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NSR database version of May 30, 2024.

Search: Author = A.Likar

Found 70 matches.

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2015CV01      Appl.Radiat.Isot. 104, 160 (2015)

A.Cvetinovic, A.Likar, M.Lipoglavsek, A.Mihelic, T.Petrovic, J.Vesic, B.Vodenik

Precise measurement of the half-life of 61Cu

RADIOACTIVITY 61Cu(β+), (EC) [from 60Ni(p, γ)]; measured decay products, Eγ, Iγ; deduced T1/2, level energies, J, π. Comparison with theoretical calculations.

doi: 10.1016/j.apradiso.2015.07.005
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2013GA25      Eur.Phys.J. A 49, 70 (2013)

J.Gajevic, A.Cvetinovic, A.Likar, M.Lipoglavsek, P.Pelicon, T.Petrovic, A.Sanchez Ortiz

Electron screening in nickel

ATOMIC PHYSICS Ni(p, γ), (p, X), E=0.86-3.08 MeV; measured thick target Eγ, Iγ using HPGe, backscattered protons, X-rays from PIXE using SiLi from metallic Ni and NiO; deduced isotope yields, levels, γ transitions, branching ratios, electron screening potential, electron density vs intranuclear distance.

doi: 10.1140/epja/i2013-13070-3
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2006LI05      Nucl.Instrum.Methods Phys.Res. A557, 523 (2006)

M.Lipoglavsek, A.Likar, M.Vencelj, T.Vidmar, R.A.Bark, E.Gueorguieva, F.Komati, J.J.Lawrie, S.M.Maliage, S.M.Mullins, S.H.T.Murray, T.M.Ramashidzha

Measuring high-energy γ-rays with Ge clover detectors

NUCLEAR REACTIONS 208Pb(p, γ), E ≈ 11-17 MeV; measured Eγ, Iγ; deduced excitation functions. Afrodite array.

doi: 10.1016/j.nima.2005.11.067
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2006LI17      Phys.Rev. C 73, 044609 (2006)

A.Likar, M.Lipoglavsek, M.Vencelj, T.Vidmar, R.A.Bark, E.Gueorguieva, F.Komati, J.J.Lawrie, S.M.Maliage, S.M.Mullins, S.H.T.Murray, T.M.Ramashidzha

Proton capture to continuum states of 209Bi

NUCLEAR REACTIONS 208Pb(p, γ), E=14.8, 15.7, 16.9 MeV; measured Eγ, Iγ, γγ-coin. Afrodite array. Comparison with model predictions.

doi: 10.1103/PhysRevC.73.044609
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2006VE09      Phys.Scr. T125, 222 (2006)

M.Vencelj, C.Baktash, P.Fallon, P.Hausladen, A.Likar, M.Lipoglavsek, C.-H.Yu

Core excitation in 98Cd

NUCLEAR REACTIONS 58Ni(46Ti, xnypzα), E=175 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin; deduced isotopic yields. 98Cd deduced levels, J, π. Gammasphere, Microball arrays.

doi: 10.1088/0031-8949/2006/T125/061
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2005LI58      Phys.Rev. C 72, 061304 (2005)

M.Lipoglavsek, M.Vencelj, C.Baktash, P.Fallon, P.A.Hausladen, A.Likar, C.-H.Yu

100Sn core excitations in 97Ag

NUCLEAR REACTIONS 58Ni(46Ti, 2npα), E=175 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin. 97Ag deduced levels, J, π, configurations. Gammasphere, Microball arrays, comparison with shell model predictions.

doi: 10.1103/PhysRevC.72.061304
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2005SO06      Nucl.Phys. A753, 251 (2005)

D.Sohler, M.Palacz, Zs.Dombradi, M.Hjorth-Jensen, C.Fahlander, L.-O.Norlin, J.Nyberg, T.Back, K.Lagergren, D.Rudolph, A.Algora, C.Andreoiu, G.de Angelis, A.Atac, D.Bazzacco, J.Cederkall, B.Cederwall, B.Fant, E.Farnea, A.Gadea, M.Gorska, H.Grawe, N.Hashimoto-Saitoh, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, S.M.Lenzi, A.Likar, M.Lipoglavsek, M.Moszynski, D.R.Napoli, C.Rossi-Alvarez, H.A.Roth, T.Saitoh, D.Seweryniak, O.Skeppstedt, J.Timar, M.Weiszflog, M.Wolinska

Maximally aligned states in the proton drip line nucleus 106Sb

NUCLEAR REACTIONS 54Fe(58Ni, npα), E=240 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin, γ-ray polarization. 106Sb deduced high-spin levels, J, π, configurations. Euroball, ISIS arrays.

doi: 10.1016/j.nuclphysa.2005.02.153
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2004SO05      Nucl.Phys. A733, 37 (2004)

D.Sohler, J.Timar, Zs.Dombradi, J.Cederkall, J.Huijnen, M.Lipoglavsek, M.Palacz, A.Atac, C.Fahlander, H.Grawe, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, J.Persson, D.Seweryniak, G.de Angelis, P.Bednarczyk, D.Foltescu, D.Jerrestam, S.Juutinen, E.Makela, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen, M.Weiszflog

Band-terminating states in 101Ag

NUCLEAR REACTIONS 50Cr(58Ni, 3pα), E=261 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin. 101Ag deduced high-spin levels, J, π, configurations, band termination. Cranked Nilsson-Strutinsky calculations. Nordball array.

doi: 10.1016/j.nuclphysa2003.12.002
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2003SO04      Eur.Phys.J. A 16, 171 (2003)

D.Sohler, Zs.Dombradi, J.Blomqvist, J.Cederkall, J.Huijnen, M.Lipoglavsek, M.Palacz, A.Atac, C.Fahlander, H.Grawe, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, J.Persson, D.Seweryniak, G.de Angelis, P.Bednarczyk, D.Foltescu, D.Jerrestam, S.Juutinen, E.Makela, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, J.Timar, S.Tormanen, M.Weiszflog

Maximally aligned states in 99Ag

NUCLEAR REACTIONS 50Cr(58Ni, p2α), E=261 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin. 99Ag deduced high-spin levels, J, π, configurations. Nordball array, shell model calculations.

doi: 10.1140/epja/i2002-10092-x
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2002LI04      Phys.Rev. C65, 021302 (2002)

M.Lipoglavsek, C.Baktash, M.P.Carpenter, D.J.Dean, T.Engeland, C.Fahlander, M.Hjorth-Jensen, R.V.F.Janssens, A.Likar, J.Nyberg, E.Osnes, S.D.Paul, A.Piechaczek, D.C.Radford, D.Rudolph, D.Seweryniak, D.G.Sarantites, M.Vencelj, C.-H.Yu

100Sn Core Excitations in 102In

NUCLEAR REACTIONS 50Cr(58Ni, npα), E=225 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin. 102In deduced levels, possible J, π, configurations. Gammasphere, Microball arrays. Comparison with large-scale shell model calculations.

doi: 10.1103/PhysRevC.65.021302
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2002LI33      Phys.Rev. C65, 051307 (2002)

M.Lipoglavsek, C.Baktash, M.P.Carpenter, D.J.Dean, T.Engeland, C.Fahlander, M.Hjorth-Jensen, R.V.F.Janssens, A.Likar, J.Nyberg, E.Osnes, S.D.Paul, A.Piechaczek, D.C.Radford, D.Rudolph, D.Seweryniak, D.G.Sarantites, M.Vencelj, C.H.Yu

Excited States of the Proton Emitter 105Sb

NUCLEAR REACTIONS 50Cr(58Ni, 2np), E=225 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin. 105Sb deduced levels, possible J, π. Gammasphere, Microball arrays. Comparison with shell model results.

doi: 10.1103/PhysRevC.65.051307
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2002LI45      Phys.Rev. C66, 011302 (2002)

M.Lipoglavsek, C.Baktash, J.Blomqvist, M.P.Carpenter, D.J.Dean, T.Engeland, C.Fahlander, M.Hjorth-Jensen, R.V.F.Janssens, A.Likar, J.Nyberg, E.Osnes, S.D.Paul, A.Piechaczek, D.C.Radford, D.Rudolph, D.Seweryniak, D.G.Sarantites, M.Vencelj, C.-H.Yu

Breakup of the Doubly Magic 100Sn Core

NUCLEAR REACTIONS 50Cr(58Ni, xnypzα)99Cd/101In, E=225 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin; deduced relative yields. 99Cd, 101In deduced high-spin levels, J, π, configurations, core excitation. Gammasphere, Microball arrays, large-scale shell model calculations.

doi: 10.1103/PhysRevC.66.011302
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2002SO12      Nucl.Phys. A708, 181 (2002)

D.Sohler, M.Palacz, Zs.Dombradi, J.Blomqvist, C.Fahlander, L.-O.Norlin, J.Nyberg, T.Back, K.Lagergren, D.Rudolph, A.Algora, C.Andreoiu, G.de Angelis, A.Atac, D.Bazzacco, J.Cederkall, B.Cederwall, B.Fant, E.Farnea, A.Gadea, M.Gorska, H.Grawe, N.Hashimoto-Saitoh, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, S.M.Lenzi, A.Likar, M.Lipoglavsek, M.Moszynski, D.R.Napoli, C.Rossi-Alvarez, H.A.Roth, T.Saitoh, D.Seweryniak, O.Skeppstedt, J.Timar, M.Weiszflog, M.Wolinska

Neutron Excitations Across the N = 50 Shell Gap in 102In

NUCLEAR REACTIONS 54Fe(58Ni, np2α), E=240 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin, γ-ray polarization. 102In deduced levels, J, π, configurations, transition multipolarities. Euroball and ISIS arrays, neutron wall. Comparison with shell model calculations.

doi: 10.1016/S0375-9474(02)01014-X
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2001BE15      Nucl.Phys. A686, 204 (2001)

E.Betak, F.Cvelbar, A.Likar, T.Vidmar

Model Calculations of the Radiative Capture Process and the Brink-Axel Hypothesis

NUCLEAR REACTIONS 140Ce, 208Pb(n, γ), E=4-18 MeV; calculated σ(E), excitation functions. Consistent direct-semidirect and preequilibrium exciton models. Comparisons with data.

doi: 10.1016/S0375-9474(00)00562-5
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2001FA01      Phys.Rev. C63, 021307 (2001)

C.Fahlander, M.Palacz, D.Rudolph, D.Sohler, J.Blomqvist, J.Kownacki, K.Lagergren, L.O.Norlin, J.Nyberg, A.Algora, C.Andreoiu, G.de Angelis, A.Atac, D.Bazzacco, L.Berglund, T.Back, J.Cederkall, B.Cederwall, Zs.Dombradi, B.Fant, E.Farnea, A.Gadea, M.Gorska, H.Grawe, N.Hashimoto-Saitoh, A.Johnson, A.Kerek, W.Klamra, S.M.Lenzi, A.Likar, M.Lipoglavsek, M.Moszynski, D.R.Napoli, C.Rossi-Alvarez, H.A.Roth, T.Saitoh, D.Seweryniak, O.Skeppstedt, M.Weiszflog, M.Wolinska

Excited States in 103Sn: Neutron single-particle energies with respect to 100Sn

NUCLEAR REACTIONS 54Fe(58Ni, n2α), E=240 MeV; measured Eγ, Iγ, (neutron)γ-, (charged particle)γ-, γγ-coin. 103Sn deduced levels, J, π, single particle neutron orbital energies. Comparison with other Sn isotopes and Shell model calculations. Euroball array.

doi: 10.1103/PhysRevC.63.021307
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2001LI12      Nucl.Phys. A682, 399c (2001)

M.Lipoglavsek, C.Baktash, M.P.Carpenter, D.J.Dean, C.Fahlander, M.Hjorth-Jensen, R.V.F.Janssens, A.Likar, J.Nyberg, S.D.Paul, A.Piechaczek, D.C.Radford, D.Rudolph, D.Seweryniak, D.G.Sarantites, M.Vencelj, C.H.Yu

First Observation of Excitation Across the 100Sn Core

NUCLEAR REACTIONS 50Cr(58Ni, xnypzα)95Rh/96Pd/97Pd/98Pd/100Pd/98Ag/99Ag/100Ag/101Ag/103Ag/98Cd/99Cd/100Cd/101Cd/102Cd/103Cd/104Cd/101In/102In/103In/104In/105In/102Sn/103Sn/104Sn/105Sn/106Sn/105Sb/106Sb, E=225 MeV; measured γγ-, (charged particle)γ-, (neutron)γ-coin; deduced relative yields. Gammasphere, Microball arrays.

doi: 10.1016/S0375-9474(00)00666-7
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2001PA12      Acta Phys.Pol. B32, 999 (2001)

M.Palacz, C.Fahlander, D.Sohler, D.Rudolph, J.Blomqvist, J.Kownacki, K.Lagergren, L.O.Norlin, J.Nyberg, A.Algora, C.Andreoiu, G.De Angelis, A.Atac, D.Bazzacco, L.Berglund, T.Back, J.Cederkall, B.Cederwall, Zs.Dombradi, B.Fant, E.Farnea, A.Gadea, M.Gorska, H.Grawe, N.Hashimoto-Saitoh, A.Johnson, A.Kerek, W.Klamra, S.M.Lenzi, A.Likar, M.Lipoglavsek, M.Moszynski, D.Napoli, C.Rossi-Alvarez, H.Roth, T.Saitoh, D.Seweryniak, O.Skeppstedt, M.Weiszflog, M.Wolinska

Investigations of Neutron Deficient Nuclei close to 100Sn with Euroball

NUCLEAR REACTIONS 54Fe(58Ni, n2α), E=240 MeV; measured Eγ, Iγ, γγ-, (neutron)γ-, (charged particle)γ-coin. 103Sn deduced levels, possible J, π. Euroball array. Comparison with shell model.


2001PE05      Nucl.Phys. A686, 41 (2001)

G.E.Perez, D.Sohler, A.Algora, Zs.Dombradi, B.M.Nyako, J.Timar, L.Zolnai, R.Wyss, J.Cederkall, A.Johnson, A.Kerek, W.Klamra, L.-O.Norlin, M.Lipoglavsek, C.Fahlander, A.Likar, M.Palacz, A.Atac, J.Nyberg, J.Persson, A.Gizon, J.Gizon, A.J.Boston, E.S.Paul, H.Grawe, R.Schubart, D.T.Joss, S.Juutinen, E.Makela, J.Kownacki, M.de Poli, P.Bednarczyk, G.de Angelis, D.Seweryniak, D.Foltescu, H.A.Roth, O.Skeppstedt, D.Jerrestam, T.Shizuma, G.Sletten, S.Tormanen

Structure of High-Spin States in 100Pd

NUCLEAR REACTIONS 50Cr(58Ni, 4pα), E=261 MeV; 70Zn(36S, 6n), E=130 MeV; measured Eγ, Iγ, γγ-, (particle)γ-coin, γ-ray angular correlation and linear polarization. 100Pd deduced high-spin levels, J, π, multipolarities, terminating bands. Nordball and Eurogam II arrays, cranked mean-field calculations.

doi: 10.1016/S0375-9474(00)00513-3
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2000LI06      J.Phys.(London) G26, 219 (2000)

A.Likar, T.Vidmar

Direct Capture of Protons in the Medium-Energy Range

NUCLEAR REACTIONS 12C, 11B(p, γ), E=98, 176 MeV; calculated σ(E, θ). Optical model, comparison with data.

doi: 10.1088/0954-3899/26/3/301
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2000PA16      Nucl.Instrum.Methods Phys.Res. A443, 304 (2000)

G.Pausch, H.Prade, M.Sobiella, H.Schnare, R.Schwengner, L.Kaubler, C.Borcan, H.-G.Ortlepp, U.Oehmichen, H.Grawe, R.Schubart, J.Gerl, J.Cederkall, A.Johnson, A.Kerek, W.Klamra, M.Moszynski, D.Wolski, M.Kapusta, A.Axelsson, M.Weiszflog, T.Hartlein, D.Pansegrau, G.de Angelis, S.Ashrafi, A.Likar, M.Lipoglavsek

RoSiB - A 4π Silcon Ball for Charged-Particle Detection in EUROBALL

NUCLEAR REACTIONS 46Ti(58Ni, xnypzα), E=228 MeV; 58Ni(16O, xnypzα), E=95 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin; deduced detector characteristics. Monte Carlo simulation.

doi: 10.1016/S0168-9002(99)01090-6
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1999CV01      Nucl.Phys. A645, 262 (1999)

F.Cvelbar, A.Likar, T.Vidmar

Angular Distribution Effect on the Integrated Cross Section for Radiative Capture of 14 MeV Neutrons

NUCLEAR REACTIONS 40Ca, 28Si, 89Y, 208Pb(n, γ), E=14 MeV; calculated Iγ(θ), Legendre coefficient a2. Consistent direct-semidirect model. Comparisons with data.

doi: 10.1016/S0375-9474(98)00609-5
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1999DA10      Phys.Rev. C59, 1956 (1999)

I.Danko, D.Sohler, Zs.Dombradi, S.Brant, V.Krstic, J.Cederkall, M.Lipoglavsek, M.Palacz, J.Persson, A.Atac, C.Fahlander, H.Grawe, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, V.Paar, R.Schubart, D.Seweryniak, D.Vretenar, G.de Angelis, P.Bednarczyk, D.Foltescu, D.Jerrestam, S.Juutinen, E.Makela, B.M.Nyako, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen

Collective and Broken Pair States of 65, 67Ga

NUCLEAR REACTIONS 12C(58Ni, pα), (58Ni, 3p), E=261 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin. 65,67Ga deduced high-spin levels, J, π, configurations. Nordball array.

NUCLEAR STRUCTURE 65,67Ga; calculated levels, J, π, B(E2), B(M1). Interacting boson-fermion plus interacting pair model.

doi: 10.1103/PhysRevC.59.1956
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1999LI26      J.Phys.(London) G25, 1713 (1999)

A.Likar, T.Vidmar, F.Cvelbar

Mass and State Dependence of the Interaction Function in the Direct-Semidirect Capture Model

NUCLEAR STRUCTURE 40Ca, 90Y, 141Ce, 209Pb; calculated nucleon capture particle-vibration coupling parameters; deduced mass-dependence features. Consistent direct-semidirect model.

doi: 10.1088/0954-3899/25/8/313
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1998CE03      Eur.Phys.J. A 1, 7 (1998); Erratum Eur.Phys.J. A 2, 111 (1998)

J.Cederkall, M.Lipoglavsek, M.Palacz, J.Persson, J.Blomqvist, A.Atac, C.Fahlander, H.Grawe, A.Johnson, W.Klamra, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, R.Schubart, D.Seweryniak, G.de Angelis, P.Bednarczyk, Zs.Dombradi, D.Foltescu, M.Gorska, D.Jerrestam, S.Juutinen, E.Makela, B.M.Nyako, G.Perez, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen

Maximum Spin Aligned States in 4798Ag51

NUCLEAR REACTIONS 50Cr(58Ni, np2α), E=261 MeV; measured Eγ, Iγ, γγ-, (evaporated particle)γ-coin. 98Ag deduced levels, possible J, π, configurations.

doi: 10.1007/s100500050024
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1998LI21      Nucl.Phys. A635, 43 (1998)

A.Likar, T.Vidmar

Integrated Cross Sections in Fast Neutron Capture in Light Nuclei

NUCLEAR REACTIONS 28Si, 32S, 40Ca(n, γ), E=fast; calculated σ, σ(θ). Direct-semidirect capture model. Comparison with data.

doi: 10.1016/S0375-9474(98)00161-4
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1998LI26      Nucl.Phys. A637, 365 (1998)

A.Likar, T.Vidmar

Integrated Cross Sections in Fast Neutron Capture in Medium Weight and Heavy Nuclei

NUCLEAR REACTIONS 89Y, 208Pb(n, γ), E=4-20 MeV; calculated σ(θ=90°). 89Y, Ba(n, γ), E=14 MeV; calculated σ(Eγ). Consistent direct-semi-direct capture model, capture systematics for A=20-240 discussed. Comparison with data.

doi: 10.1016/S0375-9474(98)00244-9
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1998SO23      Nucl.Phys. A644, 141 (1998)

D.Sohler, Zs.Dombradi, S.Brant, J.Cederkall, M.Lipoglavsek, M.Palacz, V.Paar, J.Persson, A.Atac, C.Fahlander, H.Grawe, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, R.Schubart, D.Seweryniak, G.de Angelis, P.Bednarczyk, D.Foltescu, D.Jerrestam, S.Juutinen, E.Makela, B.M.Nyako, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen

Structure of 68As Studied via the 12C(58Ni, pn) Reaction

NUCLEAR REACTIONS 12C(58Ni, np), E=261 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin, angular distribution ratios. 68As deduced levels, J, π. Enriched targets, Nordball array. Interacting boson-fermion-fermion model calculations.

doi: 10.1016/S0375-9474(98)00575-2
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1997CE08      Z.Phys. A359, 227 (1997)

J.Cederkall, G.Perez, M.Lipoglavsek, M.Palacz, J.Persson, A.Atac, J.Blomqvist, C.Fahlander, H.Grawe, A.Johnson, W.Klamra, J.Kownacki, A.Likar, L.O.Norlin, J.Nyberg, R.Schubart, D.Seweryniak, G.de Angelis, P.Bednarczyk, Zs.Dombradi, D.Foltescu, D.Jerrestam, S.Juutinen, E.Makela, B.M.Nyako, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen

New Spectroscopic Information on 98Pd

NUCLEAR REACTIONS 50Cr(58Ni, 2p2α), E=261 MeV; measured Eγ, Iγ, γγ-coin, γ(θ). 98Pd deduced high-spin levels, J, π, configurations.

doi: 10.1007/s002180050392
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1997GO02      Acta Phys.Pol. B28, 303 (1997)

M.Gorska, M.Lipoglavsek, H.Grawe, J.Nyberg, A.Atac, A.Axelsson, R.Bark, J.Blomqvist, J.Cederkall, B.Cederwall, G.de Angelis, C.Fahlander, A.Johnson, S.Leoni, A.Likar, M.Matiuzzi, S.Mitarai, L.-O.Norlin, M.Palacz, J.Persson, H.A.Roth, R.Schubart, D.Seweryniak, T.Shizuma, O.Skeppstedt, G.Sletten, W.B.Walters, M.Weiszflog

Spectroscopy of the T(z) = 1 Nuclei Close to 100Sn

NUCLEAR REACTIONS 46Ti(58Ni, 2nα), E=215 MeV; 50Cr(58Ni, 2nα), E=225 MeV; measured γγ-coin sum spectra, γ(recoil)(t). 98Cd deduced levels, J, π, T1/2, isomers, decay features, B(λ). 102Sn deduced levels, J, π, T1/2, isomers, decay features.


1997GO18      Phys.Rev.Lett. 79, 2415 (1997)

M.Gorska, M.Lipoglavsek, H.Grawe, J.Nyberg, A.Atac, A.Axelsson, R.Bark, J.Blomqvist, J.Cederkall, B.Cederwall, G.de Angelis, C.Fahlander, A.Johnson, S.Leoni, A.Likar, M.Matiuzzi, S.Mitarai, L.-O.Norlin, M.Palacz, J.Persson, H.A.Roth, R.Schubart, D.Seweryniak, T.Shizuma, O.Skeppstedt, G.Sletten, W.B.Walters, M.Weiszflog

4898Cd50: The two-proton-hole spectrum in 50100Sn50

NUCLEAR REACTIONS 46Ti(58Ni, 2nα), E=215, 225 MeV; 50Cr(58Ni, 2n2α), E=215, 225 MeV; measured Eγ, Iγ, γγ-, nγ-, αγ-coin, Iγ vs time; deduced 98Cd production. 98Cd deduced levels, J, π, isomeric state T1/2, B(λ), configurations. Other nuclei compared.

doi: 10.1103/PhysRevLett.79.2415
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1997KO51      Nucl.Phys. A627, 239 (1997)

J.Kownacki, M.Lipoglavsek, L.-O.Norlin, J.Nyberg, D.Seweryniak, J.Cederkall, M.Palacz, J.Persson, A.Atac, B.Cederwall, C.Fahlander, H.Grawe, A.Johnson, A.Kerek, W.Klamra, M.Karny, F.Liden, A.Likar, R.Schubart, R.Wyss, E.Adamides, G.de Angelis, P.Bednarczyk, Zs.Dombradi, D.Foltescu, M.Gorska, E.Ideguchi, D.Jerrestam, R.Julin, S.Juutinen, S.Mitarai, E.Makela, G.Perez, M.Piiparinen, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen, T.Vass, A.Virtanen

High-Spin Studies of the Neutron Deficient Nuclei 103In, 105In, 107In, and 109In

NUCLEAR REACTIONS 50Cr(58Ni, 2n3p), (58Ni, pα), (58Ni, 3p), E=261 MeV; 54Fe(58Ni, p2α), (58Ni, 5p), (58Ni, 3pα), E=270 MeV; 92Mo(19F, 2p), E=95 MeV; measured Eγ, Iγ(θ), γγ-coin. 103,105,107,109In deduced high-spin levels, J, π, configuration. Shell model, hole-core coupling scheme.

doi: 10.1016/S0375-9474(97)00479-X
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1997LI03      Nucl.Phys. A615, 18 (1997)

A.Likar, T.Vidmar

Neutron Optical Potential from Capture Reactions

NUCLEAR REACTIONS 40Ca, 89Y, 140Ce, 208Pb(n, γ), E ≈ resonance; analyzed capture σ(θ), σ(E); deduced model parameter dependence. Direct-semidirect model, optical model.

doi: 10.1016/S0375-9474(96)00471-X
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1997LI10      Nucl.Phys. A619, 49 (1997)

A.Likar, T.Vidmar

Direct Neutron Capture in Light Nuclei

NUCLEAR REACTIONS 12C, 16O(n, γ), E < 600 keV; calculated σ(En); deduced influence of scattering potential depth. Consistent direct-semidirect model.

doi: 10.1016/S0375-9474(97)00129-2
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1997LI11      Nucl.Phys. A619, 57 (1997)

A.Likar, T.Vidmar

Fast Neutron Capture in 206Pb, 165Ho, and 238U as Seen Through the Consistent Direct-Semidirect Model

NUCLEAR REACTIONS 165Ho, 238U(n, γ), E=6-16 MeV; 206Pb(n, γ), E=2-12 MeV; calculated σ(En). 166Ho, 207Pb, 239U deduced single-particle states binding energy, spectroscopic factors, GDR related features. Differences between modified, standard direct-semidirect models, studied.

doi: 10.1016/S0375-9474(97)00131-0
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1997PA20      Acta Phys.Pol. B28, 309 (1997)

M.Palacz, J.Cederkall, M.Lipoglavsek, J.Persson, A.Atac, J.Blomqvist, H.Grawe, C.Fahlander, J.Iwanicki, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, R.Schubart, D.Seweryniak, Z.Sujkowski, R.Wyss, G.de Angelis, P.Bednarczyk, Zs.Dombradi, D.Foltescu, D.Jerrestam, S.Juutinen, E.Makela, G.Perez, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen, T.Vass

In Beam γ-Ray Spectroscopy of Very Neutron Deficient Odd-Cadmium Isotopes

NUCLEAR REACTIONS 50Cr(58Ni, n2α), (58Ni, n2pα), (58Ni, n4p), E not given; measured Eγ, Iγ, γγ-coin. 99,101,103Cd deduced high-spin levels, J, π. Results from other Cd isotopes compared.

NUCLEAR STRUCTURE 99,101,103Cd; calculated high-spin levels. Shell model.

Data from this article have been entered in the XUNDL database. For more information, click here.


1997PA25      Nucl.Phys. A624, 210 (1997)

M.Palacz, J.Cederkall, M.Lipoglavsek, J.Persson, A.Atac, J.Blomqvist, H.Grawe, C.Fahlander, J.Iwanicki, A.Johnson, A.Kerek, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, R.Schubart, D.Seweryniak, Z.Sujkowski, R.Wyss, G.de Angelis, P.Bednarczyk, Zs.Dombradi, D.Foltescu, D.Jerrestam, S.Juutinen, E.Makela, G.Perez, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen, T.Vass

In-Beam γ-Ray Spectroscopy of 103Cd

NUCLEAR REACTIONS 58Ni(50Cr, 4pnγ), E=216-261 MeV; measured γγ-coin, Eγ, Iγ. 103Cd deduced high-spin levels, J, π, band structure.

doi: 10.1016/S0375-9474(97)00325-4
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1997PE25      Nucl.Phys. A627, 101 (1997)

J.Persson, J.Cederkall, M.Lipoglavsek, M.Palacz, A.Atac, J.Blomqvist, C.Fahlander, H.Grawe, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, R.Schubart, D.Seweryniak, G.de Angelis, P.Bednarczyk, Zs.Dombradi, D.Foltescu, D.Jerrestam, S.Juutinen, E.Makela, G.Perez, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen, T.Vass

In-Beam γ-Ray Spectroscopy of 102Cd

NUCLEAR REACTIONS 58Ni(50Cr, 2pα), E=261 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ). 102Cd deduced high-spin levels, J, π, transitions multipolarity. Shell model calculations.

doi: 10.1016/S0375-9474(97)00405-3
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1997RI11      Nucl.Phys. A621, 879 (1997)

A.Ringbom, G.Tibell, J.Blomgren, H.Conde, S.Dangtip, K.Elmgren, N.Olsson, J.Rahm, C.Fahlander, L.Nilsson, J.Nyberg, P.-U.Renberg, L.Westerberg, A.Likar

Excitation and Neutron Decay of Xenon Studied by Forward-Angle Scattering of High-Energy 17O Ions

NUCLEAR REACTIONS Xe(17O, 17O'), E=4.24, 6 GeV; measured neutron decay spectrum versus Xe excitation energy following Coulomb excitation; deduced missing energy spectra. Statistical decay calculations.

doi: 10.1016/S0375-9474(97)00194-2
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1997RI14      Nucl.Phys. A626, 241c (1997)

A.Ringbom, G.Tibell, J.Blomgren, H.Conde, S.Dangtip, K.Elmgren, J.Nilsson, N.Olsson, C.Fahlander, L.Nilsson, J.Nyberg, P.-U.Renberg, L.Westerberg, A.Likar

Excitation and Neutron Decay of Xenon by Forward-Angle Scattering of 250A MeV 17O Ions

NUCLEAR REACTIONS Xe(17O, n17O), E=250 MeV/nucleon; measured En, In(θ), σ(E(17O)); deduced resonance structures. Cluster-jet target, tof.

doi: 10.1016/S0375-9474(97)00541-1
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1997SO06      Z.Phys. A357, 239 (1997)

D.Sohler, Zs.Dombradi, S.Brant, J.Cederkall, M.Lipoglavsek, M.Palacz, V.Paar, J.Persson, A.Atac, C.Fahlander, H.Grawe, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, R.Schubart, D.Seweryniak, G.de Angelis, P.Bednarczyk, D.Foltescu, M.Fayez-Hassan, D.Jerrestam, S.Juutinen, E.Makela, B.M.Nyako, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen

Spectroscopy of Neutron Deficient 65Ge

NUCLEAR REACTIONS 12C(58Ni, nα), E=261 MeV; measured γγ-coin, Iγ(θ). 65Ge deduced high-spin levels, J, π. Interacting boson-fermion model.

doi: 10.1007/s002180050238
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1996CE03      Phys.Rev. C53, 1955 (1996); Erratum Phys.Rev. C54, 960 (1996)

J.Cederkall, M.Lipoglavsek, M.Palacz, J.Persson, A.Atac, C.Fahlander, H.Grawe, A.Johnson, W.Klamra, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, R.Schubart, D.Seweryniak, G.de Angelis, P.Bednarczyk, Zs.Dombradi, D.Foltescu, D.Jerrestam, S.Juutinen, E.Makela, B.M.Nyako, G.Perez, M.de Poli, H.A.Roth, T.Schizuma, O.Skeppstedt, G.Sletten, S.Tormanen

First Evidence for Excited States in 101In

NUCLEAR REACTIONS 50Cr(58Ni, 2npα), E=261 MeV; measured γ(particle)-, γγ-coin. 101In deduced levels, possible J, π.

doi: 10.1103/PhysRevC.53.1955
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1996KO23      Acta Phys.Pol. B27, 87 (1996)

J.Kownacki, A.Atac, J.Cederkall, B.Cederwall, C.Fahlander, H.Grawe, E.Ideguchi, A.Johnson, R.Julin, S.Juutinen, M.Karny, A.Kerek, W.Klamra, A.Likar, M.Lipoglavsek, L.-O.Norlin, J.Nyberg, S.Mitarai, E.Makela, M.Palacz, J.Persson, M.Piiparinen, D.Seweryniak, R.Schubart, G.Sletten, S.Tormanen, A.Virtanen, R.Wyss

The Isospin Dependent p-n Multiplets in the Region of Doubly Magic 100Sn

NUCLEAR REACTIONS 50Cr, 54Fe(58Ni, X), E=261, 270 MeV; measured γγ-coin, γγ(θ). 102,104,106,108In deduced levels, configurations. Information on 99Cd, 101In, 106,107,108Sb, 108,109Te also obtained.


1996LI04      Nucl.Phys. A598, 235 (1996)

A.Likar

Nuclear Dicke States and the Direct-Semdirect Model

NUCLEAR REACTIONS 40Ca, 208Pb(n, γ), E ≤ 20 MeV; analyzed capture σ(θ) vs E; deduced nuclear Dicke state role. Modified direct semidirect model.

doi: 10.1016/0375-9474(95)00440-8
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1996LI06      Phys.Rev.Lett. 76, 888 (1996)

M.Lipoglavsek, J.Cederkall, M.Palacz, J.Persson, A.Atac, J.Blomqvist, C.Fahlander, H.Grawe, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, R.Schubart, D.Seweryniak, G.de Angelis, P.Bednarczyk, Zs.Dombradi, D.Foltescu, D.Jerrestam, S.Juutinen, E.Makela, G.Perez, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen, T.Vass

Stability of 50100Sn50 Deduced from Excited States in 4899Cd51

NUCLEAR REACTIONS 50Cr(58Ni, X), E=261 MeV; measured Eγ, Iγ, γγ-coin, neutron, α-particle multiplicity intensity ratios for 99,101Cd, 105,103,104In, 98Ag, 97Pd, 95Rh. 99Cd deduced high-spin levels, J, π, T1/2, B(λ) in one case.

doi: 10.1103/PhysRevLett.76.888
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1996LI48      Nucl.Phys. A611, 56 (1996)

A.Likar, T.Vidmar

Interference of Isovector and Isoscalar Giant Quadrupole Resonances in Y and Pb

NUCLEAR REACTIONS, ICPND 208Pb(p, γ), E=8-26 MeV; 89Y(n, γ), E=10-35 MeV; 209Bi(n, γ), E=16-28 MeV; analyzed σ(E), asymmetry vs E; deduced isovector, isoscalar GQR interference. Direct-semi-direct capture model.

doi: 10.1016/S0375-9474(96)00322-3
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1996LI50      Z.Phys. A356, 239 (1996)

M.Lipoglavsek, M.Gorska, J.Nyberg, A.Atac, A.Axelsson, R.A.Bark, J.Blomqvist, J.Cederkall, B.Cederwall, G.de Angelis, C.Fahlander, H.Grawe, A.Johnson, S.Leoni, A.Likar, M.Matiuzzi, S.Mitarai, L.-O.Norlin, M.Palacz, J.Persson, H.A.Roth, R.Schubart, D.Seweryniak, T.Shizuma, O.Skeppstedt, D.Sohler, G.Sletten, W.B.Walters, M.Weiszflog

In-Beam Study of 102Sn

NUCLEAR REACTIONS 50Cr(58Ni, 2nα), E=225 MeV; measured γ(particle)-, γγ-coin. 102Sn deduced transitions.

doi: 10.1007/s002180050174
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1996PA30      Nucl.Phys. A608, 227 (1996)

M.Palacz, J.Cederkall, M.Lipoglavsek, J.Persson, A.Atac, J.Blomqvist, H.Grawe, C.Fahlander, A.Johnson, A.Kerek, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, R.Schubart, D.Seweryniak, Z.Sujkowski, R.Wyss, G.de Angelis, P.Bednarczyk, Zs.Dombradi, D.Foltescu, D.Jerrestam, S.Juutinen, E.Makela, G.Perez, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen, T.Vass

In-Beam γ-Ray Spectroscopy of 101Cd

NUCLEAR REACTIONS 58Ni(50Cr, n2pα), E=261 MeV; measured γγ-coin, γγ(θ), γγ(t). 101Cd deduced high-spin levels, J, π, B(λ). Shell model calculations.

doi: 10.1016/S0375-9474(96)00287-4
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1996PE13      Acta Phys.Pol. B27, 171 (1996)

J.Persson, J.Cederkall, M.Lipoglavsek, M.Palacz, A.Atac, C.Fahlander, H.Grawe, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, R.Schubart, D.Seweryniak, G.De Angelis, P.Bednarczyk, Zs.Dombradi, D.Foltescu, D.Jerrestam, S.Juutinen, E.Makela, G.Perez, M.De Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen, T.Vass

New Spectroscopic Data on 102Cd

NUCLEAR REACTIONS 50Cr(58Ni, 2pα), E=261 MeV; measured particle gated projection γ spectra. 102Cd deduced levels, J, π, band structure, configuration.


1996RI09      Nucl.Phys. A599, 283c (1996)

A.Ringbom, G.Tibell, R.Zorro, J.Blomgren, H.Conde, K.Elmgren, S.Hultqvist, J.Nilsson, N.Olsson, C.Fahlander, L.Nilsson, J.Nyberg, D.Reistad, P.-U.Renberg, L.Westerberg, A.Likar, S.Wender

Studies of Giant Resonances by Heavy Ion Scattering at a Few Hundred MeV/Nucleon

NUCLEAR REACTIONS 40Ar(16O, 16O'), E=250 MeV/nucleon; measured spectra; deduced storage ring spectrometer resolution.

doi: 10.1016/0375-9474(96)00071-1
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1996RI19      Nucl.Instrum.Methods Phys.Res. A373, 57 (1996)

A.Ringbom, G.Tibell, R.Zorro, J.Blomgren, H.Conde, K.Elmgren, S.Hultqvist, J.Nilsson, N.Olsson, C.Fahlander, L.Nilsson, J.Nyberg, D.Reistad, P.-U.Renberg, L.Westerberg, A.Likar, S.Wender

A Facility for Studies of Giant Multipole Resonances by Fast Heavy-Ion Scattering

NUCLEAR REACTIONS 40Ar(16O, X), (16O, 16O'), E=250 MeV/nucleon; measured inelastic scattered particles spectra. 40Ar deduced structure near expected isovector dipole, isoscalar quadrupole giant resonances. One quandrant of the CELIUS storage ring as a spectrometer.

doi: 10.1016/0168-9002(95)01494-2
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1995CV01      J.Phys.(London) G21, 377 (1995)

F.Cvelbar, E.Betak, A.Likar

Pre-Equilibrium and Direct-Semi-Direct Model Calculations of Nucleon Radiative Capture Excitation Functions on Heavy Nuclei

NUCLEAR REACTIONS, ICPND 142Ce, 176Yb, 208Pb, 130Te(p, γ), 89Y, 208Pb, 140Ce(n, γ), E ≈ 4-24 MeV; analyzed σ(E). Preequilibrium, direct-semi-direct models, radiative capture.

doi: 10.1088/0954-3899/21/3/012
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1995LI31      Nucl.Phys. A591, 458 (1995)

A.Likar, T.Vidmar

Fast Neutron Capture Through a Consistent Version of the Direct-Semidirect Model

NUCLEAR REACTIONS 208Pb, 12C(n, γ), E ≈ 6-20 MeV; 40Ca(n, γ), E ≈ 5-45 MeV; 140Ce, 89Y(n, γ), E ≈ 1-20 MeV; calculated capture σ(θ) vs E. Direct-semidirect model, new version.

doi: 10.1016/0375-9474(95)00201-B
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1995LI32      Nucl.Phys. A591, 479 (1995)

A.Likar, T.Vidmar

Calculation of Fore-Aft Asymmetry of γ-Rays from Fast Neutron Capture in 40Ca

NUCLEAR REACTIONS 40Ca(n, γ), E ≈ 1-45 MeV; calculated σ(θ) fore-aft γ asymmetry vs E. Direct-semidirect capture model.

doi: 10.1016/0375-9474(95)00213-K
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1995LI33      Nucl.Phys. A593, 69 (1995)

A.Likar, T.Vidmar

Fast Proton Capture Through a Consistent Version of the Direct-Semdirect Model

NUCLEAR REACTIONS 40Ca(γ, p), E=14-24 MeV; 142Ce(p, γ), E=5-30 MeV; calculated σ(E). 209Bi(p, γ), E ≈ 9-18 MeV; calculated σ(θ) vs E. Direct-semidirect model.

doi: 10.1016/0375-9474(95)00340-7
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1993CV01      J.Phys.(London) G19, 1937 (1993)

F.Cvelbar, E.Betak, A.Likar

Pre-Equilibrium and Direct-Semi-Direct Model Calculations of Proton Radiative Capture Excitation Functions Near A = 60

NUCLEAR REACTIONS, ICPND 56Fe, 58,60,61Ni, 59Co, 63Cu, 64Zn(p, γ), E ≤ 24 MeV; calculated σ(E). Preequilibrium, direct-semidirect models, radiative capture.

doi: 10.1088/0954-3899/19/11/020
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1990HA21      Nucl.Phys. A512, 399 (1990)

A.Hakansson, J.Blomgren, A.Likar, A.Lindholm, L.Nilsson, N.Olsson, R.Zorro

The Isovector E2 Resonance in Bismuth Excited by Neutron Radiative Capture

NUCLEAR REACTIONS 209Bi(n, γ), E=17.7-22 MeV; measured γ-spectra, fore-aft asymmetry. 210Bi deduced isovector quadrupole resonance, Γ, EWSR. Direct-semidirect model.

doi: 10.1016/0375-9474(90)90078-Z
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1987ZO02      Nucl.Phys. A472, 125 (1987)

R.Zorro, I.Bergqvist, S.Crona, A.Hakansson, A.Likar, A.Lindholm, L.Nilsson, N.Olsson

The Isovector Quadrupole Resonance in Yttrium Excited by Neutron Radiative Capture

NUCLEAR REACTIONS 89Y(n, γ), E=12-27 MeV; measured γ-spectra, asymmetry. 90Y deduced isovector quadrupole resonance, Γ, EWSR. Direct-semidirect model.

doi: 10.1016/0375-9474(87)90223-5
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1984BE25      Nucl.Phys. A419, 509 (1984)

I.Bergqvist, R.Zorro, A.Hakansson, A.Lindholm, L.Nilsson, N.Olsson, A.Likar

The Giant Isovector E2 Resonance in Calcium Observed in Radiative Neutron Capture

NUCLEAR REACTIONS 40Ca(n, γ), E=7-28 MeV; measured σ(θ) vs E, γ asymmetry. 41Ca deduced isovector GQR parameters, E1, E2 interference. Direct-semidirect capture model.

doi: 10.1016/0375-9474(84)90629-8
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1984LI10      Z.Phys. A317, 149 (1984)

A.Lindholm, L.Nilsson, I.Bergqvist, R.Zorro, N.Olsson, B.Castel, A.Likar

Fast Neutron Radiative Capture in Silicon

NUCLEAR REACTIONS 28Si(n, γ), E=3-14 MeV; measured σ(θ=90°) vs E; deduced reaction mechanism. 29Si deduced GDR, GQR interference channel dependence. Compound nucleus, direct-semidirect, continuum shell model analyses.

doi: 10.1007/BF01421249
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1981CV02      Fizika(Zagreb) 13, Suppl.No.2, 16 (1981)

F.Cvelbar, R.Martincic, A.Likar

Sensitivity of the Direct-Semidirect Model Calculations of the Integrated Neutron Capture Cross Section on the Exactness of the Final State Wave Function

NUCLEAR REACTIONS 89Y, 140Ce, 208Pb(n, γ), E not given; calculated integrated σ(E). Direct semi-direct capture model.


1980LI17      Nucl.Phys. A350, 74 (1980)

A.Likar, R.Martincic

Fast Neutron Capture in 208Pb as Seen Through Direct-Semidirect and Pure Resonance Models

NUCLEAR REACTIONS 208Pb(n, γ), E=8-32 MeV; calculated σ(total, E), γ(θ). Resonance, DSD models.

doi: 10.1016/0375-9474(80)90389-9
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1979LI09      Nucl.Phys. A321, 306 (1979)

A.Likar, R.Martincic

Proton Excitation of the Isovector Giant Quadrupole Resonance in 208Pb

NUCLEAR REACTIONS 208Pb(p, γ), 20 MeV ≤ E ≤ 30 MeV; calculated σ(θ). Direct-semidirect model, dipole, quadrupole, octupole interference effects.

doi: 10.1016/0375-9474(79)90128-3
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1978CV01      Fizika, Suppl. 10, 31 (1978)

F.Cvelbar, A.Likar, R.Martincic, F.Sever

Recent Studies of the Radiative Nucleon Capture in the Region of GDR

NUCLEAR REACTIONS 39K(p, γ), E=6-20 MeV; 40Ca, 88Sr, 89Y(n, γ), E not given; 40Ca(γ, p), E not given; analyzed data; deduced reaction mechanism, GDR excitation.


1978LI03      Nuclear Phys. A295, 405 (1978)

A.Likar, F.Sever

Semidirect Model Calculations of Differential Cross Sections for Some Photonuclear Reactions in 40Ca

NUCLEAR REACTIONS 40Ca(γ, p), (γ, n); calculated σ.

doi: 10.1016/0375-9474(78)90183-5
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1978LI07      Nucl.Phys. A298, 217 (1978)

A.Likar, A.Lindholm, L.Nilsson, I.Bergqvist, B.Palsson

Angular Distributions of γ-Rays from Fast Neutron Capture in Strontium and Yttrium

NUCLEAR REACTIONS 88Sr, 89Y(n, γ), E=7-11 MeV; measured Iγ(E, θ) in GDR, GQR region. Direct-semidirect (dsd) model analysis.

doi: 10.1016/0375-9474(78)90253-1
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1978LI20      Nucl.Phys. A307, 77 (1978)

A.Likar, F.Sever, R.Martincic

Fast Proton Capture in 208Pb According to Direct-Semidirect Model

NUCLEAR REACTIONS 208Pb(p, γ), E=10-30 MeV; calculated σ(E).

doi: 10.1016/0375-9474(78)90428-1
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1977LI08      Nucl.Phys. A280, 49 (1977)

A.Likar, M.Potokar, F.Cvelbar

Angular Distribution of γ-Rays from the Radiative Capture of Fast Nucleons

NUCLEAR REACTIONS 88Sr, 40Ca, 208Pb(n, γ), E=4-20 MeV; 39K, 64Ni(p, γ), E < 25 MeV; calculated γ(θ) coefficient.

doi: 10.1016/0375-9474(77)90292-5
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1977PO01      Nucl.Phys. A277, 29 (1977)

M.Potokar, A.Likar, M.Budnar, F.Cvelbar

Analysis of Fast Neutron Capture Data Based on the Refined Direct-Semidirect Model

NUCLEAR REACTIONS 208Pb, 88Sr, 40Ca, 89Y(n, γ), E ≈ 14 MeV; calculated σ.

doi: 10.1016/0375-9474(77)90260-3
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1975LI26      Fizika 7, 157 (1975)

A.Likar, M.Potokar, F.Cvelbar

Angular Distribution of Neutron Capture γ-Rays in the Semidirect Capture Model

NUCLEAR REACTIONS 40Ca, 207Pb(n, γ), E < 20 MeV; calculated angular distribution in GDR region.


1973PO14      Nucl.Phys. A213, 525 (1973)

M.Potokar, A.Likar, F.Cvelbar, M.Budnar, E.R.Hodgson

The Radiative Capture of 14.1 MeV Neutrons in 138Ba, W, Pb and 209Bi

NUCLEAR REACTIONS 138Ba, W, Pb, 209Bi(n, γ), E=14.1 MeV; measured σ(Eγ). Natural targets.

doi: 10.1016/0375-9474(73)90751-3
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30185.


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