NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = P.J.Karol Found 31 matches. 2016KA49 Pure Appl.Chem. 88, 139 (2016) P.J.Karol, R.C.Barber, B.M.Sherrill, E.Vardaci, T.Yamazaki Discovery of the elements with atomic numbers Z = 113, 115 and 117 (IUPAC Technical Report) COMPILATION 282Nh, 287,288,289Mc, 293,294Ts(α); compiled, experimental nuclear reaction and decay data.
doi: 10.1515/pac-2015-0502
2016KA50 Pure Appl.Chem. 88, 155 (2016) P.J.Karol, R.C.Barber, B.M.Sherrill, E.Vardaci, T.Yamazaki Discovery of the element with atomic number Z = 118 completing the 7th row of the periodic table (IUPAC Technical Report) COMPILATION 294Og, 290Lv, 286Fl(α); compiled, experimental nuclear reaction and decay data.
doi: 10.1515/pac-2015-0502
2011BA54 Pure Appl.Chem. 83, 1485 (2011) R.C.Barber, P.J.Karol, H.Nakahara, E.Vardaci, E.W.Vogt Discovery of the elements with atomic numbers greater than or equal to 113 (IUPAC Technical Report) COMPILATION 291Lv, 287Fl, 283Cn(α); compiled, experimental nuclear reaction and decay data.
doi: 10.1351/PAC-REP-10-05-01
2009BA62 Pure Appl.Chem. 81, 1331 (2009) R.C.Barber, H.W.Gaggeler, P.J.Karol, H.Nakahara, E.Vardaci, E.Vogt Discovery of the element with atomic number 112 (IUPAC Technical Report) COMPILATION 277Cn(α); compiled, experimental nuclear reaction and decay data.
doi: 10.1351/PAC-REP-08-03-05
2003KA71 Pure Appl.Chem. 75, 1601 (2003) P.J.Karol, H.Nakahara, B.W.Petley, E.Vogt On the claims for discovery of elements 110, 111, 112, 114, 116, and 118 (IUPAC Technical Report) NUCLEAR STRUCTURE Z=110-112; Z=114; Z=116; Z=118; compiled, analyzed priority claims for element discovery.
doi: 10.1351/pac200375101601
2001KA20 Nucl.Phys. A686, 109 (2001) M.Kaplan, C.J.Copi, P.A.DeYoung, G.J.Gilfoyle, P.J.Karol, D.J.Moses, W.E.Parker, K.E.E.Rehm, J.Sarafa, E.Vardaci Studies of Light Charged Particle Emission from Fission and ER Reactions in the System 344 MeV 28Si + 121Sb → 149Tb(E* = 240 MeV) NUCLEAR REACTIONS 121Sb(28Si, X), E=344 MeV; measured proton and α spectra in coincidence with fission fragments and evaporation residues; deduced reaction mechanism features. Comparison with statistical model predictions.
doi: 10.1016/S0375-9474(00)00573-X
2001KA70 Pure Appl.Chem. 73, 959 (2001) P.J.Karol, H.Nakahara, B.W.Petley, E.Vogt On the discovery of the elements 110-112 (IUPAC Technical Report) NUCLEAR STRUCTURE Z=110-112; compiled, analyzed priority claims for element discovery.
doi: 10.1351/pac200173060959
2001MI12 Nucl.Phys. A686, 525 (2001) Z.Milosevich, E.Vardaci, P.A.DeYoung, C.M.Brown, M.Kaplan, J.P.Whitfield, D.Peterson, C.Dykstra, M.Barton, P.J.Karol, M.A.McMahan Small Angle Particle-Particle Correlation Measurements in the Reactions 280 MeV 40Ar + 27Al and 670 MeV 55Mn + 12C NUCLEAR REACTIONS 27Al(40Ar, X), E=280 MeV; 12C(55Mn, X), E=670 MeV; measured pp-, pd-, pα-, dd-, dα-, αα-coin, relative momentum distributions, correlation functions; deduced role of compound nucleus spin distribution. Comparison with statistical model.
doi: 10.1016/S0375-9474(00)00569-8
2000BR20 Phys.Rev. C61, 054611 (2000) C.M.Brown, Z.Milosevich, M.Kaplan, E.Vardaci, P.A.DeYoung, J.P.Whitfield, D.Peterson, C.Dykstra, P.J.Karol, M.A.McMahan Light-Charged-Particle Emission in the Matched Reactions 280 MeV 40Ar + 27Al and 670 MeV 55Mn + 12C: Coincidence results NUCLEAR REACTIONS 27Al(40Ar, X), E=280 MeV; 12C(55Mn, X), E=670 MeV; measured exclusive light particle spectra, angular distributions, multiplicities, coincidence cross section ratios. Comparison with statistical model calculations.
doi: 10.1103/PhysRevC.61.054611
1999BR48 Phys.Rev. C60, 064612 (1999) C.M.Brown, Z.Milosevich, M.Kaplan, E.Vardaci, P.DeYoung, J.P.Whitfield, D.Peterson, C.Dykstra, P.J.Karol, M.A.McMahan Light Charged Particle Emission in the Matched Reactions 280 MeV 40Ar + 27Al and 670 MeV 55Mn + 12C: Inclusive studies NUCLEAR REACTIONS 27Al(40Ar, X), E=280 MeV; 12C(55Mn, X), E=670 MeV; measured light charged particles energy spectra, σ(θ), multiplicities. Comparison with statistical model calculations.
doi: 10.1103/PhysRevC.60.064612
1993KO16 Phys.Rev. C48, 236 (1993) Deep Spallation of Medium Mass Isotopes by Protons NUCLEAR REACTIONS 89Y, 92,96,100Mo, 130Te(p, X)43Sc/44Sc/44mSc/46Sc/47Sc/48Sc, E=0.8 GeV; measured residuals production σ; deduced mass 47 isobaric yield curves. Deep spallation.
doi: 10.1103/PhysRevC.48.236
1992KA36 Phys.Rev. C46, 1988 (1992) Transparency in High-Energy Nuclear Collisions NUCLEAR REACTIONS 40Ca(p, p), E > 40 MeV; 12C(12C, 12C), E > 50 MeV; calculated average reaction transparency. 208Pb, 12C(12C, X), 40Ca(40Ca, X), 208Pb(208Pb, X), E not given; calculated reaction σ, transparency. Sharp cut off models.
doi: 10.1103/PhysRevC.46.1988
1991KA02 Phys.Rev. C43, 908 (1991) Unified Multifragmentation-Evaporation Nuclear Reaction Models NUCLEAR REACTIONS, ICPND 89Y, 92,96,100Mo, 130Te(p, X), E=0.8 GeV; measured yields of 43,44,47,48Sc; deduced mass yield curves. Activation technique.
doi: 10.1103/PhysRevC.43.908
1989SH39 Radiochim.Acta 46, 1 (1989) S.Shibata, M.J.Tobin, P.J.Karol Absolute γ-Ray Abundance of 87Zr RADIOACTIVITY 87Zr [from 89Y, 92,96,100Mo(p, X), E=500, 800 MeV]; measured absolute γ-ray abundance. Radiochemical method. NUCLEAR REACTIONS, ICPND 89Y, 92,96,100Mo(p, X), E=500, 800 MeV; measured isotopic yield distributions for 85-89Zr. Radiochemical method.
doi: 10.1524/ract.1989.46.1.1
1989TO07 Phys.Rev. C39, 2330 (1989) Isobaric Yield Curves at A = 72 from the Spallation of Medium Mass Isotopes by Intermediate Energy Protons NUCLEAR REACTIONS 89Y, 92,96,100Mo, 130Te(p, X), E=800 MeV; measured production σ for 65Ga-82Br; deduced A=72 isobar yields.
doi: 10.1103/PhysRevC.39.2330
1988SM07 Phys.Rev. C38, 210 (1988) A.R.Smith, J.C.Hill, J.A.Winger, P.J.Karol Cross Section for the 12C(139La, X)11C Reaction at Relativistic Energies NUCLEAR REACTIONS 12C(139La, X), 11C, E=1.29 GeV/nucleon; measured residual production σ, relativistic energies. Linear transport model, other data analyzed.
doi: 10.1103/PhysRevC.38.210
1988TO08 Phys.Rev. C38, 267 (1988) Unexpected Recoil Systematics of Intermediate Energy Spallation Products NUCLEAR REACTIONS 89Y(p, X)65Ga/66Ga/67Ge/67Ga/68Ga/69As/69Ge/70As/70Ga/71As/72As/72Ga/73Ga/74Br/74As/74Ga/75Br/75Ge/76Br/76As/77Br/77Ge/78Br/80Br/82Br, E=800 MeV; measured residual production, recoil properties. Activation technique.
doi: 10.1103/PhysRevC.38.267
1983KA22 Can.J.Chem. 61, 750 (1983) Nuclear Mean Free Paths and Transparency at Intermediate Energies NUCLEAR REACTIONS Be, B, C, O, Al, Fe, Cu, Ge, Sn, Pb(p, X), E=0.53 GeV/nucleon; C, 4He, 2H(p, X), 2H, 4He(d, X), C, 4He(α, X), E=2.1 GeV/nucleon; C(12C, X), C(α, X), E=2.1 GeV/nucleon; C(12C, X), C(α, X), 4He(α, X), (d, X), (p, X), E=0.87 GeV/nucleon; calculated σ(reaction).
doi: 10.1139/v83-139
1983KA27 Phys.Rev. C28, 1850 (1983) P.J.Karol, M.J.Tobin, S.Shibata Estimation of Neutron-Induced Spallation Yields of Krypton Isotopes NUCLEAR REACTIONS 89Y(n, X), E=0.2-3 GeV; calculated cumulative yields for 78,80,82,83,84,86Kr. Rb, Sr, Y, Zr(n, X), (p, X), E not given; calculated spallation yield ratios for 78,80,82,83,84,86Kr. Data systematics input.
doi: 10.1103/PhysRevC.28.1850
1983SH27 Can.J.Chem. 61, 754 (1983) Identification of 20-Minute Zr-84 RADIOACTIVITY 84Zr(β+), (EC) [from 92,96,100Mo(p, X), E=500, 800 MeV]; measured γ-spectra, 112.5 keV γ-ray abundance; deduced T1/2. NUCLEAR REACTIONS 96,100Mo(p, X), E=800 MeV; 92Mo(p, X), E=500, 800 MeV; measured γ-spectra; deduced evidence for 84Zr, Zr isotope production relative σ vs N/Z. Enriched targets.
doi: 10.1139/v83-140
1981KA05 Phys.Rev. C23, 415 (1981) Relevance of Final-State Nucleon-Nucleon Charge Exchange in Inclusive (π, πN) Reactions NUCLEAR REACTIONS 12C(π+, π+n), (π-, π-n), E=50-400 MeV; 25Mg(π+, π+p), (π-, π-p), E=100, 300 MeV; 197Au(π+, π+n), (π-, π-n), E=50-300 MeV; calculated σ(π+)/σ(π-).One-step quasifree intranuclear cascade model, final state interactions.
doi: 10.1103/PhysRevC.23.415
1977KU16 Phys.Rev. C16, 1984 (1977) Isobaric Yield Curves at A = 72 from the Spallation of Molybdenum Isotopes by High-Energy Alpha Particles NUCLEAR REACTIONS 92,96,100Mo(α, X), E=720 MeV; measured σ(A), A=65-76; deduced yield curves at A=72. Enriched targets, Ge(Li) detectors.
doi: 10.1103/PhysRevC.16.1984
1976CH18 Phys.Rev. C14, 1068 (1976) Y.Y.Chu, E.-M.Franz, G.Friedlander, P.J.Karol Interaction of 28-GeV Protons with Thorium: Study of Charge Dispersions and Mass Yields NUCLEAR REACTIONS 232Th(p, F), E=28 GeV; measured σ(A, Z), A=43-173; deduced charge dispersion curve.
doi: 10.1103/PhysRevC.14.1068
1975KA07 Phys.Rev. C11, 1203 (1975) Nucleus-Nucleus Reaction Cross Sections at High Energies: Soft-Spheres Model NUCLEAR REACTIONS 27Al, 64Cu, 208Pb, 238U(p, X), E=20 GeV; 40Ca, 59Ni, 119Sn, 208Pb(π-, X), E=2 GeV; 64Cu, 208Pb(p-bar, X), (K-, X), E=13.3 GeV; 12C, 32S, 64Cu, 208Pb(16O, X), E=34 GeV; calculated σ.
doi: 10.1103/PhysRevC.11.1203
1974KA22 Phys.Rev. C10, 150 (1974) Spallation of Copper by High-Energy Alpha Particles NUCLEAR REACTIONS 63,65Cu(α, X), E=410, 720 MeV; measured yields for A=7-65 spallation products.
doi: 10.1103/PhysRevC.10.150
1973KA19 Phys.Lett. 44B, 459 (1973) P.J.Karol, A.A.Caretto, Jr., R.L.Klobuchar, D.M.Montgomery, R.A.Williams, M.V.Yester Cross Sections for (π, πn) Reactions on 14N and 19F at the (3/2, 3/2) Resonance RADIOACTIVITY 11C, 13N, 18F; measured γγ-coin. NUCLEAR REACTIONS 14N, 19F(π+, X), 19F(π-, π-n), E=190 MeV; measured σ production of 13N, 18F.
doi: 10.1016/0370-2693(73)90334-1
1973YE02 Phys.Lett. 45B, 327 (1973) M.V.Yester, A.A.Caretto, Jr., M.Kaplan, P.J.Karol, R.L.Klobuchar Cross Section of (π+, π+n+π0p) Reaction on 12C at the (3/2, 3/2) Resonance NUCLEAR REACTIONS 12C(π+, X); measured σ.
doi: 10.1016/0370-2693(73)90046-4
1971CH48 Phys.Rev. C4, 2202 (1971) Y.Y.Chu, E.M.Franz, G.Friedlander, P.J.Karol Interaction of 28-GeV Protons with Uranium: Charge and Mass Distribution of Rare-Earth Products NUCLEAR REACTIONS U(p, X), E=28 GeV; measured cumulative, independent yields of 50 rare-earth nuclides.
doi: 10.1103/PhysRevC.4.2202
1971CH57 Inorg.Nucl.Chem.Lett. 7, 1205 (1971) The Half-Life of 172Hf RADIOACTIVITY 172Hf; measured T1/2.
doi: 10.1016/0020-1650(71)80067-3
1970KA23 J.Inorg.Nucl.Chem. 32, 2817 (1970) Half-Life Determinations for 169,170,171Lu, 166Yb, 165,166,167Tm, and 160Er RADIOACTIVITY 169,170,171Lu, 166Yb, 165,166,167Tm, 160Er; measured T1/2.
doi: 10.1016/0022-1902(70)80343-8
1968KA36 Phys.Rev. 166, 1089 (1968) Nuclear-Structure Effects in Simple High-Energy Spallation Reactions NUCLEAR REACTIONS 50Cr(p, 2n2p), 50Cr(p, 2np), 50Cr(p, 2p), 50Cr(p, n2p), 58Ni(p, 2n2p), 58Ni(p, 2np), 58Ni(p, 2p), 58Ni(p, 4n6p), 58Ni(p, 5n5p), 58Ni(p, 5n6p), 58Ni(p, 6n5p), 58Ni(p, 6n6p), 58Ni(p, n2p), 58Ni(p, np), 64Zn(p, 2n2p), 64Zn(p, 2np), 64Zn(p, 3n2p), 64Zn(p, n2p), 64Zn(p, np), E=370 MeV; measured products, 57Ni, Eπ, Iπ; deduced σ, σ(E). Data were imported from EXFOR entry C0274.
doi: 10.1103/PhysRev.166.1089
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