A.Wender, L.R.Nilsson Isovector Giant Quadrupole Resonance in the 40Ca(n, γ0) Reaction NUCLEAR REACTIONS 40Ca(n, γ), E=8-44 MeV; measured σ(θ) vs E, γ-asymmetry. 41Ca deduced isovector GQR parameters.
doi: 10.1103/PhysRevC.46.1880
1992LY01 Phys.Rev. C45, 308 (1992) C.R.Lyndon, H.O.Funsten, C.F.Perdrisat, V.Punjabi, J.M.Finn, B.J.Lieb, C.E.Stronach, N.L.Fuqua, H.S.Plendl, J.R.Mackenzie, R.Nair, J.R.Comfort, R.A.Giannelli, J.J.Reidy, L.Redmond, P.E.Koehler, S.A.Wender Coincidence Analyzing-Power Measurements of the Reaction 12C(p(pol), p'γ)12C(*) Through the 15.11-MeV State NUCLEAR REACTIONS 12C(polarized p, p'γ), E=318 MeV; measured coincidence analyzing powers vs φp. Relativistic, non-relativistic DWBA.
doi: 10.1103/PhysRevC.45.308
1991NE07 Nucl.Instrum.Methods Phys.Res. B56/57, 451 (1991) R.O.Nelson, C.M.Laymon, S.A.Wender High-Resolution Inelastic Gamma-Ray Measurements with a White Neutron Source from 1 to 200 MeV NUCLEAR REACTIONS 56Fe(n, X), E=27.1-29 MeV; measured Eγ, Iγ for X=2n, n, np, 3n, nα. 56Fe(n, n'), (n, 2n), E ≤ 200 MeV; measured σ(θ) vs E. White neutron source.
doi: 10.1016/0168-583X(91)96068-V
1990HA19 Phys.Rev. C41, 2556 (1990) A.Hakansson, A.Lindholm, L.Nilsson, J.Blomgren, P.-O.Soderman, D.M.Drake, S.A.Wender, N.Olsson 12C(n, γ0)13C Cross Section in the 8-11 MeV Region NUCLEAR REACTIONS 12C(n, γ), E=8-11 MeV; measured σ(θ=90°).
doi: 10.1103/PhysRevC.41.2556
1988KO03 Phys.Rev. C37, 917 (1988) P.E.Koehler, C.D.Bowman, F.J.Steinkruger, D.C.Moody, G.M.Hale, J.W.Starner, S.A.Wender, R.C.Haight, P.W.Lisowski, W.L.Talbert 7Be(n, p)7Li Total Cross Section from 25 MeV to 13.5 keV NUCLEAR REACTIONS 7Be(n, p), E=0.025-13500 eV; measured σ. 8Be levels deduced Γp, Γn, Γ. Calculated astrophysical reaction rate. R-matrix analysis.
doi: 10.1103/PhysRevC.37.917
1988MU06 J.Phys.(London) G14, Supplement S275 (1988) T.Murakami, C.A.Gossett, I.Halpern, D.P.Rosenzweig, D.W.Storm, D.R.Tieger, P.T.Debevec, A.Freytag, L.J.Morford, S.A.Wender, D.H.Dowell Photoneutron Studies of the Giant Isovector Quadrupole Resonance in Calcium, Cadmium, and Lead NUCLEAR REACTIONS Ca, Cd, Pb(γ, n), E=28-39 MeV bremsstrahlung; measured σ(θ), neutron asymmetry; deduced electric dipole, quadrupole amplitude interference role.
doi: 10.1088/0305-4616/14/S/029
1988RA12 Nucl.Sci.Eng. 98, 348 (1988) P.Ramakrishnan, G.E.Mitchell, C.R.Gould, S.A.Wender, G.F.Auchampaugh Photon Production Cross Section for 181Ta NUCLEAR REACTIONS 181Ta(n, X), E=2-100 MeV; measured photon production σ(E, Eγ); deduced σ(E).
doi: 10.13182/NSE88-A23535
1988RA13 Nucl.Sci.Eng. 98, 357 (1988) P.Ramakrishnan, G.E.Mitchell, C.R.Gould, S.A.Wender, G.F.Auchampaugh, R.C.Little Neutron-Induced Photon Production Cross Sections NUCLEAR REACTIONS Ta(n, X), E < 20 MeV; measured Eγ, Iγ, photon production σ(E, Eγ); deduced σ(E).
doi: 10.13182/NSE88-A23536
1988WE06 J.Phys.(London) G14, Supplement S417 (1988) S.A.Wender, S.J.Seestrom-Morris, R.O.Nelson A White Neutron Source from 1 to 400 MeV NUCLEAR REACTIONS 12C(n, n'γ), E=5-25 meV; measured σ(E).
doi: 10.1088/0305-4616/14/S/041
1987MU02 Phys.Rev. C35, 479 (1987) T.Murakami, I.Halpern, D.W.Storm, P.T.Debevec, L.J.Morford, S.A.Wender, D.H.Dowell Forward-to-Backward Asymmetry of the (γ, n) Reaction in the Energy Range 20-30 MeV NUCLEAR REACTIONS Cd, Pb, 206Pb(γ, n), E=20-30 MeV; measured σ(Eγ, θ), asymmetries. Cd, Pb deduced E2 isovector resonance excitation energies, widths. Liquid scintillator. Direct-semidirect calculations.
doi: 10.1103/PhysRevC.35.479
1987ST26 Can.J.Phys. 65, 677 (1987) D.W.Storm, I.Halpern, C.A.Gossett, T.Murakami, D.P.Rosenzweig, D.R.Tieger, P.T.Debevec, A.Freytag, L.J.Morford, S.A.Wender, D.H.Dowell (γ, n) Studies of the Giant Isovector E2 Resonance in Lead, Cadmium, and Calcium NUCLEAR REACTIONS Ca, Cd, Pb(γ, n), E=20-40 MeV; measured σ(En), σ(θn), asymmetries; deduced giant isovector, quadrupole resonance parameters. Natural targets. Direct semdirect calculations.
doi: 10.1139/p87-096
1986BE17 Nucl.Phys. A456, 426 (1986) I.Bergqvist, D.M.Drake, D.K.McDaniels, S.A.Wender, A.Lindholm, L.Nilsson, N.Olsson, R.Zorro, F.S.Dietrich The 12C(n, γ0)13C Reaction in the Giant Resonance Region NUCLEAR REACTIONS 12C(n, γ), E=7-19.5 MeV; measured σ(E, θ=90°). 13C deduced giant, pygmy resonances. DSD model, 12,13C(n, γ) data input.
doi: 10.1016/0375-9474(86)90403-3
1986GO14 Radiat.Eff. 92, 139 (1986) C.R.Gould, J.Dave, G.E.Mitchell, P.Ramakrishnan, G.F.Auchampaugh, R.C.Little, S.A.Wender Photon Production Cross Section Measurements for Ta and Be NUCLEAR REACTIONS Ta, 9Be(n, γ), E=2-25 MeV; measured γ-ray production σ.
doi: 10.1080/00337578608208307
1986LI14 Radiat.Eff. 95, 239 (1986) P.W.Lisowski, S.A.Wender, G.F.Auchampaugh The WNR/PSR Facility - Neutron Physics Capabilities from Sub-Thermal to 800 MeV NUCLEAR REACTIONS 12C(p, n), E at 1050 MeV/c; measured σ(θ) vs neutron momentum.
doi: 10.1080/00337578608208702
1986MO05 Phys.Rev. C33, 1224 (1986) G.L.Morgan, P.W.Lisowski, S.A.Wender, R.E.Brown, N.Jarmie, J.F.Wilkerson, D.M.Drake Measurement of the Branching Ratio 3H(d, γ)/3H(d, n) using Thick Tritium Gas Targets NUCLEAR REACTIONS, ICPND 3H(d, γ), (d, n), E=0.0-0.72 MeV; measured Eγ, Iγ, En, relative γ yield. 5He resonance deduced branching ratio.
doi: 10.1103/PhysRevC.33.1224
1985DY01 Phys.Rev. C31, 240 (1985) P.Dyer, A.M.Sabbas, S.A.Wender Laser Spectroscopy of the Transitional Nucleus 151Sm RADIOACTIVITY 151Sm(β-); measured hfs, isotope shifts; deduced μ, quadrupole moment. 151,152Sm deduced rms radius variation. Muonic atom King plot, atomic beam resonance-fluorescence technique.
doi: 10.1103/PhysRevC.31.240
1984WE11 Nucl.Instrum.Methods 220, 371 (1984) S.A.Wender, G.F.Auchampaugh, J.F.Wilkerson, N.W.Hill, L.R.Nilsson, N.R.Roberson A High-Energy Gamma-Ray Detector System for Fast Neutron-Induced Reactions NUCLEAR REACTIONS 12C(n, n'), E=4.9-100 MeV; measured γ-spectra, σ(θγ) vs E. 40Ca(n, γ), E=2-20 MeV; measured absolute σ(θγ=90°) vs E. Pulsed neutron source, bismuth germanate crystal detector.
doi: 10.1016/0167-5087(84)90298-9
1983DR13 Nucl.Phys. A410, 429 (1983) D.M.Drake, N.R.Roberson, S.A.Wender, H.R.Weller Polarized Triton Capture on 12C NUCLEAR REACTIONS 12C(t, γ), (polarized t, γ), E=2.3-6.5 MeV; measured σ(E, θ), A(θ). Direct capture model calculation.
doi: 10.1016/0375-9474(83)90635-8
1983GU03 Nucl.Phys. A395, 1 (1983) P.P.Guss, K.Murphy, R.C.Byrd, C.E.Floyd, S.A.Wender, R.L.Walter, T.B.Clegg, W.Wylie The Analyzing Power for the 2H(d, n)3He(g.s.) Reaction from 5.5 to 11.5 MeV NUCLEAR REACTIONS 2H(polarized d, n), E=5.5, 7, 8.5, 10, 11.5 MeV; measured A(θ). Report discrepancies with previous measurements. Polynomial expansions analysis.
doi: 10.1016/0375-9474(83)90085-4
1983WO02 Nucl.Phys. A394, 139 (1983) E.Woye, W.Tornow, G.Mack, C.E.Floyd, P.P.Guss, K.Murphy, R.C.Byrd, S.A.Wender, R.L.Walter, T.B.Clegg, W.Wylie The Analyzing Power A(y)(θ) for 12C(n, n0, 1)12C between 8.9 and 14.9 MeV Neutron Energy NUCLEAR REACTIONS 12C(n, n), (n, n'), E=8.9-14.9 MeV; measured A(E, θ); deduced optical potential parameters. 12C level deduced quadrupole deformation.
doi: 10.1016/0375-9474(83)90167-7
1982BA18 Phys.Rev.Lett. 48, 1461 (1982) Effect of Laser Radiation on the Decay of 235mU RADIOACTIVITY 235mU; calculated electron configuration dependence of T1/2, internal conversion probability. Laser induced atomic excitation.
doi: 10.1103/PhysRevLett.48.1461
1982DA21 Nucl.Instrum.Methods 200, 285 (1982) J.H.Dave, C.R.Gould, S.A.Wender, S.M.Shafroth The 1H(7Li, n)7Be Reaction as an Intense MeV Neutron Source NUCLEAR REACTIONS 1H(7Li, n), E=13.15-22 MeV; measured σ(θ) vs E. Tof.
doi: 10.1016/0167-5087(82)90444-6
1982FL01 Phys.Rev. C25, 1682 (1982) C.E.Floyd, P.P.Guss, K.Murphy, C.R.Howell, R.C.Byrd, G.Tungate, S.A.Wender, R.L.Walter, T.B.Clegg Analyzing Powers for Neutron Elastic Scattering at Forward Angles NUCLEAR REACTIONS 40Ca, 54Fe, 65Cu, 120Sn, 208Pb(polarized n, n), E=14 MeV; measured A(θ).
doi: 10.1103/PhysRevC.25.1682
1982TO11 Nucl.Phys. A385, 373 (1982) W.Tornow, E.Woye, G.Mack, C.E.Floyd, K.Murphy, P.P.Guss, S.A.Wender, R.C.Byrd, R.L.Walter, T.B.Clegg, H.Leeb Analyzing Power and Differential Cross Section at 9.9, 11.9 and 13.9 MeV for Ca(n, n)Ca NUCLEAR REACTIONS 40Ca(polarized n, n), E=9.9, 11.9, 13.9 MeV; measured A(E, θ), σ(E, θ); deduced optical model parameters, Coulomb correction terms. Optical potential analysis, l-dependence, Fourier-Bessel expansion of the real central potential.
doi: 10.1016/0375-9474(82)90093-8
1982WE01 Phys.Rev. C25, 89 (1982) S.A.Wender, H.R.Weller, N.R.Roberson, D.R.Tilley, R.G.Seyler Neutron Capture in the Giant Resonance Region of 15N NUCLEAR REACTIONS 14N(n, γ), E=5.6-13 MeV; measured σ(θ, E), γ(θ). Direct semi-direct model.
doi: 10.1103/PhysRevC.25.89
1982WE03 Nucl.Instrum.Methods 192, 273 (1982) C.R.Westerfeldt, S.A.Wender, E.G.Bilpuch, G.E.Mitchell, W.K.Wells Measurement of Nuclear E0 Transitions NUCLEAR REACTIONS 72Ge(p, p'e), E=3-4.34 MeV; measured p'e-coin, I(ce)(t), σ(E). 72Ge level deduced T1/2. 73As deduced IAR. Pulsed beam, large solid angle electron detector.
doi: 10.1016/0029-554X(82)90832-1
1981DR08 Phys.Rev.Lett. 47, 1581 (1981) D.M.Drake, S.Joly, L.Nilsson, S.A.Wender, K.Anoil, I.Halpern, D.Storm E2 Isovector Giant Resonance as Seen through the Capture of Fast Neutrons NUCLEAR REACTIONS 208Pb(n, γ), E=7-20 MeV; measured σ(Eγ), asymmetry. 209Pb deduced E2 giant isovector resonance.
doi: 10.1103/PhysRevLett.47.1581
1981FL04 Phys.Rev.Lett. 47, 1042 (1981) C.E.Floyd, P.P.Guss, K.Murphy, R.C.Byrd, G.Tungate, S.A.Wender, R.L.Walter, T.B.Clegg Determination of the Spin-Orbit Interaction for Neutron-Nucleus Scattering NUCLEAR REACTIONS 54Fe, 65Cu(polarized n, n), E=14 MeV; measured σ(θ), A(θ); deduced neutron-nucleus spin-orbit interaction. Optical model.
doi: 10.1103/PhysRevLett.47.1042
1980MC06 Phys.Rev.Lett. 45, 243 (1980) R.C.McBroom, H.R.Weller, S.Manglos, N.R.Roberson, S.A.Wender, D.R.Tilley, D.M.Skopik, L.G.Arnold, R.G.Seyler Evidence for a 2+ Resonance in 4He at 40 MeV NUCLEAR REACTIONS 3H(p, γ), E=17-31 MeV; measured σ(θ, E), asymmetry vs E. 4He(e, t), E not given; measured asymmetry vs E. 4He deduced resonance, J, π, Γ.
doi: 10.1103/PhysRevLett.45.243
1980TU01 Phys.Rev. C21, 525 (1980) J.D.Turner, N.R.Roberson, S.A.Wender, H.R.Weller, D.R.Tilley Polarized Proton Capture on 13C NUCLEAR REACTIONS 13C(polarized p, γ), E=8.05-15.5 MeV; measured σ(θ), A(θ). 13C(p, γ), E=6.24-17.0 MeV; measured σ(90°). 14N deduced E1, E2 amplitudes, phases. direct-semidirect model.
doi: 10.1103/PhysRevC.21.525
1979CA03 Nucl.Phys. A319, 165 (1979) R.R.Cadmus, Jr., T.B.Clegg, E.J.Ludwig, S.A.Wender Spins and Parities of Low-Lying States in 77Kr from the 78Kr(d, t)77Kr Reaction NUCLEAR REACTIONS 78Kr(polarized d, t), E=15.95 MeV; measured σ(θ), A(θ). 77Kr levels deduced J, π, S. Enriched target. DWBA analysis.
doi: 10.1016/0375-9474(79)90178-7
1979JE03 Z.Phys. A291, 609 (1979) M.Jensen, D.R.Tilley, H.R.Weller, N.R.Roberson, S.A.Wender, T.B.Clegg Polarized-Neutron Capture in the Giant-Resonance Region of 41Ca NUCLEAR REACTIONS 40Ca(polarized n, γ), E=10 MeV; measured σ(θ), A(θ). 41Ca deduced E2 contribution in giant dipole region. Legendre polynomial analysis.
1979JE05 Phys.Rev.Lett. 43, 609 (1979) M.Jensen, D.R.Tilley, H.R.Weller, N.R.Robertson, S.A.Wender, T.B.Clegg Polarized-Neutron Capture In The Giant-Resonance Region Of 41Ca NUCLEAR REACTIONS 40Ca(n, γ), E=10 MeV; measured products, Eγ, Iγ; deduced σ(θ), polarization data. Data were imported from EXFOR entry 12708.
doi: 10.1103/PhysRevLett.43.609
1979SK01 Phys.Rev. C19, 601 (1979) D.M.Skopik, H.R.Weller, N.R.Roberson, S.A.Wender 2H(p, γ)3He Reaction Using Polarized and Unpolarized Protons NUCLEAR REACTIONS 2H(p, γ), E=3.0-14.8 MeV; measured absolute capture σ. 2H(polarized p, γ), E=5.0-8 MeV; measured σ(θ), A(θ). 3He deduced E1, E2 amplitudes, phases.
doi: 10.1103/PhysRevC.19.601
1979SK04 Phys.Rev. C20, 409 (1979) D.M.Skopik, J.J.Murphy II, H.R.Weller, R.A.Blue, N.R.Roberson, S.A.Wender, D.R.Tilley Reactions 15N(γ, d0)13C and 13C(d, γ0)15N in the Giant Resonance Region NUCLEAR REACTIONS 15N(e, e'd), E not given; measured σ(θ); deduced σ(γ, d). 13C(polarized d, γ), E=6.74 MeV; measured σ(θ), A(θ). 15N deduced E1 matrix elements, T-character, phases around 22-MeV excitation.
doi: 10.1103/PhysRevC.20.409
1979WE08 Phys.Rev. C20, 1589 (1979) H.R.Weller, S.Manglos, S.A.Wender, N.R.Roberson, M.Potokar, D.R.Tilley Inelastic α Cross Sections in the Region of the Giant Quadrupole Resonance for Nuclei Near Mass 60 NUCLEAR REACTIONS 52Cr, 54,58Fe, 60Ni(α, α'), E=8-18 MeV; measured σ(Eα, θ).
doi: 10.1103/PhysRevC.20.1589
1978MA36 J.Phys.(London) G4, 1347 (1978) Internal Conversion in 100Tc NUCLEAR REACTIONS 100Mo(p, n), E=3.7 MeV; measured γ(t), K X-ray. 100Tc level deduced T1/2, ICC, λ.
doi: 10.1088/0305-4616/4/8/016
1978WE02 Phys.Rev. C17, 1260 (1978) H.R.Weller, R.A.Blue, P.L.Von Behren, N.R.Roberson, C.R.Gould, D.R.Tilley, S.A.Wender Angular Distribution Measurements for Radiative Capture of Fast Neutrons by 40Ca NUCLEAR REACTIONS 40Ca(n, γ), E=8.0, 12.0 MeV; measured σ(θ). DSD calculations.
doi: 10.1103/PhysRevC.17.1260
1978WE03 Phys.Rev. C17, 1365 (1978) S.A.Wender, C.R.Gould, D.R.Tilley, D.G.Rickel, R.W.Zurmuhle Confirmation of 8+ Assignment to the 11.86 MeV Level in 24Mg NUCLEAR REACTIONS 12C(16O, αγ), E=42 MeV; measured linear polarization, αγ-coin. 24Mg level deduced J, π.
doi: 10.1103/PhysRevC.17.1365
1978WE11 Phys.Rev.Lett. 41, 1217 (1978) S.A.Wender, N.R.Roberson, M.Potokar, H.R.Weller, D.R.Tilley Quadrupole Radiation in Fast-Neutron Capture on 40Ca NUCLEAR REACTIONS 40Ca(n, γ), E=6-13 MeV; measured σ(E). DSD calculations.
doi: 10.1103/PhysRevLett.41.1217
1976WE06 Nucl.Phys. A259, 246 (1976) Isomeric γ-Ray Transitions in 98Tc NUCLEAR REACTIONS 98Mo(p, nγ), E=4 MeV; measured Eγ, Iγ(t), delayed X-rays. 98Tc deduced levels, T1/2, λ, ICC. Pulsed beam, enriched target.
doi: 10.1016/0375-9474(76)90065-8
1976WE23 Phys.Rev. C14, 1179 (1976) S.A.Wender, C.R.Gould, D.R.Tilley, D.G.Rickel, J.D.Turner, N.R.Roberson g Factor of the 738 keV State in 43K NUCLEAR REACTIONS 40Ar(α, p), E=15 MeV; measured γγ(θ, H, t). 43K level deduced T1/2, g.
doi: 10.1103/PhysRevC.14.1179
1975WE08 Nucl.Phys. A241, 332 (1975) Integral Rotation of 3/2- Levels in 65Zn and 67Zn NUCLEAR REACTIONS 62,64Ni(α, nγ), Eα=8.5, 7.5 MeV; measured Iγ(θ), Iγ(θ, H). 65Zn levels deduced g-factor. 65,67Zn deduced mixing ratios, transition rates.
doi: 10.1016/0375-9474(75)90322-X
1975WE16 Can.J.Phys. 53, 1401 (1975) S.A.Wender, A.Islam, R.G.Summers-Gill The Lifetime of the 72.6 keV Level in 138La NUCLEAR REACTIONS 138Ba(p, nγ), E=7 MeV; measured nγ(t). 138La level deduced T1/2, λ, J, π.
doi: 10.1139/p75-178
1975WE21 Can.J.Phys. 53, 2544 (1975) Nuclear g Factor of the g9/2 Level in 65Zn NUCLEAR REACTIONS 62Ni(α, nγ), E=14 MeV; measured γ(θ, H). 65Zn level deduced g.
doi: 10.1139/p75-309
1974KE11 Nucl.Phys. A226, 381 (1974) P.G.Kerr, S.A.Wender, J.A.Cameron Magnetic Rotation of Levels of 53Mn and 54Mn Following the 53,54Cr(p, n) and 51V(α, n) Reactions NUCLEAR REACTIONS 53,54Cr(p, nγ), E=2.5, 3.0 MeV; 51V(α, nγ), E=7.5 MeV; measured Eγ, γ(θ) in Cr, V metal, γ(θ, H) in CrFe, VFe. 53Mn level deduced g; 54Mn level deduced gtau.
doi: 10.1016/0375-9474(74)90490-4
1974WE05 Can.J.Phys. 52, 1137 (1974) Nuclear g Factor of the 339 keV Level of 59Ni NUCLEAR REACTIONS 56Fe(α, nγ), E=7.5 MeV; measured γ(θ, H, t). 59Ni deduced g.
doi: 10.1139/p74-150
1973WE20 Phys.Rev. B8, 4901 (1973) Recoil Radiation Damage in Tungsten Compounds Observed Using the Mossbauer Effect Following Coulomb Excitation NUCLEAR REACTIONS 182,183,184,186W(γ, γ); measured level-width. Mossbauer measurement.
doi: 10.1103/PhysRevB.8.4901
1972HE01 Phys.Rev. C5, 219 (1972) N.Hershkowitz, S.A.Wender, A.B.Carpenter Relative Quadrupole Moments of the First Excited States of W180 and W182 NUCLEAR MOMENTS 180,182W levels measured quadrupole moment ratio. Mossbauer expt. NUCLEAR REACTIONS 180,182W(γ, γ), E=103, 101 keV; measured Mossbauer effect. 180,182W levels deduced quadrupole moment ratio. 180W deduced transition. Coulomb excitation.
doi: 10.1103/PhysRevC.5.219
1971OB02 Phys.Rev. C3, 1585 (1971) L.W.Oberley, N.Hershkowitz, S.A.Wender, A.B.Carpenter Relative Quadrupole Moments of the First Excited States of W182, W184, And W186 NUCLEAR REACTIONS 182,184,186W(γ, γ), E=100, 111, 123 keV; measured Mossbauer effect. 182,184,186W deduced relative quadrupole moment.
doi: 10.1103/PhysRevC.3.1585
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