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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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1990GU01      Nucl.Phys. A506, 196 (1990)

J.Gulyas, Zs.Dombradi, T.Fenyes, J.Timar, A.Passoja, J.Kumpulainen, R.Julin

Structure of 106In Nucleus

NUCLEAR REACTIONS 106Cd(p, nγ), E=8, 8.7, 9, 11 MeV; measured Eγ, Iγ, γγ-coin, I(ce), Iγ(θ). 106In deduced levels, γ-branching, δ, J, π. Hyperpure Ge, Ge(Li), Ge(LEPS) detectors, superconducting magnetic lens plus Si(Li), intermediate-image magnetic plus Si(Li) electron spectrometers. Enriched targets.

doi: 10.1016/0375-9474(90)90383-W
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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.


1989DI13      Nucl.Instrum.Methods Phys.Res. A282, 10 (1989)

J.S.Dionisio, Ch.Vieu, J.M.Lagrange, M.Pautrat, J.Vanhorenbeeck, A.Passoja

Case Studies of Target Properties in Nuclear Spectroscopy

RADIOACTIVITY 195,197Pb(EC), (β+) [from 186W(16O, X), E=95 MeV]; measured electron spectra energy differences. 200mPb; measured I(ce) following isomer decays. 187Au(EC), (β+); measured γ(e)-coin. 200Pb deduced levels. Recoil ion catcher method, target properties role.

doi: 10.1016/0168-9002(89)90103-4
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1989KR12      Nucl.Phys. A503, 113 (1989)

A.Krasznahorkay, Zs.Dombradi, J.Timar, Z.Gacsi, T.Kibedi, A.Passoja, R.Julin, J.Kumpulainen, S.Brant, V.Paar

Nuclear Structure of 110In

NUCLEAR REACTIONS 107Ag(α, nγ), E=14.5, 17 MeV; 110Cd(p, nγ), E=7.5 MeV; measured Eγ, Iγ, γγ-coin, (e-)p(t), (e-)(α)(t), DSA. 110In deduced levels, γ-branching, γ-multipolarity, J, π, T1/2. Ge(Li), Ge(HP), Ge(LEPS) detectors, superconducting magnetic lens plus Si(Li), and miniorange plus Si(Li) electron spectrometers. Enriched targets.

doi: 10.1016/0375-9474(89)90257-1
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1989MO15      Nucl.Phys. A500, 43 (1989)

G.Molnar, T.Belgya, B.Fazekas, A.Veres, S.W.Yates, E.W.Kleppinger, R.A.Gatenby, R.Julin, J.Kumpulainen, A.Passoja, E.Verho

Particle-Hole and Vibrational States in Doubly Closed Subshell 96Zr from In-Beam Inelastic Neutron and Proton Scattering

NUCLEAR REACTIONS 96Zr(n, n'γ), E=2-4.7 MeV; measured Eγ, Iγ, γ(θ), σ(Eγ, E). 96Zr(p, p'γ), E=9.5 MeV; measured Eγ, Iγ, pγ-coin. 96Zr deduced levels, J, π, branching ratios, δ, T1/2, configuration. Enriched targets, Ge(Li), hyperpure Ge, Si(Li) detectors. Subshell closures, shape coexistence, quadrupole, octupole, and hexadecapole vibrations, two-phonon states.

doi: 10.1016/0375-9474(89)90129-2
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14075.


1988AY02      Nucl.Phys. A480, 104 (1988)

J.Aysto, C.N.Davids, J.Hattula, J.Honkanen, K.Honkanen, P.Jauho, R.Julin, S.Juutinen, J.Kumpulainen, T.Lonnroth, A.Pakkanen, A.Passoja, H.Penttila, P.Taskinen, E.Verho, A.Virtanen, M.Yoshii

Levels in 110Pd, 112Pd, 114Pd and 116Pd from the Beta Decays of the On-Line Mass Separated Rh Isotopes

RADIOACTIVITY 110,112,114,116Rh(β-) [from 238U(p, F), E=20 MeV]; measured T1/2-), Q(β-), I(γ), (β-)(ce)-, β-γ-, γγ-coin. 110,112,114,116Pd deduced levels, J, π, level systematics. Ge(Li), Ge, Si-Li, plastic detectors.

doi: 10.1016/0375-9474(88)90387-9
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1988KI04      Phys.Rev. C37, 2391 (1988)

T.Kibedi, Zs.Dombradi, T.Fenyes, A.Krasznahorkay, J.Timar, Z.Gacsi, A.Passoja, V.Paar, D.Vretenar

Structure of 112In Nucleus

NUCLEAR REACTIONS 112Cd(p, nγ), E=4.8 MeV; 109Ag(α, nγ), E=17.1 MeV; measured Eγ, Iγ, I(ce). 112In deduced levels, J, π, γ multipolarity, ICC. Model calculations.

NUCLEAR STRUCTURE 112In; calculated levels, μ, quadrupole moment, Iγ. Interacting boson fermion fermion model.

doi: 10.1103/PhysRevC.37.2391
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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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1987KR15      Nucl.Phys. A473, 471 (1987)

A.Krasznahorkay, T.Fenyes, J.Timar, T.Kibedi, A.Passoja, R.Julin, J.Kumpulainen

Level Structure of 110In from the 110Cd(p, nγ)110In Reaction

NUCLEAR REACTIONS, ICPND 110Cd(p, nγ), E=5.2, 5.6, 6 MeV; measured Eγ, Iγ, γγ-coin, I(ce), level σ, σ(E, Eγ, θ). 110In deduced levels, γ-branching, γ mixing ratio, J, π. Ge(Li), hyperfine Ge detectors, combined magnetic plus Si(Li) electron spectrometer. Enriched targets.

doi: 10.1016/0375-9474(87)90136-9
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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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1986PA19      Z.Phys. A325, 299 (1986)

A.Passoja

First Measurement of K-Shell-Electron to Internal-Pair Conversion Probability Ratios for E0 Transitions in (fp) Shell Region

NUCLEAR REACTIONS 54Fe, 60Ni, 64Zn, 70Ge(p, p'), E=6.9 MeV; measured internal-pair, I(ce) spectra. 54Fe, 60Ni, 64Zn, 70Ge deduced E0 transition K shell electron to internal-pair conversion probability ratios. Enriched targets. Point nucleus approximation.


1986PA23      Phys.Scr. 34, 634 (1986)

A.Passoja

New Methods of In-Beam Internal-Pair Spectroscopy Applied to Nuclear Structure Investigations

NUCLEAR STRUCTURE 16O, 40,42Ca, 54Fe, 60Ni, 64Zn, 70Ge, 90Zr; analyzed K-shell electron to internal-pair conversion probability ratio data.

NUCLEAR REACTIONS 54Fe, 58,60Ni, 64,66Zn(p, p'), E=5-9 MeV; 13C(d, p), E=4.5 MeV; analyzed E0 internal pair transition data; deduced B(E2).

doi: 10.1088/0031-8949/34/6A/019
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1986TI01      Nucl.Phys. A455, 477 (1986)

J.Timar, T.Fenyes, T.Kibedi, A.Passoja, M.Luontama, W.Trzaska, V.Paar

Proton-Neutron Multiplet States in 114In

NUCLEAR REACTIONS 114Cd(p, nγ), E=4.8, 5.3, 7 MeV; measured Eγ, Iγ, I(ce). 114In deduced levels, γ-branching ratios, J, π, γ-multipolarity. Ge(Li), hyperpure Ge detectors, combined magnetic plus Si(Li) electron spectrometer, enriched targets.

doi: 10.1016/0375-9474(86)90318-0
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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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1984FE07      ATOMKI Kozlem. 26, 22 (1984)

T.Fenyes, T.Kibedi, J.Timar, A.Passoja, M.Luontama, W.Trzaska, V.Paar

Proton-Neutron Multiplet States in 114In

NUCLEAR REACTIONS 114Cd(p, nγ), E=4.8, 5.3, 7 MeV; measured Eγ, Iγ. 114In deduced levels, J, π, γ-branching ratios, γ-multipolarity, multiplet classification. Cluster vibration model.


1984JU01      ATOMKI Kozlem. 26, 36 (1984)

R.Julin, M.Luontama, A.Passoja, W.Trzaska

Decay of 0+2 States in Even-Even N = 82 Nuclei

NUCLEAR REACTIONS 144Sm(p, p'), 140Ce, 138Ba(d, 2n), E not given; measured I(ce), centroid shifts. 144Sm, 142Nd, 140Ce levels deduced decay characteristics, T1/2, (E0/E2) branching ratio, monopole transition strength, B(E2).

RADIOACTIVITY 144Eu, 142Pr, 142Pm(β+), (EC); measured Eγ, Iγ, I(ce) following β-decay. 144Sm, 142Nd, 140Ce levels deduced decay characteristics, (E0/E2) branching ratio, B(E2), monopole transition strength.


1984PA15      ATOMKI Kozlem. 26, 75 (1984)

A.Passoja, P.Tikkanen, A.Krasznahorkay, Z.Gacsi, T.Kibedi, T.Fenyes

Adaption of a Superconducting Solenoid Transporter Si(Li)-Si(Li) Spectrometer for In-Beam Studies of Internal-Pair Transitions

NUCLEAR REACTIONS 19F, 23Na(p, αγ), 27Al, 42Ca(p, p'γ), E=3.5-4 MeV; measured γ spectra. 20Ne, 27Al, 42Ca deduced internal pair transition characteristics. Superconducting solenoid transporter, Si(Li)-Si(Li) spectrometer.


1984PA16      Nucl.Instrum.Methods 223, 96 (1984)

A.Passoja, P.Tikkanen, A.Krasznahorkay, Z.Gacsi, T.Kibedi, T.Fenyes

Adaptation of a Superconducting-Solenoid-Transporter Si(Li)-Si(Li) Spectrometer for In-Beam Studies of Internal-Pair Transitions

NUCLEAR REACTIONS 23Na, 19F(p, α), 27Al, 42Ca(p, p'γ), E=3.5-4 MeV; measured pair spectra, Eγ, Iγ, sum coincidence spectra; deduced pair line efficency.

doi: 10.1016/0167-5087(84)90249-7
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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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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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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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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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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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