NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = H.R.von Gunten Found 37 matches. 1992TU04 Phys.Rev. C46, 1364 (1992) A.Turler, H.R.von Gunten, J.D.Leyba, D.C.Hoffman, D.M.Lee, K.E.Gregorich, D.A.Bennett, R.M.Chasteler, C.M.Gannett, H.L.Hall, R.A.Henderson, M.J.Nurmia Actinide Production from the Interactions of 40Ca and 44Ca with 248Cm and a Comparison with the 48Ca + 248Cm System NUCLEAR REACTIONS 248Cm(40Ca, X), (44Ca, X), E=231-323 MeV; measured production σ(E) for 227Th to 249Cm; deduced isotopic distribution widths.
doi: 10.1103/PhysRevC.46.1364
1990HO27 Nucl.Instrum.Methods Phys.Res. B52, 544 (1990) H.J.Hofmann, G.Bonani, M.Suter, W.Wolfli, D.Zimmermann, H.R.von Gunten A New Determination of the Half-Life of 32Si RADIOACTIVITY 32Si [from 37Cl(p, 2pα), 31P(n, γ)32P(n, p)]; measured T1/2. Source from activation technique.
doi: 10.1016/0168-583X(90)90474-9
1988WE12 Nucl.Instrum.Methods Phys.Res. A269, 615 (1988) R.B.Welch, F.Gyger, D.T.Jost, H.R.Von Gunten, U.Krahenbuhl NEWFIT, a Computer Program for the Analysis of Alpha, X-Ray and Gamma-Ray Spectra NUCLEAR STRUCTURE 152Eu, 76As, 122Sb; calculated γ-spectra. 208,209,210Po, 240,239Pu, 248,250,252Cf; calculated α-spectra. New computer code.
doi: 10.1016/0168-9002(88)90142-8
1987HO27 Nucl.Instrum.Methods Phys.Res. B29, 32 (1987) H.J.Hofmann, J.Beer, G.Bonani, H.R.Von Gunten, S.Raman, M.Suter, R.L.Walker, W.Wolfli, D.Zimmermann 10Be: Half-life and AMS-standards RADIOACTIVITY 10Be(β-); measured decay products, Eβ, Iβ; deduced T1/2. Comparison with available data.
doi: 10.1016/0168-583x(87)90198-4
1986GA06 Phys.Rev. C33, 1983 (1986) H.Gaggeler, W.Bruchle, M.Brugger, M.Schadel, K.Summerer, G.Wirth, J.V.Kratz, M.Lerch, Th.Blaich, G.Herrmann, N.Hildebrand, N.Trautmann, D.Lee, K.J.Moody, K.E.Gregorich, R.B.Welch, G.T.Seaborg, D.C.Hoffman, W.R.Daniels, M.M.Fowler, H.R.von Gunten Production of Cold Target-Like Fragments in the Reaction of 48Ca + 248Cm NUCLEAR REACTIONS 248Cm(Ca, X)210Rn/211Rn/212Rn/219Rn/220Rn/221Rn/222Rn/221Ra/222Ra/223Ra/223Ac/224Ac/225Ac/226Ac/225Th/226Th/227Th/228Th/230U/237U/236Pu/238Pu/243Pu/245Pu/246Pu, E=248-263 MeV; measured residuals yields, σ vs mass; deduced production mechanism.
doi: 10.1103/PhysRevC.33.1983
1985AR02 Phys.Rev.Lett. 54, 406 (1985) P.Armbruster, Y.K.Agarwal, W.Bruchle, M.Brugger, J.P.Dufour, H.Gaggeler, F.P.Hessberger, S.Hofmann, P.Lemmertz, G.Munzenberg, K.Poppensieker, W.Reisdorf, M.Schadel, K.-H.Schmidt, J.H.R.Schneider, W.F.W.Schneider, K.Summerer, D.Vermeulen, G.Wirth, A.Ghiorso, K.E.Gregorich, D.Lee, M.Leino, K.J.Moody, G.T.Seaborg, R.B.Welch, P.Wilmarth, S.Yashita, C.Frink, N.Greulich, G.Herrmann, U.Hickmann, N.Hildebrand, J.V.Kratz, N.Trautmann, M.M.Fowler, D.C.Hoffman, W.R.Daniels, H.R.von Gunten, H.Dornhofer Attempts to Produce Superheavy Elements by Fusion of 48Ca with 248Cm in the Bombarding Energy Range of 4.5-5.2 MeV/u NUCLEAR REACTIONS 248Cm(48Ca, X), E=4.5-5.2 MeV/nucleon; measured superheavy production σ upper limits vs T1/2. Different separation techniques.
doi: 10.1103/PhysRevLett.54.406
1985HO13 Phys.Rev. C31, 1763 (1985) D.C.Hoffman, M.M.Fowler, W.R.Daniels, H.R.von Gunten, D.Lee, K.J.Moody, K.Gregorich, R.Welch, G.T.Seaborg, W.Bruchle, M.Brugger, H.Gaggeler, M.Schadel, K.Summerer, G.Wirth, Th.Blaich, G.Herrmann, N.Hildebrand, J.V.Kratz, M.Lerch, N.Trautmann Excitation Functions for Production of Heavy Actinides from Interactions of 40Ca and 48Ca Ions with 248Cm NUCLEAR REACTIONS 248Cm(40Ca, X)244Bk/245Bk/246Bk/248Bk/248mBk/250Bk/245Cf/246Cf/248Cf/250Cf/252Cf/249Es/250Es/252Es/253Es/254Es/254mEs/250Fm/251Fm/252Fm/254Fm/256Fm, E=221-294 MeV; 248Cm(48Ca, X)245Bk/246Bk/248Bk/248mBk/250Bk/246Cf/248Cf/250Cf/252Cf/253Cf/254Cf/250Es/252Es/253Es/254Es/254mEs/252Fm/254Fm/255Fm/256Fm, E=223-318 MeV; measured residuals production σ(E).
doi: 10.1103/PhysRevC.31.1763
1984LI05 Nucl.Phys. A417, 365 (1984) Y.F.Liu, K.J.Moody, D.Lee, Y.Morita, G.T.Seaborg, H.R.Von Gunten The Decay of 251Bk RADIOACTIVITY 251Bk(β-) [from 248Cm(18O, X), E=97 MeV]; measured β- endpoint energy, T1/2; deduced mass. 251Cf levels deduced Iγ.
doi: 10.1016/0375-9474(84)90402-0
1983LE09 Phys.Rev. C27, 2656 (1983) D.Lee, K.J.Moody, M.J.Nurmia, G.T.Seaborg, H.R.von Gunten, D.C.Hoffman Excitation Functions for Production of Heavy Actinides from Interactions of 18O with 248Cm and 249Cf NUCLEAR REACTIONS, ICPND 248Cm(18O, X)245Bk/246Bk/248Bk/248mBk/250Bk/251Bk/246Cf/248Cf/250Cf/252Cf/253Cf/254Cf/252Es/253Es/254Es/254mEs/255Es/252Fm/253Fm/254Fm/255Fm/256Fm, E=97, 104, 113, 122 MeV; 249Cf(18O, X)245Bk/246Bk/248Bk/248mBk/246Cf/248Cf/250Cf/249Es/250Es/251Es/252Es/253Es/254Es/254mEs/250Fm/252Fm/253Fm/254Fm/255Fm/256Fm/256Md/258Md/258mMd/259No, E=91, 97, 104, 113, 122, 150 MeV; measured residuals production σ(E), mass distribution widths. Activation technique.
doi: 10.1103/PhysRevC.27.2656
1982ER03 Phys.Rev. C25, 2519 (1982) H.N.Erten, A.Grutter, E.Rossler, H.R.von Gunten Charge Distribution in the Reactor-Neutron-Induced Fission of 232Th NUCLEAR REACTIONS, Fission 232Th(n, F), E=reactor spectrum; measured independent yields for 82Br, 86Rb, 96,98Nb, 128Sb, 136Cs. 233Th deduced charge distribution parameters, even-odd proton, neutron enhancement factors. Activation, radiochemical techniques.
doi: 10.1103/PhysRevC.25.2519
1981ER06 Nucl.Sci.Eng. 79, 167 (1981) H.N.Erten, A.Grutter, E.Rossler, H.R.von Gunten Mass Distribution in the Reactor-Neutron-Induced Fission of Thorium-232 NUCLEAR REACTIONS, Fission 232Th(n, F), E=reactor; measured absolute yields for 99Mo, 132Te, σ(fragment mass), yields for 77,78Ge, 83,84Br, 89,90,91,92Sr, 93Y, 95,97Zr, 99Mo, 103,105,106Ru, 109,112Pd, 111,113Ag, 115,117Cd, 127,129Sb, 131,134,135I, 139,140Ba, 132Te, 141,143,144Ce, 147Nd, 149,151Pm, 153Sm.
doi: 10.13182/NSE81-A27405
1981JO04 J.Inorg.Nucl.Chem. 43, 2629 (1981) Independent Yields of 92mNb in the Thermal Neutron-Induced Fission of 233U, 235U and 239Pu NUCLEAR REACTIONS, Fission 233,235U, 239Pu(n, F), E=thermal; measured independent yield of 92mNb; deduced shell closure effect. Activation technique, radiochemical separation.
doi: 10.1016/0022-1902(81)80588-X
1981VO02 Phys.Rev. C23, 1110 (1981) H.R.von Gunten, A.Grutter, H.W.Reist, M.Baggenstos Ground-State Spontaneous-Fission Half-Lives of Uranium Isotopes RADIOACTIVITY, Fission 233,234,235,236U(SF); measured T1/2. 233,235U deduced hindrance factor. Enriched solutions of Uranium, spinner detectors.
doi: 10.1103/PhysRevC.23.1110
1980ZW01 Radiochim.Acta 27, 121 (1980) Independent Yields of 148mPm and 148gPm in the Thermal-Neutron-Induced Fission of 233U and 239Pu NUCLEAR REACTIONS 233U, 239Pu(n, F)148Pm/148mPm, E=thermal; measured residuals independent, isomeric yield ratios. Radiochemical techniques. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21706. 1978BA09 Nucl.Phys. A294, 369 (1978) P.Baertschi, A.Grutter, H.R.von Gunten, H.S.Pruys, M.Rajagopalan, H.W.Reist, E.Rossler Radiochemical Investigation of the Mass Distribution and Probability in Stopped μ- Induced Fission of 238U NUCLEAR REACTIONS 238U(μ-, F); measured mass distribution, absolute fission probability.
doi: 10.1016/0375-9474(78)90224-5
1978GA01 Phys.Rev. C17, 172 (1978) Charge Distribution in the Thermal-Neutron-Induced Fission of 249Cf: Independent and Fractional Cumulative Yields of Isotopes of Nb, I, and Cs NUCLEAR REACTIONS 249Cf(n, F), E=th; measured charge distribution, yields of 96,98Nb, 130,135I, 136Cs. Ge(Li) detector, radiochemical separation.
doi: 10.1103/PhysRevC.17.172
1978GA22 J.Inorg.Nucl.Chem. 40, 1859 (1978) Charge Distribution in the Photofission of 238U with Bremsstrahlung of E (max) 20-50 MeV NUCLEAR REACTIONS 238U(γ, F), E(max)=31 MeV; measured fractional independent yields of 136Cs, 150Pm.
doi: 10.1016/0022-1902(78)80243-7
1978KA05 Nucl.Phys. A295, 141 (1978) Evidence on the Influence of Fission Channels on Fission Phenomena NUCLEAR REACTIONS 239Pu(n, F), E=low; calculated fission widths for 0+ resonances.
doi: 10.1016/0375-9474(78)90025-8
1978KA07 J.Inorg.Nucl.Chem. 40, 377 (1978) Independent Yields of 96Nb and 51 min 98Nb in the Thermal Neutron-Induced Fission of 233U, 235U and 239Pu NUCLEAR REACTIONS 233,235U, 239Pu(n, F), E=th; measured yields for 96,98Nb.
doi: 10.1016/0022-1902(78)80408-4
1978KA09 Phys.Rev. C17, 1510 (1978) Cumulative Mass Yields in the Neutron-Induced Fission of 239Pu at the Resonance Energy of 0.3 eV NUCLEAR REACTIONS 239Pu(n, F), E=0.3 eV; measured Sr, Ag, Cd yields.
doi: 10.1103/PhysRevC.17.1510
1977GA10 J.Inorg.Nucl.Chem. 39, 1105 (1977) Cumulative Yields of Rare Earth Elements in the Thermal Neutron-Induced Fission of 249Cf NUCLEAR REACTIONS 249Cf(n, F), E=th; measured cumulative yields.
doi: 10.1016/0022-1902(77)80284-4
1976BA21 Helv.Phys.Acta 49, 187 (1976) P.Baertschi, A.Grutter, H.R.von Gunten, H.S.Pruys, M.Rajagopalan Stopped Negative Muon-Induced Fission of 238U NUCLEAR REACTIONS 238U(μ-, F), E ≈ 0 MeV; measured fission yields for 91Sr, 93Y, 99Mo, 111Ag, 113Ag, 115Cd, 143Ce; deduced muon induced fission probability.
1976GA38 J.Inorg.Nucl.Chem. 38, 205 (1976) H.Gaggeler, H.R.von Gunten, H.S.Pruys Independent yields of 150Pm in the Thermal Neutron-Induced Fission of 233U, 235U, 239Pu and 249Cf and Cross-Section for the 149Pm(n, γ)150Pm Reaction NUCLEAR REACTIONS 233,235U, 239Pu, 249Cf(n, F)146Pm/148Pm/150Pm/160Tb, 149Pm(n, γ), E thermal; measured fission products, Eγ, Iγ; deduced independent fission yields.
doi: 10.1016/0022-1902(76)80394-6
1976RA01 J.Inorg.Nucl.Chem. 38, 351 (1976) M.Rajagopalan, H.S.Pruys, A.Grutter, E.A.Hermes, H.R.von Gunten Mass Yields in the 14 MeV Neutron-Induced Fission of 238U NUCLEAR REACTIONS 238U(n, F), E=14 MeV; measured yields.
doi: 10.1016/0022-1902(76)80434-4
1975PR05 J.Inorg.Nucl.Chem. 37, 1587 (1975) H.S.Pruys, E.A.Hermes, H.R.Von Gunten The Decay of 152m1Eu and 152m2Eu and Reaction Cross Sections of 153Eu for 14 MeV Neutrons RADIOACTIVITY 152mEu; measured T1/2, Eγ, Iγ. NUCLEAR REACTIONS 153Eu(n, α), (n, p), (n, 2n), E=14 MeV; measured σ.
doi: 10.1016/0022-1902(75)80280-6
1975RA34 Nucl.Sci.Eng. 58, 414 (1975) M.Rajagopalan, H.S.Pruys, A.Grutter, H.R.von Gunten, E.A.Hermes, R.Richmond, E.Rossler, A.Schmid, P.Wydler Mass Yields in the Fission of Uranium-235 and Plutonium-239 in the Neutron Spectrum of a Gas-Cooled Fast Reactor NUCLEAR REACTIONS 235U, 239Pu(n, F), E=reactor spectrum; measured σ(fragment mass).
doi: 10.13182/NSE75-A26796
1974BE02 Phys.Rev. C9, 48 (1974) K.Behringer, A.Grutter, H.R.von Gunten, A.Schmid, A.Wyttenbach, B.Hahn, U.Moser, H.W.Reist Search for Superheavy Elements RADIOACTIVITY Z=110-115 [from natural samples, W(24 GeV p)]; measured spontaneous fission rate. Deduced limits for T1/2, yields.
doi: 10.1103/PhysRevC.9.48
1974EG01 Radiochim.Acta 21, 200 (1974) C.Egger, H.R.von Gunten, A.Schmid, H.S.Pruys Absolute Yields of 99Mo in the Thermal Neutron-Induced Fission of 233U And 239Pu NUCLEAR REACTIONS 233U, 239Pu(n, F), E=thermal; measured 99Mo yields. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22059. 1970VO16 J.Inorg.Nucl.Chem. 32, 3441 (1970) H.R.von Gunten, K.F.Flynn, A.Schmid The Thermal-Neutron Fission Cross Section of 227Th NUCLEAR REACTIONS, Fission 227Th(n, F), E=thermal; measured σ.
doi: 10.1016/0022-1902(70)80151-8
1969FL07 Helv.Chim.Acta 52, 2216 (1969) Massen- und Ladungsverteilung bei der Spaltung von 249Cf mit thermischen Neutronen. Vorlaufige Mitteilung NUCLEAR REACTIONS 249Cf(n, F), E thermal; measured fission products radiochemically; deduced fission yields of 25 mass chains and one shielded nuclide (independent yields), nubar, division of nuclear charge consistent with the equal charge displacement hypothesis characteristic of low-energy fission.
doi: 10.1002/hlca.19690520805
1969VO14 J.Inorg.Nucl.Chem. 31, 3357 (1969) H.R.von Gunten, K.F.Flynn, L.E.Glendenin Independent Yields of 82Br, 86Rb, 136Cs and 150Pm in Spontaneous Fission of 252Cf RADIOACTIVITY, Fission 252Cf; measured fission yields; deduced charge distribution.
doi: 10.1016/0022-1902(69)80318-0
1969VO24 Actinides Rev. 1, 275 (1969) Distribution of Mass in Spontaneous and Neutron-Induced Fission NUCLEAR STRUCTURE, Fission 238U(SF); calculated, reviewed T1/2, mass distributions. 252Cf(SF); calculated, reviewed mass distributions. NUCLEAR REACTIONS 237Np, 241Am(n, F), E=reactor spectrum; 232Th, 235,238U(n, F), E ≤ 14 MeV; calculated, reviewed σ.
1967VO04 J.Inorg.Nucl.Chem. 29, 2826 (1967) H.R.Von Gunten, A.Wyttenbach, H.Dulakas Half-Life of 210Pb (RaD) NUCLEAR STRUCTURE 210Pb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(67)80026-5
1967VO08 Radiochim.Acta 8, 112 (1967) Absolute Fission-Yields of 99Mo and 139Ba in the Thermal Neutron Fission of 235U NUCLEAR REACTIONS, Fission 235U(n, F), E=thermal; measured 99Mo, 139Ba fission yields. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23562. 1967VO11 Phys.Rev. 161, 1192 (1967) H.R.Von Gunten, K.F.Flynn, L.E.Glendenin Distribution Of Mass And Charge In Fission Of 245Cm NUCLEAR REACTIONS 245Cm(n, f), E=0.0253 eV; measured products, 143Ce, 141Ce, 140Ba, 137Cs, 133I, 131I, 132Te, 129Te, 129Sb, 127Sb, 125Sb, 125Sn, 123Sn, 121Sn, 115Cd, 113Ag, 111Ag, 112Pd, 109Pd, 106Ru, 105Ru, 103Ru, 99Mo, 97Zr, 95Zr, 91Y, 90Sr, 89Sr, 83Br, 77As, 136Cs, 86Rb, 144Ce, 147Nd, 147Pm, 149Pm, 151Pm, 153Sm, 156Eu; deduced yields. Data were imported from EXFOR entry 13230.
doi: 10.1103/PhysRev.161.1192
1964WY01 Radiochim.Acta 3, 118 (1964) A.Wyttenbach, H.R.von Gunten, H.Dulakas Fission of 232Th by Reactor Neutrons: Fission Yields of some Mass-Chains NUCLEAR REACTIONS 232Th(n, F)90Sr/131I/137Cs/140Ba/141Ce/144Ce, E ∼ 2 MeV; measured fission products; deduced cumulative fission yields.
doi: 10.1524/ract.1964.3.3.118
1963VO02 Nucl.-Med. (Stuttgart) 3, 417 (1963) H.R.von Gunten, W.Scherle, H.Hugli Die Herstellung von Y90 fur Therapeutische Anwendungen
Back to query form |