NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = J.Kantele Found 83 matches. 1994LH01 Phys.Rev. C49, 1379 (1994) G.Lhersonneau, B.Pfeiffer, K.-L.Kratz, T.Enqvist, P.P.Jauho, A.Jokinen, J.Kantele, M.Leino, J.M.Parmonen, H.Penttila, J.Aysto, and the ISOLDE Collaboration Evolution of Deformation in the Neutron-Rich Zr Region from Excited Intruder State to the Ground State RADIOACTIVITY 99,98Y(β-); measured Eγ, Iγ, I(ce), γγ(t), (γ)(e)(t). 98,99Zr levels deduced J, π, intruder states, shape coexistence, ICC, 0+ → 0+ transition features, B(λ). On-line mass separation.
doi: 10.1103/PhysRevC.49.1379
1992KU01 Phys.Rev. C45, 640 (1992) J.Kumpulainen, R.Julin, J.Kantele, A.Passoja, W.H.Trzaska, E.Verho, J.Vaaramaki, D.Cutoiu, M.Ivascu Systematic Study of Low-Spin States in Even Cd Nuclei NUCLEAR REACTIONS 106,108,110,112,116Cd(p, p'), E=7-9 MeV; 107,109Ag(p, 2n), E=12.3-17.4 MeV; 108,110Pd(α, 2n), E=17-20MeV; measured Eγ, Iγ, γγ-, pγ-coin, γ(θ). 106,108,110,112,116Cd deduced levels, J, π, ICC. Enriched targets, Ge, Si(Li) detectors. RADIOACTIVITY 106,108,110In(EC), (β+); measured Eγ, Eβ. 106,108,110Cd deduced levels J, π, ICC, Ge, Si(Li) detectors.
doi: 10.1103/PhysRevC.45.640
1991PA17 Nucl.Instrum.Methods Phys.Res. A306, 504 (1991) J.M.Parmonen, Z.Janas, W.H.Trzaska, J.Aysto, J.Kantele, P.P.Jauho, A.Jokinen, H.Penttila Electron-Transporter Spectrometer for On-Line Isotope Separator RADIOACTIVITY 115Rh, 115m,115Pd, 115m,115Ag, 115,115mCd, 115mIn; measured (ce)(β-)-, (ce)(K X-ray)-coin. On-Line isotope separator, electron transport spectrometer.
doi: 10.1016/0168-9002(91)90044-Q
1990KU01 Z.Phys. A335, 109 (1990) J.Kumpulainen, R.Julin, J.Kantele, A.Passoja, W.H.Trzaska, E.Verho, J.Vaaramaki New Features in Systematics of Low-Spin States in Even 106-120Cd NUCLEAR REACTIONS 106,108,110Cd(p, p'), E not given; measured pγ-, γγ-coin, γ(θ), I(ce). 107,109Ag(p, 2n), E not given; measured not given. 106,108,110,112,116,118,120Cd deduced levels, J, π, absolute transition rates. Other data input. RADIOACTIVITY 106,108,110In; measured γγ-coin, γ(θ), I(ce). 106,108,110Cd deduced levels, J, π, γ-branching ratios.
1990TR01 Z.Phys. A335, 475 (1990) W.H.Trzaska, J.Kantele, R.Julin, J.Kumpulainen, P.Van Duppen, M.Huyse, J.Wauters Comparison of Experimental and Calculated K/L Ratios of E0 Transitions in Some Heavy Nuclei RADIOACTIVITY 154Gd, 192,194,196,198,202,204,206,208Pb, 208Po; compiled measured, calculated I(ce) ratios; deduced no major differences.
1989ES01 Phys.Rev. C39, 76 (1989) R.Estep, R.K.Sheline, D.J.Decman, E.A.Henry, L.G.Mann, R.A.Meyer, W.Stoffl, L.E.Ussery, J.Kantele Levels in 112Pd and 102Mo NUCLEAR REACTIONS 110Pd, 100Mo(t, pγ), E=16 MeV; measured pγ-, pγγ-coin. 102Mo, 112Pd deduced levels, J, π, band structure.
doi: 10.1103/PhysRevC.39.76
1989KA07 Nucl.Instrum.Methods Phys.Res. A275, 149 (1989) A Simplified Method for Computing K Internal-Conversion Coefficients for E1, E2, E3, M1, M2, and M3 Transitions from Tabulated Values NUCLEAR STRUCTURE Z=30-90; analyzed data; deduced K-shell ICC.
doi: 10.1016/0168-9002(89)90345-8
1989TR14 Phys.Rev. C40, 1520 (1989) W.H.Trzaska, R.Julin, J.Kantele, J.Kumpulainen Solution of Controversy Over 1583-keV Levels in 204Pb NUCLEAR REACTIONS 204Pb(p, p'), E=12.1-12.7 MeV; measured I(ce), Eγ, Iγ. 204Pb deduced levels, J, π, 0+ level configurations. Other data input.
doi: 10.1103/PhysRevC.40.1520
1988KA22 Nucl.Instrum.Methods Phys.Res. A271, 625 (1988) A Quick Method of Obtaining the Electronic Factors (Omega(K)), (Omega(L(I))) and (Omega(L(II))) for E0 Transitions NUCLEAR STRUCTURE Z=30-100; calculated E0 transition electronic factors.
doi: 10.1016/0168-9002(88)90332-4
1987ES01 Phys.Rev. C35, 1485 (1987) R.J.Estep, R.K.Sheline, D.J.Decman, E.A.Henry, L.G.Mann, R.A.Meyer, W.Stoffl, L.E.Ussery, J.Kantele Measurement of E0 Transitions in Neutron-Rich Nuclei near A = 100 NUCLEAR REACTIONS 98,100Mo, 104Ru, 106,108,110Pd(t, p), E=16 MeV; measured γp-, (ce)p-coin. 100,102Mo, 106Ru, 108,110,112Pd deduced levels, T1/2, E0 transitions, E0/E2 branching ratios.
doi: 10.1103/PhysRevC.35.1485
1987JU06 Phys.Rev. C36, 1129 (1987) R.Julin, J.Kantele, J.Kumpulainen, M.Luontama, A.Passoja, W.Trzaska, E.Verho, J.Blomqvist E0 Study of O+ States near 5 MeV in 208Pb NUCLEAR REACTIONS 208Pb(p, p'), E=17.3 MeV; 207Pb(d, p), E=10 MeV; measured I(ce), pγ-coin. 208Pb deduced levels, J, π, γ-multipolarity.
doi: 10.1103/PhysRevC.36.1129
1987YA13 Phys.Rev. C36, 2143 (1987) S.W.Yates, L.G.Mann, E.A.Henry, D.J.Decman, R.A.Meyer, R.J.Estep, R.Julin, A.Passoja, J.Kantele, W.Trzaska E0 Decay of 0+ States in 146Gd: Search for two-phonon octupole excitations NUCLEAR REACTIONS 144Sm(α, 2n), E=25.5 MeV; 144Sm(3He, n), E=15-20 MeV; measured Eγ, Iγ, I(ce). 146Gd deduced levels, J, π, E0 transitions.
doi: 10.1103/PhysRevC.36.2143
1986KA07 Phys.Lett. 171B, 151 (1986) J.Kantele, M.Luontama, W.Trzaska, R.Julin, A.Passoja, K.Heyde E0 Transitions in 202,204Pb and Intruder-State Systematics of Even-Even Lead Isotopes NUCLEAR REACTIONS 203,205Tl(p, 2n), E=14.5 MeV; measured Eγ, Iγ, I(ce), γγ-coin. 202,204Pb deduced levels, I(ce) branching ratios, configuration, J, π, T1/2, upper limits.
doi: 10.1016/0370-2693(86)91523-6
1986LU06 Z.Phys. A324, 317 (1986) M.Luontama, R.Julin, J.Kantele, A.Passoja, W.Trzaska, A.Backlin, N.-G.Jonsson, L.Westerberg Electromagnetic Properties of Low-Spin States in 102,104Pd NUCLEAR REACTIONS 102Pd(p, p'), (p, 2n), E=6-15 MeV; measured p'γ-coin, I(ce), γ(t). 102,104Pd(16O, 16O'), E=44 MeV; measured Eγ, Iγ following Coulomb excitation. 102,104Pd levels deduced B(λ), relative σ.
1986PA14 J.Phys.(London) G12, 1047 (1986) A.Passoja, J.Kantele, M.Luontama, R.Julin, E.Hammaren, P.O.Lipas, P.Toivonen Electromagnetic Decay of 02+ and O3+ States in the N = 88-90 Nuclei of 150,152Sm RADIOACTIVITY 152m,150mEu(EC), (β+), (β-) [from 150Sm(p, n), E=9.5 MeV; 151Eu(n, γ), E=thermal]; measured Iγ, Eγ, I(ce), I(ce)(X-ray)-coin. 150,152Sm deduced levels, J, π, B(λ), E0 strength parameter. Enriched targets, Ge(Li) detectors, magnetic plus Si-Li conversion electron spectrometer. Interacting boson model.
doi: 10.1088/0305-4616/12/10/013
1985PA07 Nucl.Phys. A438, 413 (1985) A.Passoja, R.Julin, J.Kantele, J.Kumpulainen, M.Luontama, W.Trzaska Electromagnetic Decay of Excited 0+ States in 64,66,68Zn RADIOACTIVITY 64Ga(β+), (EC) [from 64Zn(p, n), E=14 MeV]; measured Iγ, Eγ, I(ce). Ge(Li) detectors, magnetic plus Si-Li conversion electron, internal pair spectrometers, enriched targets. NUCLEAR REACTIONS 64,66,68Zn(p, p'γ), E=5.9-6.9 MeV; measured Iγ, Eγ, I(ce), internal pair production spectrum, γp-coin, γp(t), (ce)p(t). 64,66,68Zn deduced levels, J, π, B(E0)/B(E2), E0 strength parameter.
doi: 10.1016/0375-9474(85)90383-5
1985PA15 Nucl.Phys. A441, 261 (1985) A.Passoja, R.Julin, J.Kantele, M.Luontama, M.Vergnes E0 Transitions in 70Ge and Shape-Coexistence Interpretation of Even-Mass Ge Isotopes NUCLEAR REACTIONS 70Ge(p, p'γ), E=6.9 MeV; measured Iγ, Eγ, I(ce), internal pair production spectrum, γp'-coin, (ce)p(t). 70Ge deduced levels, J, π, B(E0)/B(E2), E0 strength parameter (ρ)2. Ge(Li) detectors, magnetic plus Si-Li conversion electron, internal pair spectrometers, enriched targets.
doi: 10.1016/0375-9474(85)90033-8
1984DE17 Nucl.Instrum.Methods 219, 523 (1984) D.J.Decman, E.A.Henry, J.Kantele, L.G.Mann, W.Stoffl, R.J.Estep, L.E.Ussery Electron Spectroscopy in Coincidence with Protons from the (t, p) Reaction NUCLEAR REACTIONS 98Mo, 204Pb(t, p), E=16 MeV; measured σ(Ep), (ce)p-coin. 98Mo(t, p), (t, t'), (t, 2n), 100Mo(t, p), (t, 2n), E=16 MeV; measured I(ce), (ce)p-coin. Electron spectrometer in coincidence with thin annular Si(Au) proton detector.
doi: 10.1016/0167-5087(84)90225-4
1984KA10 Phys.Rev. C29, 1693 (1984) J.Kantele, W.Stoffl, L.E.Ussery, D.J.Decman, E.A.Henry, R.J.Estep, R.W.Hoff, L.G.Mann Reinvestigation of the Gamma Branch from the 238U Shape Isomer NUCLEAR REACTIONS, ICPND 238U(d, np), E=18.1 MeV; measured Eγ, Iγ; deduced (isomeric/ground state) σ. 238U deduced shape isomer SF, conversion decay characteristics, levels. RADIOACTIVITY 238mU(SF), (IT) [from 238U(d, np), E=18.1 MeV]; measured Eγ, Iγ; deduced isomer decay process relative probabilities.
doi: 10.1103/PhysRevC.29.1693
1984KA17 ATOMKI Kozlem. 26, 59 (1984) J.Kantele, W.Stoffl, L.E.Ussery, D.J.Decman, E.A.Henry, R.J.Estep, R.W.Hoff, L.G.Mann Gamma Branch from the 238U Shape Isomer NUCLEAR REACTIONS, ICPND 238U(d, np), E=18 MeV; measured γ spectra; deduced 238mU production σ. 238U deduced isomer decay characteristics, transitions. In-beam spectroscopy.
1983KA06 Nucl.Instrum.Methods 206, 403 (1983) J.Kantele, M.Luontama, W.Trzaska, A.Passoja Single-Detector Particle Identification in Conjunction with Coincidence Measurements NUCLEAR REACTIONS 152Sm(p, p'γ), (p, dγ), (p, tγ), E=17 MeV; measured Eγ, Iγ, pγ-, dγ-, tγ-coin; 152Sm(p, 2n), E=19 MeV; measured I(ce), (ce)p-coin. Thin Si(Au), NE 102A, cylindrical plastic scintillation detectors.
doi: 10.1016/0167-5087(83)90376-9
1983KA11 Phys.Rev.Lett. 51, 91 (1983) J.Kantele, W.Stoffl, L.E.Ussery, D.J.Decman, E.A.Henry, R.W.Hoff, L.G.Mann, G.L.Struble Observation of an E0 Isomeric Transition from the 238U Shape Isomer RADIOACTIVITY 238mU [from 238U(d, pn), E=18 MeV]; measured I(ce); deduced shape isomer E0 transition, J, π, T1/2 assignment consistency. Reevaluation of Iγ data, superconducting, solenoid type electron spectrometer.
doi: 10.1103/PhysRevLett.51.91
1983PA05 Phys.Lett. 124B, 157 (1983) A.Passoja, J.Kantele, M.Luontama, J.Kumpulainen, R.Julin, P.O.Lipas, P.Toivonen Disproof of the Alleged Two-Phonon Character of the O+2 State in 64Zn RADIOACTIVITY 64Ga(β+), (EC); measured I(ce). 64Zn deduced level. NUCLEAR REACTIONS 64Zn(p, p'), E=5.9-6.9 MeV; measured Eγ, Iγ, γp-coin. 64Zn deduced γ-branching, B(E2), B(E0)/B(E2), monopole transition strengths, 0+ level T1/2. Discussed inadequacy of existing nuclear models.
doi: 10.1016/0370-2693(83)91425-9
1983PA09 Phys.Scr. T5, 145 (1983) A.Passoja, J.Kantele, M.Luontama, J.Kumpulainen, R.Julin Search for the Two-Phonon 0+ Strength in 64Zn NUCLEAR REACTIONS 64Zn(p, p'), E=6.9 MeV; measured I(ce), γp-coin, pair spectrum. 64Zn deduced 0+2 state T1/2, nonphonon character, B(E2), E0 transition strength.
doi: 10.1088/0031-8949/1983/T5/025
1983PA10 Phys.Scr. T5, 147 (1983) A.Passoja, M.Vergnes, J.Kantele, M.Luontama Electric Monopole Strengths in Even-Mass Ge and Se Isotopes RADIOACTIVITY 74,76Br(β+), (EC) [from 74,76Se(p, n), E=9 MeV]; measured Eγ, Iγ, I(ce). 74,76Se levels deduced I(K X-ray)/Iγ, T1/2, E0/E2 branching ratios. NUCLEAR REACTIONS 70Ge(p, p'), E=6.9 MeV; measured γ(ce)(t). 72Ge(t, p), E not given; measured Eγ, Iγ, I(ce). 74Se(p, p'), E=5.9 MeV; measured γ-spectra centroid shift, (ce)γ(t). 70Ge, 74Se deduced level T1/2, B(E2) ratios. 74Ga deduced level T1/2, I(K X-ray)/Iγ, B(E2) ratios.
doi: 10.1088/0031-8949/1983/T5/026
1983TR11 Nucl.Instrum.Methods 212, 221 (1983) Semiconductor Telescope Spectrometer for Beta-Ray Spectra RADIOACTIVITY 93Ru(β+), (EC); measured β+ endpoint energy; deduced agreement with mass systematics. Semiconductor telescope spectrometer.
doi: 10.1016/0167-5087(83)90695-6
1982KA07 Nucl.Instrum.Methods 193, 495 (1982) J.Kantele, E.Hammaren, D.G.Burke, J.C.Waddington A Test of the Feasibility of γp-Coincidence Techniques in Conjunction with the (t, pγ) Reaction NUCLEAR REACTIONS 150Sm(t, pγ), E=15 MeV; measured Eγ, Iγ, pγ-coin. Ge(Li), Si-Au detectors.
doi: 10.1016/0029-554X(82)90241-5
1982KA22 Nucl.Instrum.Methods 200, 253 (1982) J.Kantele, R.Julin, M.Luontama, A.Passoja A Method for Centroid-Shift Time Measurements with Magnetic Plus Si(Li) Combination Conversion-Electron Spectrometer NUCLEAR REACTIONS 144Sm(3He, n), E=15.3 MeV; 62Ni, 92Zr(p, p'), E=7.08 MeV; measured I(ce), (ce)(t). 146Gd, 92Zr level deduced T1/2. Centroid timing method, magnetic plus Si-Li combination electron spectrometer, composite Ni, Zr target.
doi: 10.1016/0167-5087(82)90439-2
1981BA05 Nucl.Phys. A351, 490 (1981) A.Backlin, N.G.Jonsson, R.Julin, J.Kantele, M.Luontama, A.Passoja, T.Poikolainen 0+ States and E0 and E2 Transition Rates in Even Sn Nuclei NUCLEAR REACTIONS 112,114,116,118,120,122,124Sn(16O, 16O'), E=48 MeV; measured Eγ, Iγ, γγ-coin, Coulomb excitation; 112,114,116,118,120,122,124Sn(p, p'γ), E not given; measured Iγ, Eγ, I(ce), γp'-, (ce)p'-coin, γp(t), (ce)p(t), Coulomb excitation; 124Sn(p, 2n), E not given; measured Eγ, Iγ, I(ce). 112,114,116,118,120,122,124Sn deduced levels, J, π, ICC, B(E0), B(E2), sign of matrix product. RADIOACTIVITY 116,118,120Sb; measured Iγ, I(ce), γγ(θ); 116,118In; measured Iγ, I(ce), βγ-coin. 116,118Sn deduced levels, J, π, B(λ). Ge(Li), annular NaI detectors, magnetic spectrometers, enriched targets.
doi: 10.1016/0375-9474(81)90184-6
1981CE06 Phys.Scr. 24, 930 (1981) A.Celler, M.Luontama, J.Kantele, J.Zylicz Cross Sections of 232Th(p, xn+yp) Reactions at E(p) = 6.8 to 20.2 MeV NUCLEAR REACTIONS 232Th(p, xnyp), E=6.8-20.2 MeV; measured σ(E) for x=1, 2, 3, y=0, 1; deduced reaction mechanism. In-beam spectroscopy, activation technique, Ge(Li), hyperpure Ge detectors. Statistical, preequilibrium models.
doi: 10.1088/0031-8949/24/6/003
1981JO03 Nucl.Phys. A371, 333 (1981) N.-G.Jonsson, A.Backlin, J.Kantele, R.Julin, M.Luontama, A.Passoja Collective States in Even Sn Nuclei NUCLEAR REACTIONS 112,114,116,118,120,122,124Sn(16O, 16O'γ), E=48 MeV; measured Eγ, Iγ, γγ-coin. 112,114,116,118,120,122,124Sn(p, p'γ), E=6-8 MeV; measured Eγ, Iγ. 112,114,116,118,120,122,124Sn deduced B(E2), B(E3), B(E1). Ge(Li), NaI detectors. Enriched targets. RADIOACTIVITY 116Sb; measured Iγ. 116Sn deduced B(E2) ratio.
doi: 10.1016/0375-9474(81)90071-3
1981JU03 Z.Phys. A303, 147 (1981) R.Julin, J.Kantele, M.Luontama, A.Passoja Decay of 0+2 States in 88,92,94Zr and E0 Systematics of Zr Isotopes RADIOACTIVITY 88Zr [from 89Y(p, 2n), E=17.2 MeV]; measured I(ce), Eγ, Iγ. 88Zr levels deduced B(E0)/B(E2). NUCLEAR REACTIONS 92Zr(p, p'), E=7.08 MeV; 94Zr(p, p'), E=8.11 MeV; measured I(ce), Eγ, Iγ, T1/2 for 0+ states; deduced monopole strengths. 92,94Zr levels deduced B(E0)/B(E2), configurations. Si-Li detector plus magnetic lens electron spectrometer.
doi: 10.1007/BF01420272
1981PA10 Nucl.Phys. A363, 399 (1981) A.Passoja, R.Julin, J.Kantele, M.Luontama High-Resolution Study of E0 Internal Pair Decay of Excited 0+ States in 58,60,62Ni NUCLEAR REACTIONS 58,60,62Ni(p, p'γ), E=6.9 MeV; measured Iγ, Eγ, I(ce), internal pair production spectrum, γp'-coin, γp'(t). 58,60,62Ni deduced levels, J, π, B(E0)/B(E2), E0 strength parameter. Ge(Li) detectors, magnetic plus Si(Li) conversion-electron, internal-pair spectrometers. Enriched targets.
doi: 10.1016/0375-9474(81)90265-7
1980JU04 Phys.Lett. B94, 123 (1980) R.Julin, J.Kantele, M.Lountama, A.Passoja, P.Kleinheinz, J.Blomqvist Electromagnetic Decay of the 0+2 State in the Doubly Closed Shell Nucleus 14664Gd82 NUCLEAR REACTIONS 144Sm(3He, n), E=14-27 MeV; measured I(ce), Eγ, Iγ, (ce)(3He)(t). 146Gd deduced level, T1/2, J, π, γ-multipolarity.
doi: 10.1016/0370-2693(80)90839-4
1980JU05 Z.Phys. A296, 315 (1980) R.Julin, J.Kantele, M.Luontama, A.Passoja, T.Poikolainen, A.Backlin, N.-G.Jonsson Decay Characteristics of 0+2 and 0+3 States in 112Cd and 114Cd RADIOACTIVITY 112Cd [from 111Cd(d, p), E=9 MeV; 112Cd(p, n)112In(β-decay)], 114Cd [from 113Cd(d, p), E=8 MeV]; measured Eγ, Iγ, I(ce), T1/2, γγ-, e-p-, γp-coin. 112,114Cd levels deduced B(E2), T1/2. NUCLEAR REACTIONS Cd(16O, 16O'), E=44 MeV; measured double Coulomb excitation σ. 112,114Cd levels deduced B(E2), T1/2. Metallic Cd target.
doi: 10.1007/BF01438525
1979KA01 Z.Phys. A289, 157 (1979) J.Kantele, R.Julin, M.Luontama, A.Passoja, T.Poikolainen, A.Backlin, N.-G.Jonsson Absolute E0 and E2 Transition Rates and Collective States in 116Sn NUCLEAR REACTIONS 116Sn(16O, 16O'), E=48 MeV; measured σ(Coulomb-excitation). 116Sn deduced absolute E0, E2 transition rates. Discussed deformed excited states.
doi: 10.1007/BF01435933
1979LU10 Nucl.Instrum.Methods 159, 339 (1979) M.Luontama, J.Kantele, R.Julin, A.Passoja, T.Poikolainen, M.Pylvanainen A Combination Intermediate-Image Magnetic Plus Si(Li) Electron Spectrometer for In-Beam Experiments NUCLEAR REACTIONS 116Sn(p, p'), E=7.9 MeV; measured p(ce)-coin spectra. 111Cd(d, p), E=9 MeV; measured I(ce), p(ce)-coin spectra. 112Cd level deduced T1/2. Magnetic lens plus Si(Li) combination in-beam β-spectrometer.
doi: 10.1016/0029-554X(79)90659-1
1978EL07 Nucl.Phys. A302, 125 (1978) C.Ellegaard, R.Julin, J.Kantele, M.Luontama, T.Poikolainen Half-Life of the Lowest 2p-1h State in 209Bi NUCLEAR REACTIONS 208Pb(d, nγ), E=6, 8, 10 MeV; measured Eγ, ce(t). 209Bi deduced levels, J, π, ICC, T1/2. Enriched target.
doi: 10.1016/0375-9474(78)90290-7
1978JO07 Nucl.Instrum.Methods 152, 485 (1978) N.-G.Jonsson, J.Kantele, A.Backlin A High-Efficiency Coincidence Method for Coulomb Excitation Studies of Weakly Populated Vibration-Like Levels NUCLEAR REACTIONS 112,114Cd(16O, 16O'γ), E=44 MeV; 118Sn(16O, 16O'γ), E=48 MeV; measured Coulomb excitation. 112,114Cd, 118Sn levels deduced B(E2).
doi: 10.1016/0029-554X(78)90050-2
1978JU02 Nucl.Instrum.Methods 152, 471 (1978) R.Julin, J.Kantele, M.Luontama, A.Passoja, T.Poikolainen A Walk-Free Centroid Method for Lifetime Measurements with Pulsed Beams NUCLEAR REACTIONS 116Sn(p, p'), E=6.93 MeV; 208Pb(d, p), E=10 MeV; measured particle spectrum, γ(t). 116Sn, 209Pb levels deduced T1/2.
doi: 10.1016/0029-554X(78)90048-4
1977KA17 Phys.Scr. 15, 202 (1977) Search for Superheavy Elements in Uranium Minerals Using K X-Ray Fluorescence Analysis RADIOACTIVITY Z=121-127; measured K X-ray fluorescence yields; deduced upper limit for concentration of Z=121-127 in U.
doi: 10.1088/0031-8949/15/3/007
1976BA32 Phys.Lett. 62B, 402 (1976) A.Backlin, W.Dietrich, R.Julin, J.Kantele, M.Luontama, L.Westerberg E0 Transitions in 114,116,118Sn RADIOACTIVITY 118Sb; measured I(ce). 118Sn level deduced B(E0)/B(E2). NUCLEAR REACTIONS 114,116,118Sn(p, p'), E=6.40-6.92 MeV; measured I(ce). 114,116Sn levels deduced B(E0)/B(E2).
doi: 10.1016/0370-2693(76)90668-7
1976JU03 Phys.Lett. 65B, 337 (1976) R.Julin, J.Kantele, M.Luontama, T.Poikolainen, V.Rahkonen Half-Lives of Two-Neutron-Hole 0+2 States in 206Pb and 208Po NUCLEAR REACTIONS 209Bi(p, 2n), E=14.8 MeV; measured γ(t). 208Po, 206Pb deduced levels, λ, T1/2.
doi: 10.1016/0370-2693(76)90236-7
1975KO02 Nucl.Phys. A240, 87 (1975) M.Kortelahti, A.Pakkanen, J.Kantele Electromagnetic Transition Rates in 208Pb RADIOACTIVITY 208Tl [from equilibrium product of 228Th]; measured Eγ, Iγ, γγ-, γγγ-coin. 208Pb deduced levels, γ-branching, B(M1), B(E2).
doi: 10.1016/0375-9474(75)90438-8
1975PA07 Z.Phys. A274, 127 (1975) A.Pakkanen, M.Kortelahti, H.Helppi, J.Kantele, T.Poikolainen, R.Komu Decay of 14.6 h 90Nb RADIOACTIVITY 90Nb [from 90Zr(p, n)]; measured Eγ, Iγ, γγ-coin; deduced log ft. 90Zr deduced levels, J, π, γ-branching. Ge(Li), anti-Compton detectors. Natural targets.
doi: 10.1007/BF01408464
1974RA31 Phys.Fenn. 9, 103 (1974) Decay of 0.30 s 64Co RADIOACTIVITY 64Co [from 64Ni(n, p), E=14-15 MeV]; measured Eγ, Iγ, βγ-coin, T1/2; deduced Q, J, π. 64Ni levels deduced transitions, γ-branching.
1973KA50 Nucl.Instrum.Methods 112, 501 (1973) Corrections for Positon Annihilation in Flight in Nuclear Spectrometry RADIOACTIVITY 62Cu(β+) [from 63Cu(n, 2n), E=14 MeV]; measured positions total absolute annihilation in flight probabilities.
doi: 10.1016/0029-554X(73)90169-9
1972KA21 Phys.Lett. 39B, 625 (1972) Mass Number Dependence of Activation Capture Cross Sections for 14 MeV Neutrons NUCLEAR REACTIONS 51V, 81Br, 103Rh, 127I, 154Sm, 160Gd, 165Ho, 170Er(n, γ), E=14.5 MeV; measured activation σ.
doi: 10.1016/0370-2693(72)90014-7
1972TA13 Z.Phys. 251, 87 (1972) Evidence for Violation of the Gallagher-Moszkowski Rules in 154Pm RADIOACTIVITY 154Pm, 154mPm; measured T1/2, βγ-, γγ-coin, Eγ, Iγ deduced Q, log ft. 154Sm deduced levels, J, π, γ-branching.
doi: 10.1007/BF01380452
1972VA29 Nucl.Instrum.Methods 103, 549 (1972) The Role of Target Geometry in 14 MeV Neutron Capture Cross-Section Measurements NUCLEAR REACTIONS 81Br, 103Rh, 127I, 170Er(n, γ), E=14.5 MeV; measured σ; analyzed target geometry effects.
doi: 10.1016/0029-554X(72)90014-6
1971HA09 Z.Phys. 241, 117 (1971) J.Hattula, H.Helppi, J.Kantele Directional Correlations of Some γ-Ray Cascades in 200Hg RADIOACTIVITY 200Tl; measured γγ(θ). 200Hg levels deduced γ-mixing, J, π.
doi: 10.1007/BF01397900
1971KO03 Nucl.Phys. A163, 513 (1971) T.Komppa, A.Pakkanen, J.Kantele Reinvestigation of the Decay of 200Tl RADIOACTIVITY 200Tl[from 197Au(α, n), Hg(d, xn)]; measured Eγ, Iγ, γγ-coin; deduced log ft. 200Hg deduced levels, J, π, γ-branching. Natural targets.
doi: 10.1016/0375-9474(71)90505-7
1970HA08 Z.Phys. 231, 203 (1970) J.Hattula, E.Liukkonen, J.Kantele Levels of 118Sn Populated in the Decay of 118In and 118Sb Isomers RADIOACTIVITY 118mIn; measured Eγ, Iγ, γγ-coin; deduced log ft. 118,118mSb; measured Eγ, Iγ, γγ-coin, γγ(θ); deduced log ft. 118Sn deduced levels, J, π, B(E2).
doi: 10.1007/BF01401032
1970KA43 Nucl.Instr.Methods 86, 65 (1970) A Ge(Li)-Ge(Li) Sum-Peak (Summing Coincidence) Spectrometer RADIOACTIVITY 152Eu; measured Eγ. Ge(Li)-Ge(Li) sum coin spectrometer.
doi: 10.1016/0029-554X(70)90037-6
1969EL02 Nucl.Phys. A129, 113 (1969) C.Ellegaard, J.Kantele, P.Vedelsby Particle-Vibration Coupling in 209Pb NUCLEAR REACTIONS 208Pb(d, p), (d, pγ), E=12.0 MeV; measured σ(Ep, θ), Eγ, Iγ, γp-coin. 209Pb deduced levels, L(n), π, S. Enriched targets.
doi: 10.1016/0375-9474(69)90912-9
1969HA08 Nucl.Phys. A125, 477 (1969) J.Hattula, E.Liukkonen, J.Kantele New Isomeric State in 118In RADIOACTIVITY 118In isomer [from 118Sn(n, p)]; measured Eγ, Iγ, ICC, T1/2; deduced J, π. 118Sn deduced levels. Enriched target.
doi: 10.1016/0375-9474(69)91088-4
1969PA02 Z.Physik 218, 273 (1969) A.Pakkanen, J.Kantele, P.Suominen Levels in 208Pb Populated in the Decay of 208Tl(ThC'') RADIOACTIVITY 208Tl [from 228Th decay]; measured Eγ, Iγ, γγ-coin. 208Pb deduced levels.
doi: 10.1007/BF01458409
1968BO23 Nucl.Phys. A115, 219 (1968) M.Bonitz, J.Kantele, N.J.S.Hansen Evidence for j-Forbidden Isomeric Transition in 208Bi RADIOACTIVITY 208mBi[from 208Pb(d, 2n)]; measured Eγ, Iγ, I(ce). 208Bi deduced levels, J, π, ICC. Enriched target, Ge(Li) detector.
doi: 10.1016/0375-9474(68)90656-8
1968HA36 Nucl.Instr.Methods 65, 77 (1968) J.Hattula, J.Kantele, A.Sarmanto The Use of the Integral-Bias Summing Coincidence Spectrometer in Directional Correlation Measurements NUCLEAR STRUCTURE 106Ru, 88Y, 60Co, 118Te; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-554X(68)90010-4
1968LI01 Z.Physik 208, 208 (1968) On the Disintegration Energies of 174Lu Isomers NUCLEAR STRUCTURE 174Lu, 174Hf; measured not abstracted; deduced nuclear properties.
doi: 10.1007/BF01380123
1967EL05 Phys.Lett. 25B, 512 (1967) C.Ellegaard, J.Kantele, P.Vedelsby Experimental Evidence for Particle-Vibration Coupling in 209Pb NUCLEAR STRUCTURE 209Pb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90224-9
1967KA13 Z.Physik 204, 456 (1967) J.Kantele, E.Liukkonen, A.Sarmanto A Note on the Structure of the 1518 keV Isomeric State in 174Yb NUCLEAR STRUCTURE 174Lu, 174Tm; measured not abstracted; deduced nuclear properties.
doi: 10.1007/BF01325736
1967KA22 Ann.Acad.Sci.Fennicae Ser.A, VI, No.259 (1967) J.Kantele, J.Hattula, T.Hattula, H.Kalm, O.J.Marttila Decay of 119Te Isomers and Structure of 119Sb NUCLEAR STRUCTURE 119Te, 119Sb; measured not abstracted; deduced nuclear properties.
1966KA21 Nucl.Instr.Methods 39, 194 (1966) J.Kantele, O.J.Marttila, J.Hattula Gamma Spectrometer Systems Employing an Anti-Compton Annulus RADIOACTIVITY 52Mn; measured Eγ, Iγ, βγ-coin. 88Y, 207Bi, 208Tl; measured γγ-coin. 52Cr, 88Sr, 207,208Pb deduced levels. Anti-Compton spectrometer.
doi: 10.1016/0029-554X(66)90225-4
1964KA04 Nucl.Phys. 51, 604 (1964) J.Kantele, K.M.Broom, D.M.Chittenden II A 0.46 μs isomer in Gd157 NUCLEAR STRUCTURE 157Eu; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90298-6
1964KA10 Phys.Rev. 135, B9 (1964) Nuclear Levels of Even Sn Isotopes Populated in the Decay of In Isomers NUCLEAR STRUCTURE 120In, 122In, 118Sb, 118In; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.135.B9
1964KA15 Phys.Letters 11, 59 (1964) An 850 μs isomeric State in Yb174 NUCLEAR STRUCTURE 174Tm; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(64)90258-6
1964KA16 Ann.Acad.Sci.Fennicae Ser. A VI, No.162 (1964) J.Kantele, K.M.Broom, D.M.Chittenden II Decay of Eu157 and Tm174 NUCLEAR STRUCTURE 174Tm, 157Eu; measured not abstracted; deduced nuclear properties.
1963KA02 Phys.Rev. 129, 270 (1963) New Isotope In122 NUCLEAR STRUCTURE 122In; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.129.270
1963KA04 Nucl.Phys. 43, 187 (1963) Disintegration of Te119 Isomers NUCLEAR STRUCTURE 119Te; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90340-7
1963KA06 Univ.Arkansas, Nucl.Chem.Res., Ann.Progr.Rept. p.2 (1963) Study of the Levels and Level Systematics of Even Sn Isotopes from the Decay of In118, In120, In122, and In124 Isomers NUCLEAR STRUCTURE 120In, 122In, 124In, 118In; measured not abstracted; deduced nuclear properties.
1963KA07 Univ.Arkansas, Nucl.Chem.Res., Ann.Progr.Rept. p.4 (1963) Decay of Sc48 and Sc50 NUCLEAR STRUCTURE 50Sc, 48Sc; measured not abstracted; deduced nuclear properties.
1963KA08 Univ.Arkansas, Nucl.Chem.Res., Ann.Progr.Rept. p.5 (1963) Decay of Eu157 and Gd159 NUCLEAR STRUCTURE 157Eu, 159Gd; measured not abstracted; deduced nuclear properties.
1963KA09 Univ.Arkansas, Nucl.Chem.Res., Ann.Progr.Rept. 6 (1963) Decay of Tm173 and Tm174 NUCLEAR STRUCTURE 174Tm, 173Tm; measured not abstracted; deduced nuclear properties.
1963KA10 Univ.Arkansas, Nucl.Chem.Res., Ann.Progr.Rept., p.6 (1963) Decay of Ho167, Ho168, Ho170, and Dy167 NUCLEAR STRUCTURE 167Ho, 167Dy, 168Ho, 170Ho; measured not abstracted; deduced nuclear properties.
1963KA11 Univ.Arkansas, Nucl.Chem.Res., Progr.Rept. p.10 (1963) Rh110 NUCLEAR STRUCTURE 110Rh; measured not abstracted; deduced nuclear properties.
1963KA16 Ann.Acad.Sci.Fennicae, Ser. A VI, No.126 (1963) Radioactive Decay of Sc48, Sc50 and Sc50m NUCLEAR STRUCTURE 50Sc, 48Sc; measured not abstracted; deduced nuclear properties.
1963KA21 Phys.Letters 6, 98 (1963) New Nuclear Species Sc50m and Rh110 NUCLEAR STRUCTURE 50Sc, 110Rh; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(63)90237-3
1962KA24 Phys.Letters 2, 293 (1962) Isomeric State in Yb176 NUCLEAR STRUCTURE 176Yb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(62)90045-8
1962KA37 Nucl.Phys. 35, 353 (1962) Some Activation Cross Sections For 14.7Mev Neutrons NUCLEAR REACTIONS 11B(n, α), 11B(n, p), 16O(n, p), 19F(n, p), 27Al(n, p), 31P(n, 2n), 31P(n, α), 31P(n, p), 63Cu(n, 2n), 63Cu(n, α), 65Cu(n, 2n), 65Cu(n, α), 65Cu(n, nα), E=-1.0 eV-14.7 MeV; measured products, 11Be, Eπ, Iπ; deduced σ, σ(E). Data were imported from EXFOR entry 11196.
doi: 10.1016/0029-5582(62)90129-3
1961FI05 Arkiv Fysik 19, 323 (1961) R.W.Fink, G.Andersson, J.Kantele Nuclear Spectroscopy of Mass-Separated Neutron-Deficient Tellurium Isotopes NUCLEAR STRUCTURE 119Te, 116Te, 117Te, 118Te, 115Te, 114Te; measured not abstracted; deduced nuclear properties.
1961KA02 Bull.Am.Phys.Soc. 6, No.3, 252, H12 (1961) Activation Cross Sections for 14.5-MeV Neutrons for B11, O16, Al27, and F19 NUCLEAR STRUCTURE 11Be, 19O, 16N; measured not abstracted; deduced nuclear properties.
1959KA69 Ann.Acad.Sci.Fennicae, Ser.A VI, No.37 (1959) On the Level Structure of B10
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