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Search: Author = J.Kantele

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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
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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
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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
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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
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1989KA07      Nucl.Instrum.Methods Phys.Res. A275, 149 (1989)

J.Kantele

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
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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
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1988KA22      Nucl.Instrum.Methods Phys.Res. A271, 625 (1988)

J.Kantele

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1983TR11      Nucl.Instrum.Methods 212, 221 (1983)

W.Trzaska, J.Aysto, J.Kantele

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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0348.


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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1977KA17      Phys.Scr. 15, 202 (1977)

J.Kantele

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
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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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1974RA31      Phys.Fenn. 9, 103 (1974)

V.Rahkonen, J.Kantele

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)

J.Kantele, M.Valkonen

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
Citations: PlumX Metrics


1972KA21      Phys.Lett. 39B, 625 (1972)

J.Kantele, M.Valkonen

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset20544.


1972TA13      Z.Phys. 251, 87 (1972)

O.Tannila, J.Kantele

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
Citations: PlumX Metrics


1972VA29      Nucl.Instrum.Methods 103, 549 (1972)

M.Valkonen, J.Kantele

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1970KA43      Nucl.Instr.Methods 86, 65 (1970)

J.Kantele, P.Suominen

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1265.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1968LI01      Z.Physik 208, 208 (1968)

E.Liukkonen, J.Kantele

On the Disintegration Energies of 174Lu Isomers

NUCLEAR STRUCTURE 174Lu, 174Hf; measured not abstracted; deduced nuclear properties.

doi: 10.1007/BF01380123
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1964KA10      Phys.Rev. 135, B9 (1964)

J.Kantele, M.Karras

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12003.


1964KA15      Phys.Letters 11, 59 (1964)

J.Kantele

An 850 μs isomeric State in Yb174

NUCLEAR STRUCTURE 174Tm; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(64)90258-6
Citations: PlumX Metrics


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)

J.Kantele, M.Karras

New Isotope In122

NUCLEAR STRUCTURE 122In; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.129.270
Citations: PlumX Metrics


1963KA04      Nucl.Phys. 43, 187 (1963)

J.Kantele, R.W.Fink

Disintegration of Te119 Isomers

NUCLEAR STRUCTURE 119Te; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(63)90340-7
Citations: PlumX Metrics


1963KA06      Univ.Arkansas, Nucl.Chem.Res., Ann.Progr.Rept. p.2 (1963)

J.Kantele, M.Karras

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)

J.Kantele

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)

J.Kantele, D.M.Chittenden

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)

J.Kantele, K.M.Broom

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)

M.Karras, J.Kantele

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)

J.Kantele, M.Karras

Rh110

NUCLEAR STRUCTURE 110Rh; measured not abstracted; deduced nuclear properties.


1963KA16      Ann.Acad.Sci.Fennicae, Ser. A VI, No.126 (1963)

J.Kantele

Radioactive Decay of Sc48, Sc50 and Sc50m

NUCLEAR STRUCTURE 50Sc, 48Sc; measured not abstracted; deduced nuclear properties.


1963KA21      Phys.Letters 6, 98 (1963)

M.Karras, J.Kantele

New Nuclear Species Sc50m and Rh110

NUCLEAR STRUCTURE 50Sc, 110Rh; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(63)90237-3
Citations: PlumX Metrics


1962KA24      Phys.Letters 2, 293 (1962)

J.Kantele

Isomeric State in Yb176

NUCLEAR STRUCTURE 176Yb; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(62)90045-8
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12105.


1962KA37      Nucl.Phys. 35, 353 (1962)

J.Kantele, D.G.Gardner

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11196.


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)

J.Kantele

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)

J.Kantele

On the Level Structure of B10


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