Nuclear Science References (NSR)

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NSR database version of April 11, 2024.

Search: Author = J.L.Weil

Found 67 matches.

2016MA04 Phys.Rev. C 93, 014301 (2016)

R.Massarczyk, G.Schramm, T.Belgya, R.Schwengner, R.Beyer, D.Bemmerer, Z.Elekes, E.Grosse, R.Hannaske, A.R.Junghans, Z.Kis, T.Kogler, C.Lorenz, K.Schmidt, L.Szentmiklosi, A.Wagner, J.L.Weil

Role of electric and magnetic dipole strength functions in the ¹¹⁴Cd (γ, γ') and ¹¹³Cd (n, γ) reactions

NUCLEAR REACTIONS ¹¹⁴Cd(γ, γ'), E<10 MeV; measured Eγ, Iγ, γ(θ), photoabsorption σ(E) at bremsstrahlung facility γELBE at Dresden. ¹¹³Cd(n, γ), E=cold neutrons; measured Eγ, Iγ at Budapest reactor facility; deduced electric and magnetic dipole γ-strength function below S(n). Triple Lorentzian model (TLO). Comparison with statistical model calculations using γDEX code using RIPL3 M1 and triple Gaussian models.

doi: 10.1103/PhysRevC.93.014301
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2013MA32 Phys.Rev. C 87, 044306 (2013)

R.Massarczyk, G.Schramm, A.R.Junghans, R.Schwengner, M.Anders, T.Belgya, R.Beyer, E.Birgersson, A.Ferrari, E.Grosse, R.Hannaske, Z.Kis, T.Kogler, K.Kosev, M.Marta, L.Szentmiklosi, A.Wagner, J.L.Weil

Electromagnetic dipole strength up to the neutron separation energy from ¹⁹⁶Pt(γγ')and ¹⁹⁵Pt(n, γ) reactions

NUCLEAR REACTIONS ¹⁹⁵Pt(n, γ), E(mean)=12 meV; measured Eγ, Iγ at the research reactor in Budapest. ¹⁹⁶Pt(γ, γ'), E=0-7.9 MeV; measured Eγ, Iγ, bremsstrahlung photon fluences, photoabsorption σ(E) at the ELBE accelerator in Dresden; deduced E1 and M1 strength distributions, simulated ground-state branching ratios for 1- states. Analysis by statistical code γDEX.

doi: 10.1103/PhysRevC.87.044306
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2012SC02 Phys.Rev. C 85, 014311 (2012)

G.Schramm, R.Massarczyk, A.R.Junghans, T.Belgya, R.Beyer, E.Birgersson, E.Grosse, M.Kempe, Z.Kis, K.Kosev, M.Krticka, A.Matic, K.D.Schilling, R.Schwengner, L.Szentmiklosi, A.Wagner, J.L.Weil

Dipole strength in ⁷⁸Se below the neutron separation energy from a combined analysis of ⁷⁷Se(n, γ) and ⁷⁸Se(γ, γ') experiments

NUCLEAR REACTIONS ⁷⁷Se(n, γ), E AP 6 milli-eV, cold neutrons; ⁷⁸Se(γ, γ'), E<11.5 MeV bremsstrahlung; measured Eγ, Iγ; deduced photoabsorption cross section, level density according to constant-temperature model, dipole strength function. Comparison with simulated spectra from extreme statistical code.

doi: 10.1103/PhysRevC.85.014311
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2006AS02 Phys.Rev. C 73, 055801 (2006)

M.Assuncao, M.Fey, A.Lefebvre-Schuhl, J.Kiener, V.Tatischeff, J.W.Hammer, C.Beck, C.Boukari-Pelissie, A.Coc, J.J.Correia, S.Courtin, F.Fleurot, E.Galanopoulos, C.Grama, F.Haas, F.Hammache, F.Hannachi, S.Harissopulos, A.Korichi, R.Kunz, D.LeDu, A.Lopez-Martens, D.Malcherek, R.Meunier, Th.Paradellis, M.Rousseau, N.Rowley, G.Staudt, S.Szilner, J.P.Thibaud, J.L.Weil

E1 and E2 S factors of ¹²C(α, γ₀)¹⁶0 from γ-ray angular distributions with a 4π-detector array

NUCLEAR REACTIONS ¹²C(α, γ), E(cm)=1.30-2.78 MeV; measured Eγ, Iγ(θ); deduced E1 and E2 astrophysical S-factors.

doi: 10.1103/PhysRevC.73.055801
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2005BA02 Nucl.Phys. A747, 206 (2005)

D.Bandyopadhyay, N.Warr, C.Fransen, N.Boukharouba, V.Werner, S.W.Yates, J.L.Weil, M.T.McEllistrem

Three-phonon excitations in ¹²⁴Sn

NUCLEAR REACTIONS ¹²⁴Sn(n, n'γ), E=2.2-4.5 MeV; measured Eγ, Iγ, γγ-coin, excitation functions, angular distributions, DSA. ¹²⁴Sn deduced levels, J, π, T_1/2, two- and three-phonon excitations.

doi: 10.1016/j.nuclphysa.2004.10.003
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2005HA16 Nucl.Phys. A752, 514c (2005)

J.W.Hammer, M.Fey, R.Kunz, J.Kiener, V.Tatischeff, F.Haas, J.L.Weil, M.Assuncao, C.Beck, C.Boukari-Pelissie, A.Coc, J.J.Correia, S.Courtin, F.Fleurot, E.Galanopoulos, C.Grama, F.Hammache, S.Harissopulos, A.Korichi, E.Krmpotic, D.Le Du, A.Lopez-Martens, D.Malcherek, R.Meunier, P.Papka, T.Paradellis, M.Rousseau, N.Rowley, G.Staudt, S.Szilner

New determination of the ¹²C(α, γ)¹⁶O reaction rate from γ-ray angular distribution measurements

NUCLEAR REACTIONS ¹²C(α, γ), E(cm)=0.89-2.8 MeV; measured σ(θ), S-factors; deduced astrophysical reaction rate.

doi: 10.1016/j.nuclphysa.2005.02.056
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2005HA48 Nucl.Phys. A758, 363c (2005)

E1 and E2 capture cross section and astrophysical reaction rate of the key reaction ¹²C(α, γ)¹⁶O

NUCLEAR REACTIONS ¹²C(α, γ), E(cm)=0.89-2.8 MeV; measured Eγ, Iγ, angular distributions; deduced S-factors for E1 and E2 capture. Eurogam and Gandi arrays, astrophysical implications discussed.

doi: 10.1016/j.nuclphysa.2005.05.066
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2001CH03 Phys.Rev. C63, 014606 (2001)

G.Chen, M.Li, J.L.Weil, M.T.McEllistrem

Neutron Scattering in ^{140, 142}Ce and Strengths of Neutrons and Protons in Collective Levels of ¹⁴⁰Ce

NUCLEAR REACTIONS ^140,142Ce(n, n), (n, n'), E=7.5 MeV; measured σ(θ). ^140,142Ce deduced level configurations. Comparisons with model predictions.

doi: 10.1103/PhysRevC.63.014606
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2001GA55 Phys.Rev. C64, 047303 (2001)

Z.Gacsi, M.Csatlos, A.Krasznahorkay, D.Sohler, J.Gulyas, J.Timar, M.Hunyadi, J.L.Weil, J.van Klinken

Low-Lying, Excited K = 0 Bands in ²³⁸U

NUCLEAR REACTIONS ^234,236,238U(α, α'), E=19 MeV; measured Eγ, Iγ, E(ce), I(ce) following Coulomb excitation. ²³⁸U deduced transitions ICC, enhancement of E0 strength, K=0 bands moments of inertia.

doi: 10.1103/PhysRevC.64.047303
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2001MA74 Int.J.Mod.Phys. E10, 209 (2001)

A.Marinov, S.Gelberg, D.Kolb, J.L.Weil

Strongly Enhanced Low Energy α-Particle Decay in Heavy Actinide Nuclei and Long-Lived Superdeformed and Hyperdeformed Isomeric States

NUCLEAR REACTIONS W(p, X), E=24 GeV; measured delayed Eα; deduced possible isomeric origin. ²³⁶Am, ^236,238Bk, ²⁴⁷Es, ²⁵²No deduced yields from secondary fusion reactions.

RADIOACTIVITY ^238mAm, ^247mEs, ^252mNo(α); measured isomer decay Eα, T_1/2; deduced possible transitions between hyperdeformed and superdeformed states.

doi: 10.1142/S0218301301000472
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1993IG01 Phys.Rev. C47, 1504 (1993)

A.V.Ignatyuk, J.L.Weil, S.Raman, S.Kahane

Density of Discrete Levels in ¹¹⁶Sn

NUCLEAR STRUCTURE ¹¹⁶Sn; analyzed level data; deduced best model fit to discrete level density. Back-shifted Fermi gas, constant temperature, generalized superfluid model.

doi: 10.1103/PhysRevC.47.1504
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1991BE26 Appl.Radiat.Isot. 42, 683 (1991)

R.K.Bera, J.L.Weil, S.W.Yates, M.Jay

Production of [¹¹C] Carbon Dioxide via the ¹¹B(p, n)¹¹C Reaction and [¹⁸F] Fluoride via the ¹⁸O(p, n)¹⁸F Reaction for Radiopharmaceutical Development

doi: 10.1016/0883-2889(91)90040-8
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1991RA01 Phys.Rev. C43, 521 (1991)

S.Raman, T.A.Walkiewicz, S.Kahane, E.T.Jurney, J.Sa, Z.Gacsi, J.L.Weil, K.Allaart, G.Bonsignori, J.F.Shriner, Jr.

Nearly Complete Level Scheme of ¹¹⁶Sn Below 4.3 MeV

NUCLEAR REACTIONS ¹¹⁵Sn(n, γ), E=thermal; ¹¹⁶Sn(n, n'γ), E ≤ 4.5 MeV; measured Eγ, Iγ, γ(θ) vs E. ¹¹⁶Sn deduced levels, J, π, neutron separation energy.

doi: 10.1103/PhysRevC.43.521
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1989HI11 Phys.Rev. C40, 2509 (1989)

S.E.Hicks, Z.Cao, M.C.Mirzaa, J.L.Weil, J.M.Hanly, J.Sa, M.T.McEllistrem

Nuclear Dynamics of ¹⁹²Os as Probed in Neutron Scattering

NUCLEAR REACTIONS ¹⁹²Os(n, n), (n, n'), E=0.25-4.2 MeV; measured σ(θ), σ(E); deduced model parameters. ¹⁹²Os deduced deformation features. Coupled-channels analysis.

doi: 10.1103/PhysRevC.40.2509
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1989KO29 Phys.Rev. C40, R1093 (1989)

M.A.Kovash, B.Anderson-Pugh, M.T.McEllistrem, J.K.Ternes, J.H.Trice, J.L.Weil, S.L.Blatt, H.J.Hausman, D.G.Marchlenski, A.D.Bacher

Quadrupole and Octupole Radiation from ¹⁶O Near 39 MeV Excitation

NUCLEAR REACTIONS ¹⁵N(polarized p, γ), E=24.4, 28.8 MeV; measured Eγ, Iγ, σ(θ), analyzing power vs θ; deduced σ(E2)/σ(E1), σ(E3)/σ(E1). ¹⁶O deduced isovector quadrupole, octupole resonance components.

doi: 10.1103/PhysRevC.40.R1093
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1985LE10 Phys.Rev. C32, 277 (1985)

R.S.Lee, J.H.Hamilton, A.V.Ramayya, A.P.de Lima, D.L.Sastry, K.S.R.Sastry, E.H.Spejewski, R.L.Mlekodaj, H.K.Carter, W.-D.Schmidt-Ott, J.Lin, C.R.Bingham, L.L.Riedinger, E.F.Zganjar, J.L.Weil, B.D.Kern, A.C.Xenoulis, R.W.Fink, Sun Xi-jun, Guo Jun-sheng, Cho Chi-cheng, Pan Zong-you, Guo Ying-xian

Decay of ¹¹⁷Xe → ¹¹⁷I → ¹¹⁷Te

NUCLEAR REACTIONS ^107,109Ag(¹²C, xn), E=50-70 MeV; measured γ yields. ¹¹⁷I deduced transition.

RADIOACTIVITY ¹¹⁷Xe(EC), (β⁺) [from ¹⁰⁴Pd(¹⁶O, xn), E=86 MeV]; ¹¹⁷I(EC), (β⁺) [from ¹¹⁷Xe β-decay]; ¹¹⁷Te(β⁺), (EC) [from ¹¹⁷I β-decay]; measured Eγ, Iγ, E X-ray, I X-ray, T_1/2, γγ-coin. ¹¹⁷I, ¹¹⁷Te deduced levels, relative Iγ. ¹¹⁷Sb(EC), (β⁺) [from ¹¹⁷Te decay]; measured T_1/2. ¹¹⁷Xe, ¹¹⁷I deduced mass difference, Q(EC).

doi: 10.1103/PhysRevC.32.277
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1985MI20 Phys.Rev. C32, 1488 (1985)

M.C.Mirzaa, J.P.Delaroche, J.L.Weil, J.Hanly, M.T.McEllistrem, S.W.Yates

Collective Excitations of ¹⁹⁴Pt in Low Energy Neutron Scattering

NUCLEAR REACTIONS ¹⁹⁴Pt(n, n), (n, n'), E=2.5 MeV; measured σ(θ); deduced potential parameters. Pt(n, n), E=1-20 MeV; analyzed σ(E). ¹⁹⁴Pt deduced shape characteristics. Coupled-channels calculation.

doi: 10.1103/PhysRevC.32.1488
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1984BE05 Phys.Rev. C29, 709 (1984)

R.E.Benenson, M.T.McEllistrem, J.L.Weil, W.R.Coker, T.Tamura

Interference between Reaction Mechanisms in ³²S(³He, n)³⁴Ar

NUCLEAR REACTIONS ³²S(³He, n), E=4.6-6.5 MeV; measured σ(θ) vs E; deduced optical model parameters. ³⁵Ar deduced resonances, J, π, Γ, partial widths. Direct, compound reaction interference effects, DWBA. Tof.

doi: 10.1103/PhysRevC.29.709
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1984HA44 Phys.Rev. C30, 1454 (1984)

R.W.Harper, J.L.Weil, J.D.Brandenberger

Interaction of Neutrons with Even-A Tin Isotopes: Neutron-excess dependence in scattering at E(n) = 1.00 and 1.63 MeV

NUCLEAR REACTIONS ^{116,118,120,122,124}Sn(n, n), (n, n'), E=1, 1.63 MeV; measured σ(θ); deduced optical model parameters, neutron excess parameter dependence. Isotopically enriched samples, neutron tof. Compound-elastic scattering, level width fluctuation corrections.

doi: 10.1103/PhysRevC.30.1454
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1984KE09 ATOMKI Kozlem. 26, 26 (1984)

B.D.Kern, M.T.McEllistrem, J.L.Weil, S.W.Yates

Nuclear Structure Studies through the Combined Use of the (n, n') and (n, n'γ) Reactions

NUCLEAR REACTIONS ^94,100Mo, ¹²⁴Sn, ¹⁶⁸Er, ¹⁹⁸Pt(n, n'), (n, n'γ), E=0.5-4 MeV; measured σ(E), σ(E, Eγ), σ(θn), γ(θ). ^94,100Mo, ¹⁹⁸Pt levels deduced J.

1983YA04 Nucl.Phys. A406, 519 (1983)

S.W.Yates, A.Khan, A.J.Filo, M.C.Mirzaa, J.L.Weil, M.T.McEllistrem

Low-Lying Levels, γ-Ray Transitions, and Vibrational Structure in ¹⁹⁸Pt from (n, n'γ) Reaction Spectroscopy

NUCLEAR REACTIONS ¹⁹⁸Pt(n, n'γ), E=0.8-2.5 MeV; measured Eγ, Iγ, σ(E, Eγ, θγ). ¹⁹⁸Pt deduced levels, J, π, branching ratios. Enriched target, Ge(Li) detector, time-of-flight background suppression. Theoretical comparison.

doi: 10.1016/0375-9474(83)90374-3
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1982HA47 Phys.Rev. C26, 1432 (1982)

R.W.Harper, T.W.Godfrey, J.L.Weil

Interaction of Neutrons with Even-A Tin Isotopes. I. Total Cross Section for E(n) = 0.3-5.0 MeV

NUCLEAR REACTIONS ^{116,118,120,122,124}Sn(n, X), E=0.3-5 MeV; measured transmission; deduced σ(total) vs E. Tof, enriched targets. Optical model.

doi: 10.1103/PhysRevC.26.1432
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1981FI01 Phys.Rev. C23, 1938 (1981)

A.J.Filo, S.W.Yates, D.F.Coope, J.L.Weil, M.T.McEllistrem

Positive-and Negative-Parity Level Structures of ¹⁹⁴Pt from (n, n'γ) Reaction Spectroscopy

NUCLEAR REACTIONS ¹⁹⁴Pt(n, n'), E=1.2-4.5 MeV; measured Eγ, Iγ, σ(E, Eγ), γ(θ). ¹⁹⁴Pt deduced levels, γ-branching ratios, J, π, B(E2). Enriched target, Ge(Li) detector. Interacting boson, boson expansion models.

doi: 10.1103/PhysRevC.23.1938
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1978FL07 Phys.Rev. C18, 1566 (1978)

D.S.Flynn, K.K.Sekharan, B.A.Hiller, H.Laumer, J.L.Weil, F.Gabbard

Cross Sections and Reaction Rates for ²³Na(p, n)²³Mg, ²⁷Al(p, n)²⁷Si, ²⁷Al(α, n)³⁰P, ²⁹Si(α, n)³²S, and ³⁰Si(α, n)³³S

NUCLEAR REACTIONS ²³Na, ²⁷Al(p, n), E=5.0-6.5 MeV; ²⁷Al, ^29,30Si(α, n), E=2.8-6.8 MeV; measured σ(E). ²⁷Si(n, p), E=0-0.55 MeV; ³⁰P(n, α), E=0.4-0.9 MeV; ^32,33S(n, α), E=0-2.3 MeV; deduced σ(E); deduced nucleosynthesis reaction rates. ²³Mg(n, p), E=0-3 MeV; calculated σ(E); deduced nucleosynthesis reaction rates.

doi: 10.1103/PhysRevC.18.1566
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1978GL04 Phys.Rev. C18, 2520 (1978)

G.P.Glasgow, F.D.McDaniel, J.L.Weil, J.D.Brandenberger, M.T.McEllistrem

Level and Decay Scheme Studies in ⁹²Zr and ⁹⁴Zr via (n, n'γ) Reactions

NUCLEAR REACTIONS ^92,94Zr(n, n'γ), E=2.2-3.7 MeV; measured Eγ, σ(E, Eγ, 90°), σ(Eγ, θγ). ^92,94Zr deduced levels, δ, J, π, branching ratio. Enriched targets, Ge(Li) detectors, tof background suppression. Statistical model calculation.

doi: 10.1103/PhysRevC.18.2520
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10409.

1977CO26 Phys.Rev. C16, 2223 (1977)

D.F.Coope, S.N.Tripathi, M.C.Schell, J.L.Weil, M.T.McEllistrem

Strong Collective Excitations in Low Energy Neutron Scattering from Transitional Nuclei

NUCLEAR REACTIONS ^148,150,152Sm(n, n), (n, n'), (n, n'γ), E=2.47 MeV; measured σ(θ). Coupled channels, statistical model analysis.

doi: 10.1103/PhysRevC.16.2223
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1976BI09 Phys.Rev. C14, 1586 (1976)

C.R.Bingham, L.L.Riedinger, F.E.Turner, B.D.Kern, J.L.Weil, K.J.Hofstetter, J.Lin, E.F.Zganjar, A.V.Ramayya, J.H.Hamilton, J.L.Wood, G.M.Gowdy, R.W.Fink, E.H.Spejewski, W.D.Schmidt-Ott, R.L.Mlekodaj, H.K.Carter, K.S.R.Sastry

Decay of Mass-Separated ¹⁹⁰Tl and ¹⁹⁰Hg

RADIOACTIVITY ^190,190mTl, ¹⁹⁰Hg [from Ta, W(¹⁶O, X)]; measured Eγ, Iγ, I(ce), Eβ, γX-ray-coin, γγ-coin, T_1/2; deduced log ft, Q, ICC. ¹⁹⁰Hg, ¹⁹⁰Au deduced levels, J, π, λ.

doi: 10.1103/PhysRevC.14.1586
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1976GO02 Phys.Rev. C13, 1601 (1976)

G.M.Gowdy, A.C.Xenoulis, J.L.Wood, K.R.Baker, R.W.Fink, J.L.Weil, B.D.Kern, K.J.Hofstetter, E.H.Spejewski, R.L.Mlekodaj, H.K.Carter, W.D.Schmidt-Ott, J.Lin, C.R.Bingham, L.L.Riedinger, E.F.Zganjar, K.S.R.Sastry, A.V.Ramayya, J.H.Hamilton

On-Line Mass Separator Investigation of the New Isotope 2.9-sec ¹¹⁶I

RADIOACTIVITY ¹¹⁶I, ¹¹⁶Xe; measured Eγ, Iγ, T_1/2, βγ(t); deduced Q, log ft. ¹¹⁶I deduced J, π. ¹¹⁶Te, ¹¹⁶Xe deduced levels, J, π.

doi: 10.1103/PhysRevC.13.1601
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1976HA25 Izv.Akad.Nauk SSSR, Ser.Fiz. 40, 2 (1976); Bull.Acad.Sci.USSR, Phys.Ser. 40, No.1, 1 (1976)

J.H.Hamilton, K.R.Baker, C.R.Bingham, E.L.Bosworth, H.K.Carter, J.D.Cole, R.W.Fink, G.Garcia Bermudez, G.W.Gowdy, K.J.Hofstetter, M.A.Ijaz, A.C.Kahler, B.D.Kern, W.Lourens, B.Martin, R.L.Mlekodaj, A.V.Ramayya, L.L.Riedinger, W.D.Schmidt-Ott, E.H.Spejewski, B.N.Subba Rao, E.L.Robinson, K.S.Toth, F.Turner, J.L.Weil, J.L.Wood, A.Xenoulis, E.F.Zganjar

New Isotope ¹⁹³Pb and the Structure of ¹⁹³Tl; Shape Coexistence in ¹⁸⁸Hg and in ¹⁸⁹Au; and a New Ion Source: Recent UNISOR Research

RADIOACTIVITY ¹⁹³Pb; measured T_1/2, Eγ, Iγ, γγ-coin. ¹⁸⁸Tl; measured Eγ, Iγ, γγ-coin, I(ce), γce-coin. ¹⁸⁹Tl, ¹⁸⁹Hg; measured Eγ, Iγ, γγ-, γX-, γce-coin. ^188,189Hg, ¹⁹³Tl deduced levels, J, π, shape isomers.

1975HA27 Phys.Rev.Lett. 35, 562 (1975)

J.H.Hamilton, A.V.Ramayya, E.L.Bosworth, W.Lourens, J.D.Cole, B.Van Nooijen, G.Garcia-Bermudez, B.Martin, B.N.Subba Rao, H.Kawakami, L.L.Riedinger, C.R.Bingham, F.Turner, E.F.Zganjar, E.H.Spejewski, H.K.Carter, R.L.Mlekodaj, W.D.Schmidt-Ott, K.R.Baker, R.W.Fink, G.M.Gowdy, J.L.Wood, A.Xenoulis, B.D.Kern, K.J.Hofstetter, J.L.Weil, K.S.Toth, M.A.Ijaz, K.F.R.Faftry

Crossing of Near-Spherical and Deformed Bands in ^186,188Hg and New Isotopes ^186,188Tl

RADIOACTIVITY ^186,188Tl [from ¹⁸¹Ta(¹⁶O, 9nγ), (¹⁶O, 11nγ), E=143-145 MeV]; measured T_1/2, Eγ, Iγ, γce-, γγ-coin, γ(t); deduced ICC. ^186,188Hg deduced levels, J, π, K.

doi: 10.1103/PhysRevLett.35.562
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1975ZG01 Phys.Lett. 58B, 159 (1975)

E.F.Zganjar, J.L.Wood, R.W.Fink, L.L.Riedinger, C.R.Bingham, B.D.Kern, J.L.Weil, J.H.Hamilton, A.V.Ramayya, E.H.Spejewski, R.L.Mlekodaj, H.K.Carter, W.D.Schmidt-Ott

Rotation-Aligned Coupling and Axial Asymmetry in ¹⁸⁹-¹⁹⁵Au

RADIOACTIVITY ^{189,189m,191,191m,193}Hg; measured γγ(t), γ X-ray(t), Eγ, Iγ, I(ce); deduced ICC. ^189,191,193Au deduced levels. ^{189,191,193,195}Au deduced systematics.

doi: 10.1016/0370-2693(75)90627-9
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1974HA10 Izv.Akad.Nauk SSSR, Ser.Fiz. 38, 2036 (1974); Bull.Acad.Sci.USSR, Phys.Ser. 38, No.10, 22 (1974)

J.H.Hamilton, E.H.Spejewski, R.L.Mlekodaj, W.-D.Schmidt-Ott, R.W.Fink, A.Xenoulis, K.R.Baker, J.L.Wood, G.Gowdy, H.K.Carter, B.D.Kern, K.J.Hofstetter, J.L.Weil, E.F.Zganjar, K.S.R.Sastry, F.T.Avignone, C.R.Bingham, L.L.Riedinger, L.Harwood, F.Turner, I.A.Sellin, D.J.Pegg, J.Lin, A.V.Ramayya, S.Lee, G.Garcia-Bermudez, E.Bosworth, K.S.Toth, N.R.Johnson

Initial UNISOR Research: New Isotopes ¹⁸⁶Tl, ¹⁸⁸Tl, ¹¹⁶I; Decays of ^189,190Tl, ¹¹⁷Xe, and ¹¹⁷I; and Off-Line Atomic and Nuclear Studies

RADIOACTIVITY ^116,117Xe, ^116,117I, ^{186,188,189,190}Tl; measured T_1/2, Eγ, Iγ, γγ, Eβ; deduced Q(β). ¹²⁶I measured γγ(θ, H). ¹¹⁷I, ¹¹⁶Te, ^188,190Hg deduced levels, J, π. ¹²⁶Xe level deduced g. On-line isotope separator UNISOR.

1973GL03 Priv.Comm. (June 1973)

G.P.Glasgow, F.D.McDaniel, L.D.Brandenburger, J.L.Weil, M.T.McEllistrem

Resolution of Ambiguities in the Level Scheme of ⁹⁴Zr

1973OB02 Phys.Rev. C7, 1076 (1973)

A.W.Obst, J.L.Weil

Scattering of 9.8-MeV Neutrons from Silicon and Sulfur

NUCLEAR REACTIONS Si, S(n, n'), E=9.8 MeV; measured σ(En', θ). Deduced optical model parameters.

doi: 10.1103/PhysRevC.7.1076
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1972AL45 Phys.Lett. 41B, 577 (1972)

B.W.Allardyce, C.J.Batty, D.J.Baugh, E.Friedman, G.Heymann, J.L.Weil, M.E.Cage, G.J.Pyle, G.T.A.Squier, A.S.Clough, J.Cox, D.F.Jackson, S.Murugesu, V.Rajaratnam

Ratio of Pion-Nucleus Reaction Cross Sections and the Neutron Density Distribution for Lead

NUCLEAR REACTIONS C, Pb(π^-, X), (π⁺, X), E=0.71-2.0 GeV/c; measured σ ratios.

doi: 10.1016/0370-2693(72)90638-7
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1972GA13 Phys.Rev. C5, 1508 (1972)

W.Galati, J.D.Brandenberger, J.L.Weil

Scattering of Neutrons by Carbon from 3 to 7 MeV

NUCLEAR REACTIONS C(n, n), (n, n'), E=3-7 MeV; measured σ(E;θ); deduced phase shifts. ¹³C resonances deduced J, π, level-width.

doi: 10.1103/PhysRevC.5.1508
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1972OB01 Phys.Rev. C5, 738 (1972)

A.W.Obst, T.B.Grandy, J.L.Weil

Reaction ⁹Be(α, n)¹²C from 1.7 to 6.4 MeV

NUCLEAR REACTIONS ⁹Be(α, n), E=1.69-6.44 MeV; measured σ(E;θ).

doi: 10.1103/PhysRevC.5.738
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1972SC28 Nucl.Phys. A192, 609 (1972)

R.L.Schulte, M.Cosack, A.W.Obst, J.L.Weil

²H+d Reactions from 1.96 to 6.20 MeV

NUCLEAR REACTIONS ²H(d, d), ²H(d, ³He), ²H(d, t), ²H(d, p), ²H(d, n), E=2.0-6.2 MeV; measured σ(E, θ); deduced ²H(d, n) σ(θ). Enriched target.

doi: 10.1016/0375-9474(72)90093-0
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1971DI12 Aust.J.Phys. 24, 139 (1971)

G.U.Din, J.L.Weil

The ¹⁸O(³He, n₀)²⁰Ne and ¹⁸O(³He, n₁)²⁰Ne Reactions from 2.0 to 4.6 MeV

NUCLEAR REACTIONS ¹⁸O(³He, n), E=2-4.6 MeV; measured σ(E;θ); deduced reaction mechanism.

1969CO14 Nucl. Phys. A136, 532 (1969)

M.Cosack, M.K.Leung, M.T.McEllistrem, R.L.Schulte, M.M.Stautberg, J.L.Weil, J.C.Norman

Threshold Effects in the ⁴⁰Ar(d, p)⁴¹Ar Reaction

NUCLEAR REACTIONS ⁴⁰Ar(d, p), E = 2.10-5.45 MeV; measured σ(E;Ep, θ). ⁴⁰Ar(d, np), E =4.2-5.0 MeV; measured σ(E;Ep, θ); deduced (d, n) threshold. Natural target.

doi: 10.1016/0375-9474(69)90125-0
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1968SC11 Phys.Rev. 172, 1139 (1968)

H.L.Scott, W.Galati, J.L.Weil, M.T.McEllistrem

Proton-Induced Reactions on ⁴⁰Ar and Analogs of ⁴¹Ar Levels

NUCLEAR STRUCTURE ⁴¹K; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.172.1139
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1967BA40 Phys.Rev. 161, 928 (1967)

A.W.Barrows, Jr., F.Gabbard, J.L.Weil

¹⁹F(d, n)²⁰Ne Reaction from 2.5 to 6.5 MeV

NUCLEAR STRUCTURE ¹⁹F, ²⁰Ne; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.161.928
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1966DI04 Nucl.Phys. 86, 509(1966)

G.U.Din, J.L.Weil

The Reactions ¹¹B(³He, N)¹³N and ⁷Li(³He, N)⁹B from 1.5 to 5.5 MeV Bombarding Energy

NUCLEAR REACTIONS ⁷Li, ¹¹B(³He, n₀), E = 1.5-5.5 MeV; measured σ(E, θ). ¹⁰B, ¹⁴N deduced levels, level-width. Enriched targets.

doi: 10.1016/0029-5582(66)90493-7
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1966SW04 Nucl.Phys. 86, 119(1966)

J.B.Swint, A.C.L.Barnard, T.B.Clegg, J.L.Weil

Cross Sections as a Function of Energy for the Scattering of Protons from ¹²C

NUCLEAR REACTIONS ¹²C(p, p), E = 4.7-12.8 MeV; ¹²C(p, p'), E = 6.0-12.8 MeV; measured σ(E, θ). ¹³N deduced levels. Natural target.

doi: 10.1016/0029-5582(66)90295-1
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1965DI06 Nucl.Phys. 71, 641 (1965)

G.Din, J.L.Weil

The Reaction Be⁹(He³, n)C¹¹ from 1.3 to 5.4 MeV

NUCLEAR REACTIONS ⁹Be(³He, n), E = 1.30-5.35 MeV; measured σ(E;En, θ), L.

doi: 10.1016/0029-5582(65)90772-8
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1965DI07 Nucl.Phys. 73, 161 (1965)

G.U.Din, J.L.Weil

The ¹³C(³He, n₀)¹⁵O Reaction at 1.4 to 5.8 MeV

NUCLEAR REACTIONS ¹³C(³He, n), E = 1.4-5.8 MeV; measured σ(E;θ n). Enriched target.

doi: 10.1016/0029-5582(65)90163-X
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1964BA08 Nucl. Phys. 50, 604 (1964)

A.C.L.Barnard, C.M.Jones, J.L.Weil

Elastic Scattering of 2-11 MeV Protons by He⁴

doi: 10.1016/0029-5582(64)90233-0
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1964BA40 Bull. Am. Phys. Soc. 9, No. 6, 665, Y3 (1964)

A.Barrows, F.Gabbard, J.L.Weil, T.Young

F¹⁹(d, n)Ne²⁰ Reaction, 2.5-6.0 MeV

NUCLEAR STRUCTURE ¹⁹F, ²⁰Ne; measured not abstracted; deduced nuclear properties.

1964CL03 Nucl. Phys. 50, 621 (1964)

T.B.Clegg, A.C.L.Barnard, J.B.Swint, J.L.Weil

The Elastic Scattering of Protons from He³ from 4.5 to 11.5 MeV

doi: 10.1016/0029-5582(64)90234-2
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1964SI09 Nucl.Phys. 52, 273 (1964)

R.H.Siemssen, R.Felst, M.Cosack, J.L.Weil

The Reaction F¹⁹(d, n)Ne²⁰

NUCLEAR STRUCTURE ¹⁹F; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(64)90692-3
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1964SW02 Bull.Am.Phys.Soc. 9, No.4, 408, CA11 (1964)

J.B.Swint, T.B.Clegg, J.L.Weil, C.M.Jones, A.C.L.Barnard

Scattering of Protons by ¹²C

NUCLEAR STRUCTURE ¹²C; measured not abstracted; deduced nuclear properties.

1963BA04 Bull.Am.Phys.Soc. 8, No.2, 124, U4 (1963)

A.C.L.Barnard, C.M.Jones, J.L.Weil

He⁴(p, p)He⁴ Reaction and Phase Shifts

NUCLEAR STRUCTURE ⁴He; measured not abstracted; deduced nuclear properties.

1963CL01 Bull.Am.Phys.Soc. 8, No.2, 124, U3 (1963)

T.B.Clegg, A.C.L.Barnard, J.B.Swint, J.L.Weil

He³(p, p)He³, 4.5-10.4 MeV

NUCLEAR STRUCTURE ³He; measured not abstracted; deduced nuclear properties.

1963DI01 Bull.Am.Phys.Soc. 8, No.2, 115, I4 (1963)

G.U.Din, J.L.Weil

Excitation Functions of Li⁷(He³, n)B⁹ and O¹⁸(He³, n)Ne²⁰ and the Angular Distribution of O¹⁸(He³, n)Ne²⁰

NUCLEAR STRUCTURE ⁷Li; measured not abstracted; deduced nuclear properties.

1963SC03 Bull.Am.Phys.Soc. 8, No.2, 127, V6 (1963)

H.D.Scott, P.H.Stelson, J.L.Weil, A.C.L.Barnard

Differential Cross Sections for Reactions from Protons on A⁴⁰

NUCLEAR STRUCTURE ⁴⁰Ar; measured not abstracted; deduced nuclear properties.

1963WE01 Bull.Am.Phys.Soc. 8, No.2, 115, I5 (1963)

J.L.Weil, M.Cosack, R.Felst, R.Siemssen

Angular Distributions of F¹⁹(d, n)Ne²⁰

NUCLEAR STRUCTURE ¹⁹F; measured not abstracted; deduced nuclear properties.

1962TO12 Nuclear Phys. 39, 541 (1962); Erratum Nucl.Phys. 43, 528 (1963)

T.A.Tombrello, C.Miller Jones, G.C.Phillips, J.L.Weil

The Scattering of Protons from He³

NUCLEAR STRUCTURE ³He; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(62)90412-1
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1962WE01 Bull.Am.Phys.Soc. 7, No.1, 59, R5 (1962)

J.L.Weil, G.U.Din, H.M.Kuan, P.R.Almond

Be⁹(He³, n)C¹¹ Reaction

NUCLEAR STRUCTURE ⁹Be; measured not abstracted; deduced nuclear properties.

1962WE03 Bull.Am.Phys.Soc. 7, No.2, 111, A5 (1962)

J.L.Weil, G.U.Din

B¹¹(He³, n)N¹³ and C¹³(He³, n)O¹⁵ Reactions

NUCLEAR STRUCTURE ¹¹B, ¹³C; measured not abstracted; deduced nuclear properties.

1961TO09 Bull.Am.Phys.Soc. 6, No.6, 507, E14 (1961)

T.A.Tombrello, C.M.Jones, G.C.Phillips, J.L.Weil

Elastic Scattering of Protons from He³

NUCLEAR STRUCTURE ³He; measured not abstracted; deduced nuclear properties.

1960RE02 Bull.Am.Phys.Soc. 5, No.2, 110, N3 (1960)

T.Retz-Schmidt, T.W.Bonner, G.U.Din, J.L.Weil

Absolute Yields of Neutron Groups from Be⁹(α, n)C¹²

NUCLEAR STRUCTURE ¹²C; measured not abstracted; deduced nuclear properties.

1960RE07 Phys.Rev. 119, 1079 (1960)

T.Retz-Schmidt, J.L.Weil

Excitation Curves and Angular Distributions for N¹⁴(d, n)O¹⁵

NUCLEAR STRUCTURE ¹⁶O; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.119.1079
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1959WE33 Bull.Am.Phys.Soc. 4, No.8, 444, C8 (1959)

J.L.Weil, T.Retz-Schmidt

N¹⁴(d, n)O¹⁵ Excitation Curves and Angular Distributions

1958JO28 Phys.Rev. 112, 1252 (1958)

K.W.Jones, L.J.Lidofsky, J.L.Weil

N¹⁵(p, n)O¹⁵ Reaction Study

doi: 10.1103/PhysRev.112.1252
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1958JO29 Phys.Rev.Letters 1, 391 (1958)

K.W.Jones, L.J.Lidofsky, J.L.Weil

N¹⁵(p, n)O¹⁵ Reaction Study

doi: 10.1103/PhysRevLett.1.391
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1958WE26 Phys.Rev. 110, 466 (1958)

J.L.Weil, K.W.Jones

Total Neutron Cross Sections of Mg, Al, Fe, Cu, Zn, Mo, and Pb from 4 to 8 MeV

doi: 10.1103/PhysRev.110.466
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1958WE31 Phys.Rev. 112, 1975 (1958)

J.L.Weil, K.W.Jones

N¹⁴(d, n)O¹⁵ and N¹⁵(d, n)O¹⁶ Reactions

doi: 10.1103/PhysRev.112.1975
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