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NSR database version of April 27, 2024.

Search: Author = J.Weber

Found 29 matches.

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2022AM08      Acta Phys.Pol. B53, A1 (2022)

S.Amoroso, A.Apyan, N.Armesto, R.D.Ball, V.Bertone, C.Bissolotti, J.Blumlein, R.Boughezal, G.Bozzi, D.Britzger, A.Buckley, A.Candido, S.Carrazza, F.G.Celiberto, S.Cerci, G.Chachamis, A.M.Cooper-Sarkar, A.Courtoy, T.Cridge, J.M.Cruz-Martinez, F.Giuli, M.G.Guzzi, C.Gwenlan, L.A.Harland-Lang, F.Hekhorn, M.Hentschinski, T.J.Hobbs, S.Hoeche, A.Huss, J.Huston, S.Jadach, J.Jalilian-Marian, M.Klein, G.K.Krintiras, H.-W.Lin, C.Loizides, G.Magni, B.Malaescu, B.Mistlberger, S.Moch, P.M.Nadolsky, E.R.Nocera, F.I.Olness, F.Petriello, J.Pires, K.Rabbertz, J.Rojo, C.Royon, G.Schnell, C.Schwan, A.Siodmok, D.E.Soper, M.Sutton, R.S.Thorne, M.Ubiali, G.Vita, J.H.Weber, J.Whitehead, K.Xie, C.-P.Yuan, B.Zhou

Snowmass 2021 Whitepaper: Proton Structure at the Precision Frontier

doi: 10.5506/APhysPolB.53.12-A1
Citations: PlumX Metrics


2019PE05      Nucl.Phys. A982, 735c (2019)

P.Petreczky, A.Rothkopf, J.Weber

Realistic in-medium heavy-quark potential from high statistics lattice QCD simulations

doi: 10.1016/j.nuclphysa.2018.10.012
Citations: PlumX Metrics


2017PE18      Nucl.Phys. A967, 592 (2017)

P.Petreczky, J.Weber, for the TUMQCD Collaboration

Lattice Calculations of Heavy Quark Potential at Finite Temperature

doi: 10.1016/j.nuclphysa.2017.04.011
Citations: PlumX Metrics


1999AN44      J.Phys.(London) G25, 2161 (1999)

T.Antoni, W.D.Apel, K.Bekk, K.Bernlohr, E.Bollmann, K.Daumiller, P.Doll, J.Engler, F.Fessler, H.J.Gils, R.Glasstetter, R.Haeusler, W.Hafemann, A.Haungs, D.Heck, J.R.Horandel, T.Holst, K.-H.Kampert, H.O.Klages, J.Knapp, H.J.Mathes, H.J.Mayer, J.Milke, D.Muhlenberg, J.Oehlschlager, H.Rebel, M.Risse, M.Roth, G.Schatz, H.Schieler, F.K.Schmidt, T.Thouw, H.Ulrich, J.Unger, J.H.Weber, J.Wentz, T.Wiegert, D.Wochele, J.Kempa, T.Wibig, J.Zabierowski, F.Badea, H.Bozdog, I.M.Brancis, M.Petcu, B.Vulpescu, A.Chilingarian, A.Vardanyan

Test of High-Energy Interaction Models using the Hadronic Core of EAS


1999WE03      Phys.Rev.Lett. 82, 516 (1999)

J.M.Weber, E.Leber, M.-W.Ruf, H.Hotop

Nuclear-Excited Feshbach Resonances in Electron Attachment to Molecular Clusters

doi: 10.1103/PhysRevLett.82.516
Citations: PlumX Metrics


1981WE05      Phys.Rev. C23, 2100 (1981)

J.Weber, H.C.Britt, J.B.Wilhelmy

Comparison of 252Cf Spontaneous Fission with 250Cf(t, pf)

RADIOACTIVITY, Fission 252Cf(SF); measured σ(fragment mass), average total kinetic energy vs mass.

NUCLEAR REACTIONS, Fission 250Cf(t, pF), E=16 MeV; measured σ(fragment mass), average total kinetic energy vs mass, excitation energy.

doi: 10.1103/PhysRevC.23.2100
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12709.


1981WE17      Helv.Phys.Acta 54, 547 (1981)

J.Weber

The (n, d) Differential Elastic Cross Section at 2 MeV

NUCLEAR REACTIONS 2H(n, n), E=2.016 MeV; measured σ(θ); deduced normalization factor. Deuterated NE213 liquid scintillator, Tof.

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21874.


1980HO04      Phys.Rev. C21, 972 (1980)

D.C.Hoffman, J.B.Wilhelmy, J.Weber, W.R.Daniels, E.K.Hulet, R.W.Lougheed, J.H.Landrum, J.F.Wild, R.J.Dupzyk

12.3-min 256Cf and 43-min 258Md and Systematics of the Spontaneous Fission Properties of Heavy Nuclides

RADIOACTIVITY 256Cf(SF) [from 254Cf(t, p), E=16 MeV]; measured T1/2, (fragment)(fragment)-coin; deduced total kinetic energy, mass distribution. 258Md[from 255Es(α, n), E=26.3 MeV]; measured T1/2. 258Fm (SF) [from ϵ decay of 258Md]; measured (fragment)(fragment)-coin; deduced total kinetic energy, mass distribution.

doi: 10.1103/PhysRevC.21.972
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10923.


1980HU03      Phys.Rev. C21, 966 (1980)

E.K.Hulet, R.W.Lougheed, J.H.Landrum, J.F.Wild, D.C.Hoffman, J.Weber, J.B.Wilhelmy

Spontaneous Fission of 259Fm

NUCLEAR REACTIONS 257Fm(t, p), E=16 MeV; measured σ, (fragment)(fragment)-coin. 259Fm deduced SF isomer, T1/2, fragment mass distribution.

doi: 10.1103/PhysRevC.21.966
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10924.


1979CH13      Nucl.Phys. A319, 71 (1979)

P.Chatelain, Y.Onel, J.Weber

The (n, d) Elastic Differential Cross Section at E = 2.48 and 3.28 MeV

NUCLEAR REACTIONS 2H(n, n), E=2.48, 3.28 MeV; measured σ(E, θ).

doi: 10.1016/0375-9474(79)90172-6
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21623.


1978BO28      J.Phys.(London) G4, 1313 (1978)

D.Bovet, P.Chatelain, R.Viennet, J.Weber

Measurement of the Depolarisation Factor D(θ) for the Reaction 2H(n, n)2H at 2.45 MeV

NUCLEAR REACTIONS 2H(polarized n, n), E=2.45 MeV; measured depolarization factor. Comparison with effective-range-approximation analyses, predictions.

doi: 10.1088/0305-4616/4/8/013
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21715.


1978BR07      Phys.Rev.Lett. 40, 1010 (1978)

H.C.Britt, A.Gavron, P.D.Goldstone, R.Schoenmackers, J.Weber, J.B.Wilhelmy

Yet More Complexity in Fission: Barriers for Nuclei with N = 150-154

NUCLEAR REACTIONS 244Pu, 246,248Cm, 250Cf(t, p), (d, p), (p, p'), E not given; measured fission probability distributions.

doi: 10.1103/PhysRevLett.40.1010
Citations: PlumX Metrics


1978CH20      Helv.Phys.Acta 51, 333 (1978)

P.Chatelain, Y.Onel, J.Weber

(n, d) Elastic Differential Cross Section at 2.48 and 3.28 MeV

NUCLEAR REACTIONS 2H(n, n), E=2.48, 3.28 MeV; measured σ(θ).

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21623.


1978SP04      Z.Phys. A287, 57 (1978)

P.Sperr, W.Wagner, H.Essel, K.Hartel, W.Henning, P.Kienle, H.J.Korner, K.E.Rehm, J.Weber

Search for Delayed Fission Products from Superheavy Nuclei in the Reaction 136Xe + 208Pb

NUCLEAR REACTIONS 208Pb(136Xe, X), E(cm)=470 MeV; measured upper limit production σ for superheavy elements Z=108-116, fission mean life.

doi: 10.1007/BF01408361
Citations: PlumX Metrics


1978WI12      S.Afr.J.Phys. 1, 116 (1978)

J.B.Wilhelmy, H.C.Britt, D.C.Hoffman, W.R.Daniels, E.Cheifetz, A.Gavron, J.Weber, E.K.Hulet, J.H.Landrum, R.W.Lougheed, J.F.Wild

Fission Properties of the Heavy Actinides

NUCLEAR REACTIONS 254Es(d, pF), (t, pF), E not given; measured fission barriers.

RADIOACTIVITY, Fission 256Cf(SF) [from 254Cf(t, p)]; 258Fm(SF) [from 255Es(α, n)258Md+electron capture]; 259Fm(SF) [from 257Fm(t, p)]; measured fragment mass distribution, average kinetic energy release.


1977GA09      Phys.Rev. C15, 2238 (1977)

A.Gavron, H.C.Britt, P.D.Goldstone, R.Schoenmackers, J.Weber, J.B.Wilhelmy

Γn/Γf in Heavy Actinides

NUCLEAR REACTIONS 244Pu, 245,246,248Cm, 249,250Cf(3He, d), (3He, t), E=8, 11 MeV; measured fission probability of compound systems 244,245Am, 245,246,247,248,249Bk, 249,250,251Es.

doi: 10.1103/PhysRevC.15.2238
Citations: PlumX Metrics


1976GA11      Phys.Rev. C13, 2374 (1976)

A.Gavron, H.C.Britt, E.Konecny, J.Weber, J.B.Wilhelmy

Γn/Γf for Actinide Nuclei Using (3He, df) and (3He, tf) Reactions

NUCLEAR STRUCTURE 230,231,232,233Pa, 231,232U, 233,234,235,236,237,238,239Np, 237,238Pu, 239,240,241,242,243Am, 241,242,243,244Cm; measured fission probability in 3He induced reactions; deduced barrier heights, average Γn/Γf.

NUCLEAR REACTIONS 230,232Th, 231Pa, 234,236,238U, 237Np, 239,241Pu, 241,243Am(3He, df), (3He, tf); 232U, 242Pu(3He, df); E=25 MeV; measured fission spectra; deduced barrier heights, average neutron-, fission-widths. 230,231,232,233Pa, 231,232U, 233,234,235,236,237,238,239Np, 237,238Pu, 239,240,241,242,243Am, 241,242,243,244Cm deduced fission probability.

doi: 10.1103/PhysRevC.13.2374
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0767.


1976WE03      Phys.Rev. C13, 189 (1976)

J.Weber, B.R.Erdal, A.Gavron, J.B.Wilhelmy

Mass and Kinetic Energy Measurements of Fragments from the Isomeric and Excited State Fission of 242Am

RADIOACTIVITY, Fission 242mAm(SF); measured T1/2, σ(E(fragment mass)).

NUCLEAR REACTIONS 241Am(d, pF), E=15 MeV; measured σ(E(fragment mass)).

doi: 10.1103/PhysRevC.13.189
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14604.


1976WE13      Phys.Rev. C13, 2413 (1976)

J.Weber, H.C.Britt, A.Gavron, E.Konecny, J.B.Wilhelmy

Fission of 228Ra

NUCLEAR REACTIONS 226Ra(t, F), E=23 MeV; measured symmetric, asymmetric component fission probability; deduced fission barrier parameters, mass distributions.

doi: 10.1103/PhysRevC.13.2413
Citations: PlumX Metrics


1975GA02      Phys.Rev.Lett. 34, 827 (1975)

A.Gavron, H.C.Britt, E.Konecny, J.Weber, J.B.Wilhelmy

Measurement and Interpretation of Gamma(n)/Gamma(f) for Actinide Nuclei

NUCLEAR REACTIONS 232Th, 231Pa, 236U, 237Np, 240Pu, 241Am(3He, dF), (3He, tF). 232,233Pa, 231,232U, 236,237Np, 237,238Pu, 240,241Am, 241,242Cm; measured σ; deduced neutron-to-fission width.

doi: 10.1103/PhysRevLett.34.827
Citations: PlumX Metrics


1974BO04      Helv.Phys.Acta 46, 659 (1974)

D.Bovet, S.Jaccard, J.Weber

Sur la Determination des Phases Doublets pour la Diffusion n-d a Basse Energie

NUCLEAR REACTIONS 2H(n, n); measured nothing. Deduced phase shifts.


1974WE03      Nucl.Phys. A221, 414 (1974)

J.Weber, H.J.Specht, E.Konecny, D.Heunemann

Fragment Mass and Kinetic Energy Distribution in Isomeric Fission of 240Pu

RADIOACTIVITY 240mPu; measured fragment mass, kinetic energy distribution.

doi: 10.1016/0375-9474(74)90328-5
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22071.


1973KO17      Phys.Lett. 45B, 329 (1973)

E.Konecny, H.J.Specht, J.Weber

Symmetric and Asymmetric Fission of Ac Isotopes Near the Fission Threshold

NUCLEAR REACTIONS 226Ra(3He, pF), (3He, dF), E=23.5 MeV; measured P(fragment)(θ), d(fragment)(θ). 227,228Ac deduced fission probability, fragment anisotropy(E).

doi: 10.1016/0370-2693(73)90047-6
Citations: PlumX Metrics


1972KO10      Nucl.Phys. A187, 426 (1972)

E.Konecny, H.J.Specht, J.Weber, H.Weigmann, R.L.Ferguson, P.Osterman, M.Waldschmidt, G.Siegert

Search for Conversion Electrons Populating the 236U Fission Isomer

NUCLEAR REACTIONS, Fission 235U(n, γF), E=thermal; measured (fragment)(ce)-coin, -delay; deduced upper limit for isomeric/prompt fission ratio.

doi: 10.1016/0375-9474(72)90586-6
Citations: PlumX Metrics


1972SP06      Phys.Lett. 41B, 43 (1972)

H.J.Specht, J.Weber, E.Konecny, D.Heunemann

Identification of a Rotational Band in the 240Pu Fission Isomer

RADIOACTIVITY, Fission 240Pu(SF) [from 238U(α, 2nγ); E=25 MeV]; measured I(ce), (α)(fragment)-delay, E(ce). 240mPu deduced levels, rotational band structure.

doi: 10.1016/0370-2693(72)90363-2
Citations: PlumX Metrics


1971JA17      Helv.Phys.Acta 44, 502 (1971)

S.Jaccard, J.-F.Germond, J.Piffaretti, J.Weber

Polarisation des Neutrons Emis par la Reaction 12C(d, n)13N Sous 20° Lab. Pour E=2.75 MeV et 3 MeV

NUCLEAR REACTIONS 12C(d, n), E=2.71, 2.96 MeV; measured P(n).


1963BE15      Nucl.Phys. 42, 1 (1963)

L.E.Beghian, K.Sugimoto, M.H.Wachter, J.Weber

Neutron Polarization in the 1 MeV Region by Elastic Scattering on C, O and D

NUCLEAR STRUCTURE O, C, 2H; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(63)90709-0
Citations: PlumX Metrics


1959WE28      Bull.soc.neuchatel.sci.nat. 82, 161 (1959)

J.Weber, J.Rossel


1958RO48      Helv.Phys.Acta 31, 727 (1958)

J.Rossel, J.Weber

The Reaction K40(nth, p)Ar40

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23512.


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Note: The following list of authors and aliases matches the search parameter J.Weber: , J.H.WEBER, J.M.WEBER