NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = P.Miller Found 69 matches. 1987AN10 Phys.Rev. A36, 3699 (1987) M.C.Andrews, F.D.McDaniel, J.L.Duggan, P.D.Miller, P.L.Pepmiller, H.F.Krause, T.M.Rosseel, L.A.Rayburn, R.Mehta, G.Lapicki L- and M-Shell X-ray Production Cross Sections of Nd, Gd, Ho, Yb, Au, and Pb by 25-MeV Carbon and 32-MeV Oxygen Ions ATOMIC PHYSICS Nd, Gd, Ho, Yb, Au, Pb(12C, X), E=25 MeV; measured L X-ray, M X-ray production σ.
doi: 10.1103/PhysRevA.36.3699
1987BR13 Phys.Rev. A35, 4114 (1987) R.Bruch, N.Stolterfoht, S.Datz, P.D.Miller, P.L.Pepmiller, Y.Yamazaki, H.F.Krause, J.K.Swenson, K.T.Chung, B.F.Davis High-Resolution KLL Auger Spectra of Multiply Ionized Oxygen Projectiles Studied by Zero-Degree Electron Spectroscopy ATOMIC PHYSICS He(O, X), E=10 MeV; measured K electron Auger spectra. Zero-degree spectroscopy method, multiply ionized projectiles. Theoretical calculations.
doi: 10.1103/PhysRevA.35.4114
1986HA02 Phys.Rev. A33, 914 (1986) J.Hall, P.Richard, P.L.Pepmiller, D.C.Gregory, P.D.Miller, C.D.Moak, C.M.Jones, G.D.Alton, L.B.Bridwell, C.J.Sofield Energy Systematics of Single and Double K-Shell-Vacancy Production in Titanium Bombarded by Chlorine Ions NUCLEAR REACTIONS Ti(37Cl, X), E=6.88 MeV/nucleon; measured E K(X-ray), I K(X-ray); deduced single, double K-shell vacancy production σ.
doi: 10.1103/PhysRevA.33.914
1983GO11 Phys.Rev.Lett. 51, 451 (1983) J.Gomez del Campo, D.Shapira, J.A.Biggerstaff, C.D.Moak, P.D.Miller, N.Neskovic, R.W.Fearick, J.P.F.Sellschop Measurements of Nuclear Deexcitation Times down to 10-19 sec using Crystal Blocking of 16O on Diamond NUCLEAR REACTIONS 12C(16O, X), E=120 MeV; measured evaporation residue yields vs θ; deduced evaporation residue deexcitation times. 12C(16O, 16O), E=80, 120 MeV; measured yield distributions; deduced smearing parameter. Blocking technique, thick diamond crystal. Monte-Carlo statistical model calculations.
doi: 10.1103/PhysRevLett.51.451
1983ME16 Phys.Rev. A28, 2722 (1983) R.Mehta, J.L.Duggan, F.D.McDaniel, M.C.Andrews, G.Lapicki, P.D.Miller, L.A.Rayburn, A.R.Zander Direct Ionization and Electron Capture in M-Shell X-Ray Production by Fluorine Ions ATOMIC PHYSICS Au, Pb, Bi, U(19F, X), E=25, 27, 35 MeV; measured M-shell X-ray production σ.
doi: 10.1103/PhysRevA.28.2722
1982GR27 Metrologia 18, 93 (1982) G.L.Greene, N.F.Ramsey, W.Mampe, J.M.Pendlebury, K.Smith, W.B.Dress, P.D.Miller, P.Perrin An Improved Derived Value for the Neutron Magnetic Moment in Nuclear Magnetons
doi: 10.1088/0026-1394/18/2/005
1982HE10 Phys.Lett. 119B, 298 (1982) B.Heckel, N.F.Ramsey, K.Green, G.L.Greene, R.Gahler, O.Schaerpf, M.Forte, W.Dress, P.D.Miller, R.Golub, J.Byrne, J.M.Pendlebury A Measurement of Parity Non-Conserving Neutron Spin Rotation in Lead and Tin NUCLEAR REACTIONS Pb, Sn(polarized n, n), E ≤ 0.001 eV; measured parity nonconserving spin rotation parameter; deduced possible p-wave, structure effects.
doi: 10.1016/0370-2693(82)90674-8
1981BA22 Int.J.Appl.Radiat.Isotop. 32, 389 (1981) J.K.Bair, P.D.Miller, B.W.Wieland Neutron Yields from the 4-12 MeV Proton Bombardment of 11B, 13C and 18O as Related to the Production of 11C, 13N and 18F NUCLEAR REACTIONS 13C, 11B(p, n), E=4-12 MeV; C(p, n), E=4-5 MeV; O(p, n), E=4-10 MeV; measured thick target yields, σ(E); deduced production σ for 11C, 13N, 18F. Graphite sphere detector, silicon dioxide target.
doi: 10.1016/S0020-708X(81)81005-8
1980CE01 Phys.Rev. C21, 2471 (1980) R.A.Cecil, B.D.Anderson, A.R.Baldwin, R.Madey, A.Galonsky, P.Miller, L.Young, F.M.Waterman Neutron Angular and Energy Distributions from 710-MeV Alphas Stopping In Water, Carbon, Steel, and Lead, and 640-MeV Alphas Stopping in Lead NUCLEAR REACTIONS 2H, O, C, Fe(α, xn), E=710 MeV; Pb(α, xn), E=640, 710 MeV; measured σ(θn, En), stopped α; deduced total integrated neutron yield. Intranuclear cascade model.
doi: 10.1103/PhysRevC.21.2471
1979GR25 Phys.Rev. D20, 2139 (1979) G.L.Greene, N.F.Ramsey, W.Mampe, J.M.Pendlebury, K.Smith, W.B.Dress, P.D.Miller, P.Perrin Measurement of the Neutron Magnetic Moment NUCLEAR MOMENTS 1n; measured μ; deduced μn/μp.
doi: 10.1103/PhysRevD.20.2139
1977BH02 Z.Phys. A280, 267 (1977) R.Bhowmik, R.R.Doering, A.Galonsky, P.S.Miller Proton Decay of the Isobaric Analogs of the Ground States of 207Pb and 208Pb NUCLEAR REACTIONS 207,208Pb(p, np), E=25 MeV; measured np-coin. 207,208Pb deduced proton decay of IAS, resolved width anomalies.
doi: 10.1007/BF01434352
1977GR19 Phys.Lett. 71B, 297 (1977) G.L.Greene, N.F.Ramsey, W.Mampe, J.M.Pendlebury, K.Smith, W.D.Dress, P.D.Miller, P.Perrin A New Measurement of the Magnetic Moment of the Neutron NUCLEAR MOMENTS 1n; measured μ.
doi: 10.1016/0370-2693(77)90220-9
1976BA67 Aust.J.Phys. 29, 245 (1976) F.C.Barker, G.M.Crawley, P.S.Miller, W.F.Steele The Ghost Anomaly in the 9Be(p, d)8Be Reaction NUCLEAR REACTIONS 9Be(p, d), E=39.91 MeV; measured σ(θ); deduced anomaly.
doi: 10.1071/PH760245
1976GU05 Phys.Rev. C13, 691 (1976) D.E.Gustafson, S.T.Thornton, T.C.Schweizer, J.L.C.Ford, Jr., P.D.Miller, R.L.Robinson, P.H.Stelson High-Spin States of the Kπ = 3/2+ and 1/2+ Bands of 23Na NUCLEAR REACTIONS 12C(15N, α), E=36-39.2 MeV; measured σ(E, Eα, θ). 23Na deduced levels, J, π, K. Hauser-Feshbach calculations.
doi: 10.1103/PhysRevC.13.691
1976GU10 Nucl.Phys. A262, 96 (1976) D.E.Gustafson, J.Gomez del Campo, R.L.Robinson, P.H.Stelson, P.D.Miller, J.K.Bair High-Spin States of 26Mg Populated in the 12C(18O, α) Reaction NUCLEAR REACTIONS 12C(18O, α), E=43.2-45.9 MeV; measured σ(E) at θlab=7°. 26Mg deduced levels, K, J, π. Hauser-Feshbach calculations, suggested J, π values.
doi: 10.1016/0375-9474(76)90442-5
1975DR03 Phys.Rev.Lett. 34, 752 (1975) W.B.Dress, C.Guet, P.Perrin, P.D.Miller Observation of Two-Photon Decay in n-p Capture NUCLEAR REACTIONS 1H(n, γ), E=subthermal; measured γγ-coin, σ(Eγ). 2H deduced γ-branching ratios.
doi: 10.1103/PhysRevLett.34.752
1975GA18 Phys.Rev. C12, 1072 (1975) A.Galonsky, G.M.Crawley, P.S.Miller, R.R.Doering, D.M.Patterson Discrepancies between Formation and Decay of Isobaric Analog States of Pb and Bi NUCLEAR REACTIONS 208Pb(p, n), (p, np), E=21-35 MeV; measured σ; deduced σ discrepancy.
doi: 10.1103/PhysRevC.12.1072
1975GO25 Phys.Rev. C12, 1247 (1975) J.Gomez del Campo, D.E.Gustafson, R.L.Robinson, P.H.Stelson, P.D.Miller, J.K.Bair, J.B.McGrory Population of High-Spin States in 23Na Through the 11B(16O, α) Reaction NUCLEAR REACTIONS 11B(16O, α), E=41.6-45.4 MeV; measured σ(E, Eα, θ). 23Na deduced levels, J, π.
doi: 10.1103/PhysRevC.12.1247
1973CO19 Phys.Lett. 45B, 321 (1973) W.R.Coker, J.Lin, J.L.Duggan, P.D.Miller Multistep Contributions to 11B(h, α)10B from 8.0 to 12.0 MeV NUCLEAR REACTIONS 11B(3He, α), E=8.0, 10.0, 12.0 MeV; measured σ(θ). 10B level deduced S.
doi: 10.1016/0370-2693(73)90044-0
1973CR02 Phys.Rev. C8, 574 (1973) G.M.Crawley, P.S.Miller, G.J.Igo, J.Kulleck High-Resolution Study of 48Ca(p, t)46Ca at E = 39 MeV NUCLEAR REACTIONS 48Ca(p, t), E=39 MeV; measured σ(Et, θ). 46Ca deduced levels, J, π.
doi: 10.1103/PhysRevC.8.574
1973DR12 Phys.Rev. D7, 3147 (1973) W.B.Dress, P.D.Miller, N.F.Ramsey Improved Upper Limit for the Electric Dipole Moment of the Neutron NUCLEAR MOMENTS 1n; measured upper limit for electric dipole moment.
doi: 10.1103/PhysRevD.7.3147
1973WU01 Nucl.Phys. A199, 23 (1973) R.R.Wu, R.L.Dangle, M.M.Duncan, J.L.Duggan, P.D.Miller, Jung Lin A Study of the 11B(3He, p)13C Reaction at 12, 10, 8, 6 and 4 MeV NUCLEAR REACTIONS 11B(3He, p), E=4, 6, 8, 10, 12 MeV; measured σ(θ). Enriched target.
doi: 10.1016/0375-9474(73)90331-X
1972CR04 Phys.Rev. C6, 306 (1972) Proton Decay of the Isobaric Analogs of the Ground States of 206Pb, 207Pb, 208Pb, and 209Bi NUCLEAR REACTIONS 206,207,208Pb(p, np), E=21.3-35 MeV; measured σ(E;Ep, θ). 206,207Bi, 208Bi, 209Po deduced isobaric analog states, level-width, Coulomb energy differences.
doi: 10.1103/PhysRevC.6.306
1972CR07 Phys.Rev. C6, 1890 (1972) G.M.Crawley, P.S.Miller, A.Galonsky, T.Amos, R.Doering Widths of Analog States in Bi and Po from (p, n) Spectra NUCLEAR REACTIONS 206,207,208Pb, 209Bi(p, n), E=25 MeV; measured σ(En). 209Po-209Bi, 208Bi-208Pb, 207Bi- 207Pb, 206Bi- 206Pb deduced Coulomb energy differences, isobaric analog states, level-width.
doi: 10.1103/PhysRevC.6.1890
1971CO14 Nucl.Phys. A168, 307 (1971) W.R.Coker, P.D.Miller, J.L.Duggan, M.M.Duncan, R.L.Dangle, J.Lin The 14C(t, α0)13C Reaction at 6.0, 8.0 and 10.0 MeV NUCLEAR REACTIONS 14C(3He, α), 14C(3He, 3He), E=6.0, 8.0, 10.0 MeV; 13C(α, α), E=15, 18, 20 MeV; measured σ(θ); deduced optical model parameters. Enriched targets.
doi: 10.1016/0375-9474(71)90795-0
1971MI03 Nucl.Phys. A163, 65 (1971) Charge Exchange in Medium Mass Nuclei as Observed by the (p, np) Reaction NUCLEAR REACTIONS 67Zn, 77Se, 91Zr, 95,97Mo, 105Pd, 110,111,113Cd, 115,116,117,119Sn, 123,125Te(p, np), E=12.8-18 MeV; measured σ(E;Ep'θ(p)). 67Ga, 77Br, 91Nb, 95,97Tc, 105Ag, 110,111,113In, 115,116,117,119Sb, 123,125I deduced isobaric analog states, p-width/level-width.
doi: 10.1016/0375-9474(71)90522-7
1971SE07 Priv.Comm. (1971)
1970CR05 Phys.Rev. C2, 1071 (1970) G.M.Crawley, W.Benenson, P.S.Miller, D.L.Bayer, R.St.Onge, A.Kromminga Properties of the 209Bi Ground-State Analog in 209Po NUCLEAR REACTIONS 209Bi(p, n), (p, d), (p, np), E=24-30 MeV; measured σ(E;θ), σ(E;Ed, θ), σ(E;En, θ). 209Po deduced level, level-width, isobaric analog. 209Po-209Bi deduced Coulomb energy difference.
doi: 10.1103/PhysRevC.2.1071
1970DU07 Nucl.Phys. A151, 107 (1970) J.L.Duggan, J.Y.Park, S.D.Danielopoulos, P.D.Miller, J.Lin, M.M.Duncan, R.L.Dangle 3He Elastic Scattering from 10B and 14C in the Range 4 to 18 MeV NUCLEAR REACTIONS 10B(3He, 3He)10B, 14C(3He, 3He)14C, E = 4-18 MeV; measured σ(E;θ); deduced optical potential parameters.
doi: 10.1016/0375-9474(70)90971-1
1969MI15 Nucl.Phys. A136, 229 (1969) P.D.Miller, J.L.Duggan, M.M.Duncan, R.L.Dangle, W.R.Coker, J.Lin 11B(3He, d)12C Spectroscopic Factors NUCLEAR REACTIONS 11B(3He, d), (3He, 3He); E = 10, 12, 18 MeV; measured σ(Ed, θ). 12C levels deduced S. Enriched target.
doi: 10.1016/0375-9474(69)90050-5
1969PA11 Nucl.Phys. A134, 277 (1969) J.Y.Park, J.L.Duggan, P.D.Miller, M.M.Duncan, R.L.Dangle Elastic Scattering of 3He Particles by 9Be and 11B Between 4.0 and 18.0 MeV NUCLEAR REACTIONS 9Be, 11B(3He, 3He), E=4-18 MeV; measured σ(θ); deduced optical-model parameters. Enriched 11B target.
doi: 10.1016/0375-9474(69)91052-5
1967BI07 Phys.Letters 25B, 273 (1967) J.A.Biggerstaff, C.Bingham, P.D.Miller, J.Solomon, K.K.Seth Proton Particle-Hole States in 116Sn NUCLEAR STRUCTURE 116Sn; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90011-1
1967CO03 Nucl.Phys. A91, 97 (1967) W.R.Coker, M.M.Duncan, J.L.Duggan, P.D.Miller An Investigation of the 9Be(3He, p)11B Reaction at Low Energies NUCLEAR REACTIONS 9Be(3He, p), E = 1-3 MeV; measured σ(Ep, θ). 11B deduced levels J, π, L.
doi: 10.1016/0375-9474(67)90453-8
1967SE10 Phys.Rev. 164, 1450 (1967) K.K.Seth, J.A.Biggerstaff, P.D.Miller, G.R.Satchler Study of Proton Particle-Hole States in 40Ca by the 39K(3He, D)40Ca Reaction NUCLEAR STRUCTURE 40Ca; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.164.1450
1966SE08 Phys.Rev.Letters 17, 1294 (1966) K.K.Seth, R.G.Couch, J.A.Biggerstaff, P.D.Miller Reaction 39K(3He, P)41Ca and Two-Particle, One-Hole States NUCLEAR STRUCTURE 41Ca; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.17.1294
1965SE01 Bull.Am.Phys.Soc. 10, No.1, 10, AC8 (1965) K.K.Seth, G.Walter, P.D.Miller, J.A.Biggerstaff 15N(3He, p) Reaction and Intermediate States NUCLEAR STRUCTURE 15N; measured not abstracted; deduced nuclear properties.
1965WA28 Phys.Rev. 139, B29 (1965) R.Wagner, P.D.Miller, T.Tamura, H.Marshak Interaction of 350-keV Polarized Neutrons with Oriented Ho165 Nuclei NUCLEAR REACTIONS 165Ho(n, n), 165Ho(n, x), E=301-405 keV; measured products, 165Ho; deduced σ, σ(E), σ(θ). Data were imported from EXFOR entry 12133.
doi: 10.1103/PhysRev.139.B29
1964MI01 Bull.Am.Phys.Soc. 9, No.1, 45, DC12 (1964) P.D.Miller, J.L.Duggan, M.M.Duncan Absence of States in Be8 at 7.56, 13.91, and 18.00 MeV NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.
1964MI10 Nucl.Phys. 54, 155(1964) P.D.Miller, J.L.Duggan, M.M.Duncan Absence of States in Be8 at 7.56, 13.91 and 18.00 MeV NUCLEAR REACTIONS 7Li(p, α), (p, γ), Ep=0.50-2.0 MeV; measured α-, γ-spectra. 8Be deduced levels. Enriched target.
doi: 10.1016/0029-5582(64)90401-8
1964WA18 Phys.Letters 10, 316 (1964) R.Wagner, P.D.Miller, T.Tamura, H.Marshak The Interaction of 350 keV Polarized Neutrons with Oriented Ho165 Nuclei NUCLEAR STRUCTURE 165Ho; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(64)90522-0
1963CO24 Bull.Am.Phys.Soc. Southeastern Section, p. 18, S8, (November 1963); Bull.Am.Phys.Soc. 9, No.3, 351, S8 (1964) W.R.Coker, M.M.Duncan, J.L.Duggan, V.H.Webb, P.D.Miller The Be9(He3, p)B11 Reaction NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.
1963DU12 Nucl.Phys. 46, 336 (1963) J.L.Duggan, P.D.Miller, R.F.Gabbard A Study of the Reactions Be9(He3, n)C11, Li7(He3, n)B9 and C13(He3, n)O15 NUCLEAR STRUCTURE 13C, 9Be, 7Li; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90604-7
1963MI02 Bull.Am.Phys.Soc. 8, No.4, 292, A16 (1963) P.D.Miller, G.C.Morrison, N.Gale, G.Dearnaley α Particles from the Bombardment of B10 and B11 by Li6 and Li7 NUCLEAR STRUCTURE 11B, 10B, 6Li; measured not abstracted; deduced nuclear properties.
1963WA22 WASH-1044, p.62 (1963) R.K.H.Wagner, P.D.Miller, H.Marshak, C.W.Williams Scattering of Polarized Neutrons from Polarized Ho165 NUCLEAR STRUCTURE 165Ho; measured not abstracted; deduced nuclear properties.
1962DU03 ORNL-3268, p.12 (1962) J.L.Duggan, P.D.Miller, R.F.Gabbard A Study of the Reactions Be9(He3, n)C11, Li7(He3, n)B9, and C13(He3, n)O15 NUCLEAR STRUCTURE 13C, 7Li, 9Be; measured not abstracted; deduced nuclear properties.
1962FE07 Conf.Low Energy Nuclear Phys.Harwell, AERE-R-4131, 13, 5.4 (September 1962) A.T.G.Ferguson, N.Gale, P.D.Miller, G.C.Morrison, R.E.White NUCLEAR STRUCTURE 19F; measured not abstracted; deduced nuclear properties.
1962GA08 R.E.White - Conf.Low Energy Nuclear Phys.Harwell, AERE-R-4131, 14, 5.7 (September 1962) N.Gale, A.T.G.Ferguson, P.D.Miller, G.C.Morrison NUCLEAR STRUCTURE 24Mg; measured not abstracted; deduced nuclear properties.
1962MO13 Conf.Low Energy Nuclear Phys.Harwell, AERE-R-4131, 14, 5.6 (September 1962) G.C.Morrison, A.T.G.Ferguson, N.Gale, P.D.Miller, H.Naylor, R.E.White NUCLEAR STRUCTURE 15N; measured not abstracted; deduced nuclear properties.
1961GA08 Bull.Am.Phys.Soc. 6, No.5, 416, B6 (1961) R.F.Gabbard, P.D.Miller, J.L.Duggan C13(He3, n)O15 Reaction
1961GI07 Phys.Rev. 122, 182 (1961) J.H.Gibbons, R.L.Macklin, P.D.Miller, J.H.Neiler Average Radiative Capture Cross Sections for 7- to 170-keV Neutrons S.S.Glickstein - TID-14628 (1961) A Study of F20
doi: 10.1103/PhysRev.122.182
1961MI01 Bull.Am.Phys.Soc. 6, No.1, 60, TA2 (1961) P.D.Miller, J.L.Duggan, R.F.Gabbard Angular Yield of Neutrons from the T(p, n)He3 Reaction NUCLEAR STRUCTURE 9B, 11C, 15O; measured not abstracted; deduced nuclear properties.
1960GI02 ORNL-2910, p.33 (1960) J.H.Gibbons, W.M.Good, P.D.Miller, J.H.Neiler Neutron Total Cross Sections in the kev Energy Range
1960GO07 Bull.Am.Phys.Soc.5, No.6, 449, K2 (1960) W.M.Good, J.H.Gibbons, P.D.Miller, J.H.Neiler Total Cross Sections of Ge70,72,74,76, Cu63, Co59 Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11734. 1960JO03 Phys.Rev. 117, 525 (1960) C.M.Jones, G.C.Phillips, P.D.Miller Alpha-Alpha Scattering in the Energy Range 5 to 9 MeV NUCLEAR STRUCTURE 8Be, 4He; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.117.525
1960MI01 Bull.Am.Phys.Soc. 5, No.1, 18, E3 (1960) P.D.Miller, J.H.Gibbons, R.L.Macklin Effect of p-Wave Neutrons on Total Cross Sections in the keV Region
1959GI19 Bull.Am.Phys.Soc. 4, No.7, 414, J8 (1959) J.H.Gibbons, P.D.Miller, R.L.Macklin, J.H.Neeler Absorption Cross Section of U235 from 10 to 175 keV
1959JO19 Bull.Am.Phys.Soc. 4, No.2, 104, P8 (1959) C.M.Jones, P.D.Miller, G.C.Phillips Alpha-Alpha Scattering in the Range 4.5 to 9 MeV
1959MA37 Bull.Am.Phys.Soc. 4, No.1, 43, R10 (1959) R.L.Macklin, J.H.Neiler, J.H.Gibbons, P.D.Miller Gamma Detection of Kilovolt Neutron Capture II NUCLEAR REACTIONS 159Tb, 165Ho(n, γ), E=29-63 keV; measured reaction products, Eγ, Iγ; deduced σ.
1959MI21 ORNL-2610, p.19 (1959) P.D.Miller, W.M.Good, J.H.Gibbons, R.L.Macklin, J.H.Neiler Pulsed Van de Graaff and Fast Time-of-Flight Studies
1959MI85 Bull.Am.Phys.Soc. 4, No.1, 42, R1 (1959) P.D.Miller, W.M.Good, J.H.Gibbons, J.H.Neiler Total Cross Sections in the Kilovolt Region by Time-of-Flight Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11007. 1959MI86 Bull.Am.Phys.Soc. 4, No.2, 104, P9 (1959) Spin Polarization Determination by Elastic Scattering of Protons and He3
1959MI94 ORNL-2718, p.22 (1959) P.D.Miller, J.H.Gibbons, J.H.Neiler Total Cross Sections in the Kilovolt Range Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11007. 1959NE20 Bull.Am.Phys.Soc. 4, No.1, 43, R9 (1959) J.H.Neiler, R.L.Macklin, J.H.Gibbons, P.D.Miller Gamma Detection of Kilovolt Neutron Capture. I.
1959PH37 Phys.Rev. 115, 1268 (1959) Measurement of Spin Polarization by Nuclear Scattering
doi: 10.1103/PhysRev.115.1268
1959PH39 Compt.Rend.Congr.Intern.Phys.Nucl., Paris (1958), P.Gugenberger, Ed., Dunod, Paris, p.522 (1959) Measurement of Spin Polarization by Nuclear Scattering
1958KA32 Phys.Rev. 112, 547 (1958) E.Kashy, P.D.Miller, J.R.Risser Energy Levels in F18 from the N14(α, n)N14 and N14(α, p)O17 Reactions
doi: 10.1103/PhysRev.112.547
1958MI92 Phys.Rev. 112, 2048 (1958) Scattering of He3 from He4 and States in Be7
doi: 10.1103/PhysRev.112.2048
1958MI93 Phys.Rev. 112, 2043 (1958) Scattering of Protons from Helium and Level Parameters in Li5
doi: 10.1103/PhysRev.112.2043
1958RI35 Bull.Am.Phys.Soc. 3, No.1, 27, J10 (1958); Priv.Comm. (July 1958) J.R.Risser, P.D.Miller, E.Kashy Alpha-Particle Bombardment of N14
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