NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = T.Vertse Found 69 matches. 2018ID02 Phys.Rev. C 97, 024307 (2018) R.M.Id Betan, A.T.Kruppa, T.Vertse Shadow poles in coupled-channel problems calculated with the Berggren basis NUCLEAR STRUCTURE 5He; calculated locations of the poles of the S matrix for the Cox potential for 3/2+ resonant state of 5He formed in t+d -> α+n fusion reaction using phenomenological two-channel model and Berggren basis for expanding the coupled-channels solutions; deduced shadow pole of 5He migrates between Riemann sheets when the coupling strength is varied.
doi: 10.1103/PhysRevC.97.024307
2017SA40 Eur.Phys.J. A 53, 152 (2017) Smoothed square well potential NUCLEAR STRUCTURE A>208; calculated single-particle neutron levels, J, π using CWS (Cut-off Woods-Saxon), SV (Salamon-Vertse), SSQW (Smoothed SQuare Well) potentials.
doi: 10.1140/epja/i2017-12342-2
2016SA19 Nucl.Phys. A952, 1 (2016) Distributions of the S-matrix poles in Woods-Saxon and cut-off Woods-Saxon potentials
doi: 10.1016/j.nuclphysa.2016.04.010
2015BA32 Eur.Phys.J. A 51, 76 (2015) A.Baran, Cs.Noszaly, P.Salamon, T.Vertse Calculating broad neutron resonances in a cut-off Woods-Saxon potential NUCLEAR REACTIONS 208Pb(n, x), E not given; calculated resonance pole trajectories using CWS (cut-off Woods Saxon) potential.
doi: 10.1140/epja/i2015-15076-1
2014SA32 Phys.Rev. C 89, 054609 (2014) P.Salamon, R.G.Lovas, R.M.Id Betan, T.Vertse, L.Balkay Strictly finite-range potential for light and heavy nuclei
doi: 10.1103/PhysRevC.89.054609
2011RA29 Phys.Rev. C 84, 037602 (2011) Trajectories of S-matrix poles in a new finite-range potential NUCLEAR STRUCTURE 16O, 208Pb; calculated radial shapes, trajectories of resonant poles. Finite-range Phenomenological potential model.
doi: 10.1103/PhysRevC.84.037602
2010SA13 Phys.Rev. C 81, 064322 (2010) P.Salamon, A.T.Kruppa, T.Vertse New method for calculating shell correction NUCLEAR STRUCTURE 16,18,20,22,24O, 20Ne, 40,48Ca, 68,78Ni, 90,122,124Zr, 100,132Sn, 146Gd, 180,208Pb; calculated neutron shell corrections using the smoothed finite-range weight function and the generalized Strutinski procedure. Comparison with the semiclassical shell correction.
doi: 10.1103/PhysRevC.81.064322
2009DU16 Phys.Rev. C 80, 064311 (2009) G.G.Dussel, R.Id Betan, R.J.Liotta, T.Vertse Collective excitations in the continuum NUCLEAR STRUCTURE 208,210Pb, 210Po, 210Bi; calculated giant pairing (particle-particle and particle-hole) resonance (GPR) wave functions using shell-model formalism in the complex energy plane. NUCLEAR REACTIONS 208Pb(3He, n), E=100 MeV; calculated σ(θ) for two-particle transfer to GPR in 210Po using optical potential model.
doi: 10.1103/PhysRevC.80.064311
2009MI01 J.Phys.(London) G36, 013101 (2009) M.Michel, W.Nazarewicz, M.Ploszajczak, T.Vertse Shell model in the complex energy plane
doi: 10.1088/0954-3899/36/1/013101
2008ID01 Phys.Rev. C 78, 044308 (2008) R.Id Betan, A.T.Kruppa, T.Vertse Complex energy approaches for calculating isobaric analogue states
doi: 10.1103/PhysRevC.78.044308
2008SA12 Phys.Rev. C 77, 037302 (2008) New simple form for a phenomenological nuclear potential
doi: 10.1103/PhysRevC.77.037302
2007DU23 Nucl.Phys. A789, 182 (2007) G.G.Dussel, R.Id Betan, R.J.Liotta, T.Vertse One- and two-quasiparticle states in the complex energy plane
doi: 10.1016/j.nuclphysa.2007.04.005
2006ID01 Nucl.Phys. A771, 93 (2006) R.Id Betan, N.Sandulescu, T.Vertse Quasiparticle resonances in the BCS approach NUCLEAR STRUCTURE 17O, 79Ni; calculated single-particle states; 20,22O, 84Ni; calculated pairing energies, radii, single-particle states, quasiparticle resonances. Berggren representation.
doi: 10.1016/j.nuclphysa.2006.03.003
2006RE02 Phys.Rev. C 73, 014309 (2006) P.-G.Reinhard, M.Bender, W.Nazarewicz, T.Vertse From finite nuclei to the nuclear liquid drop: Leptodermous expansion based on self-consistent mean-field theory
doi: 10.1103/PhysRevC.73.014309
2005ID01 J.Phys.(London) G31, S1329 (2005) R.Id Betan, R.J.Liotta, N.Sandulescu, T.Vertse Description of the continuum part of the spectrum by using the complex energy plane NUCLEAR STRUCTURE 80Ni; calculated resonance energies, continuum features. 11Li; calculated ground state wave function, resonance and halo features. Complex energy plane.
doi: 10.1088/0954-3899/31/8/011
2005ID02 Phys.Rev. C 72, 054322 (2005) R.Id Betan, R.J.Liotta, N.Sandulescu, T.Vertse, R.Wyss Complex shell model representation including antibound states NUCLEAR STRUCTURE 11Li, 72Ca; calculated ground and excited states energies, two-particle wave functions; deduced halo features. Shell model formalism with antibound states.
doi: 10.1103/PhysRevC.72.054322
2004ID01 Phys.Lett. B 584, 48 (2004) R.Id Betan, R.J.Liotta, N.Sandulescu, T.Vertse A shell model representation with antibound states NUCLEAR STRUCTURE 11Li, 72Ca; calculated two-particle resonance features, role of antibound states.
doi: 10.1016/j.physletb.2004.01.042
2004ID02 Few-Body Systems 34, 51 (2004) R.Id Betan, R.J.Liotta, N.Sandulescu, T.Vertse Two-Particle Resonances in the Complex Energy Plane NUCLEAR STRUCTURE 11Li; calculated resonance energies.
doi: 10.1007/s00601-004-0028-4
2003ID01 Phys.Rev. C 67, 014322 (2003) R.Id Betan, R.J.Liotta, N.Sandulescu, T.Vertse Shell model in the complex energy plane and two-particle resonances NUCLEAR STRUCTURE 78Ni, 100Sn; calculated single-particle states, two-particle resonance features. Shell model in the complex energy plane.
doi: 10.1103/PhysRevC.67.014322
2003ID03 Acta Phys.Hung.N.S. 18, 267 (2003) R.Id Betan, R.J.Liotta, N.Sandulescu, T.Vertse Clusters as Many-Body Resonances NUCLEAR STRUCTURE 80Ni; calculated two-particle resonance energies.
doi: 10.1556/APH.18.2003.2-4.24
2003KR22 Acta Phys.Pol. B34, 2315 (2003) W.Krolas, R.Grzywacz, K.P.Rykaczewski, J.C.Batchelder, C.R.Bingham, C.J.Gross, D.Fong, J.H.Hamilton, D.J.Hartley, J.K.Hwang, Y.Larochelle, T.A.Lewis, K.H.Maier, J.W.McConnell, A.Piechaczek, A.V.Ramayya, K.Rykaczewski, D.Shapira, M.N.Tantawy, J.A.Winger, C.-H.Yu, E.F.Zganjar, A.T.Kruppa, W.Nazarewicz, T.Vertse First observation of excited states in 140Dy NUCLEAR REACTIONS 92Mo(54Fe, 4n2p), E=315 MeV; measured Eγ, Iγ, γγ-, (recoil)γ-coin; deduced σ. 140Dy deduced levels, J, π, isomer T1/2. Level systematics in neighboring nuclides discussed.
2002ID01 Phys.Rev.Lett. 89, 042501 (2002) R.Id Betan, R.J.Liotta, N.Sandulescu, T.Vertse Two-Particle Resonant States in a Many-Body Mean Field NUCLEAR STRUCTURE 80Ni; calculated two-particle resonance energies. Berggren representation.
doi: 10.1103/PhysRevLett.89.042501
2002KR04 Phys.Rev. C65, 031303 (2002) W.Krolas, R.Grzywacz, K.P.Rykaczewski, J.C.Batchelder, C.R.Bingham, C.J.Gross, D.Fong, J.H.Hamilton, D.J.Hartley, J.K.Hwang, Y.Larochelle, T.A.Lewis, K.H.Maier, J.W.McConnell, A.Piechaczek, A.V.Ramayya, K.Rykaczewski, D.Shapira, M.N.Tantawy, J.A.Winger, C.-H.Yu, E.F.Zganjar, A.T.Kruppa, W.Nazarewicz, T.Vertse First Observation of the Drip Line Nucleus 140Dy: Identification of a 7 μs K Isomer Populating the Ground State Band NUCLEAR REACTIONS 92Mo(54Fe, 2nα), E=315 MeV; measured delayed Eγ, Iγ, γγ-, (X-ray)γ-, (recoil)γ-coin. 140Dy deduced isomer J, π, T1/2, configuration. Mass separator, comparisons with model predictions. Level systematics in neighboring nuclides discussed. RADIOACTIVITY 141Ho(p); calculated proton decay branching ratios, fine structure features.
doi: 10.1103/PhysRevC.65.031303
2002NA18 Nucl.Phys. A701, 165c (2002) W.Nazarewicz, M.Bender, S.Cwiok, P.H.Heenen, A.T.Kruppa, P.-G.Reinhard, T.Vertse Theoretical Description of Superheavy Nuclei NUCLEAR STRUCTURE 257No, 261Rf, 265Sg, 269Hs, 271Ds, 277Cn; calculated levels, J, π, Qα. Z=120; calculated neutron shell correction energies. Skyrme-Hartree-Fock and relativistic mean-field calculations.
doi: 10.1016/S0375-9474(01)01567-6
2001BA26 Nucl.Phys. A682, 256c (2001) B.Barmore, A.T.Kruppa, W.Nazarewicz, T.Vertse A New Approach to Deformed Proton Emitters: Non-adiabatic coupled-channels
doi: 10.1016/S0375-9474(00)00648-5
2001CI07 Phys.Rev. C64, 057305 (2001) O.Civitarese, R.J.Liotta, T.Vertse Temperature Dependent BCS-Gap Equations in the Continuum NUCLEAR STRUCTURE Z=50-112; calculated quasiparticle energies, pair gaps for N=50, 114. 106Ba, 204Th; calculated pair gap vs temperature. Suitability of BCS method near proton drip line discussed.
doi: 10.1103/PhysRevC.64.057305
2000BB02 Phys.Rev. C62, 054315 (2000) B.Barmore, A.T.Kruppa, W.Nazarewicz, T.Vertse Theoretical Description of Deformed Proton Emitters: Nonadiabatic coupled-channel method RADIOACTIVITY 109I, 113Cs, 117La, 131Eu, 141,141mHo(p); calculated proton decay T1/2, branching ratios. Nonadiabatic coupled-channels method, comparison with data.
doi: 10.1103/PhysRevC.62.054315
2000KR03 Phys.Rev. C61, 034313 (2000) A.T.Kruppa, M.Bender, W.Nazarewicz, P.-G.Reinhard, T.Vertse, S.Cwiok Shell Corrections of Superheavy Nuclei in Self-Consistent Calculations NUCLEAR STRUCTURE Z=120; calculated neutron single-particle levels, shell corrections. Z=110-130; calculated proton shell corrections, macroscopic energies. Self-consistent Skyrme-Hartree-Fock and relativistic mean field calculations.
doi: 10.1103/PhysRevC.61.034313
2000KR07 Phys.Rev.Lett. 84, 4549 (2000) A.T.Kruppa, B.Barmore, W.Nazarewicz, T.Vertse Fine Structure in the Decay of Deformed Proton Emitters: Nonadiabatic approach RADIOACTIVITY 131Eu, 141Ho, 141mHo(p); calculated T1/2, ground and first excited state branching ratios. Comparison with data, solution of Schroedinger equation in complex energy plane.
doi: 10.1103/PhysRevLett.84.4549
2000VE03 Phys.Rev. C61, 064317 (2000) T.Vertse, A.T.Kruppa, W.Nazarewicz Shell Corrections for Finite-Depth Deformed Potentials: Green's function oscillator expansion method NUCLEAR STRUCTURE 298Fl, 132,154Sn, 100,110,120Zr; calculated shell corrections, related quantities. Green's function oscillator expansion method, Woods-Saxon potential, generalized Strutinsky smoothing procedure.
doi: 10.1103/PhysRevC.61.064317
1999RY04 Phys.Rev. C60, 011301 (1999) K.Rykaczewski, J.C.Batchelder, C.R.Bingham, T.Davinson, T.N.Ginter, C.J.Gross, R.Grzywacz, M.Karny, B.D.MacDonald, J.F.Mas, J.W.McConnell, A.Piechaczek, R.C.Slinger, K.S.Toth, W.B.Walters, P.J.Woods, E.F.Zganjar, B.Barmore, L.Gr.Ixaru, A.T.Kruppa, W.Nazarewicz, M.Rizea, T.Vertse Proton Emitters 140Ho and 141Ho: Probing the structure of unbound Nilsson orbitals NUCLEAR REACTIONS 92Mo(54Fe, xnp)140Ho/141Ho/141mHo, E=315 MeV; measured proton spectra following residual nucleus decay, (recoil)(decay)-coin; deduced production σ. RADIOACTIVITY 140,141mHo(p) [from 92Mo(54Fe, xnp)]; measured Ep, T1/2. 140,141Ho deduced proton resonance features, configurations, deformation effects. Coupled-channels analysis.
doi: 10.1103/PhysRevC.60.011301
1998DE05 Phys.Rev. C57, 986 (1998) D.S.Delion, R.J.Liotta, N.Sandulescu, T.Vertse Probing Monopole Double Giant Resonances by Dilepton (E0) Emission NUCLEAR STRUCTURE 208Pb; calculated two-particle plus two-hole levels, partial decay widths; deduced continuum coupling role, monopole, double giant resonances decay features.
doi: 10.1103/PhysRevC.57.986
1998VE02 Phys.Rev. C57, 3089 (1998) T.Vertse, A.T.Kruppa, R.J.Liotta, W.Nazarewicz, N.Sandulescu, T.R.Werner Shell Corrections for Finite Depth Potentials: Particle continuum effects NUCLEAR STRUCTURE 78Ni, 90,96,104,106,108,110,122Zr, 124Zr, 132Sn, 146Gd, 208Pb, 298Fl; calculated neutron shell correction energies. 48Ni, 90Zr, 100,132Sn, 146Gd, 180,208Pb; calculated proton shell correction energies. 146Gd, 208Pb calculated smoothed level densities. Smoothing procedure with particle continuum contribution.
doi: 10.1103/PhysRevC.57.3089
1997SA08 Phys.Rev. C55, 1250 (1997) N.Sandulescu, O.Civitarese, R.J.Liotta, T.Vertse Effects Due to the Continuum on Shell Corrections at Finite Temperatures NUCLEAR STRUCTURE 208Pb; calculated neutrons shell correction to free energy; deduced corrections wash out temperature. Extension of Strutinsky method, finite depth mean field potential continuum spectrum included.
doi: 10.1103/PhysRevC.55.1250
1996BL05 Phys.Rev. C53, 2001 (1996) J.Blomqvist, O.Civitarese, E.D.Kirchuk, R.J.Liotta, T.Vertse Feeding of Hole States by Proton Decay of Gamow-Teller and Isobaric Analog State Resonances NUCLEAR STRUCTURE 209Bi; calculated Gamow-Teller, IAR proton decay partial widths. RPA, Breggren representation.
doi: 10.1103/PhysRevC.53.2001
1996FO09 Phys.Rev. C54, 3279 (1996) S.Fortunato, A.Insolia, R.J.Liotta, T.Vertse Two-Particle - One-Hole Excitations in the Continuum NUCLEAR STRUCTURE 209Bi; calculated i11/2, j15/2 states strength function. 209Pb; calculated neutron decay associated branching ratios. Resonant multi-step shell model method.
doi: 10.1103/PhysRevC.54.3279
1996LI08 Nucl.Phys. A599, 327c (1996) R.J.Liotta, E.Maglione, T.Vertse Microscopic Structure and Decay Characteristics of Giant Resonances NUCLEAR STRUCTURE 208Pb; calculated monopole, dipole, quadrupole resonances, sum rule exhaustion, decay (in some cases) features. Continuum RPA.
doi: 10.1016/0375-9474(96)00075-9
1996LI57 Phys.Lett. 367B, 1 (1996) R.J.Liotta, E.Maglione, N.Sandulescu, T.Vertse A Representation to Describe Nuclear Processes in the Continuum
doi: 10.1016/0370-2693(95)01415-2
1995VE02 Nucl.Phys. A584, 13 (1995) T.Vertse, R.J.Liotta, E.Maglione Exact and Approximate Calculation of Giant Resonances NUCLEAR STRUCTURE 208Pb; calculated giant resonances, decay widths, energy weighted sum rules. Exact, approximate approaches.
doi: 10.1016/0375-9474(94)00502-E
1994LI68 Z.Phys. A347, 231 (1994) P.Lind, R.J.Liotta, E.Maglione, T.Vertse Resonant State Expansions of the Continuum
doi: 10.1007/BF01289789
1993LE13 Phys.Rev. C48, 1463 (1993) S.M.Lenzi, O.Dragun, E.E.Maqueda, R.J.Liotta, T.Vertse Description of Alpha Clustering Including Continuum Configuration NUCLEAR STRUCTURE 212Po; calculated α-cluster formation amplitude vs radius; deduced clustering can be described beyond daughter nucleus surface.
doi: 10.1103/PhysRevC.48.1463
1993MA01 Phys.Lett. 298B, 1 (1993) E.Maglione, R.J.Liotta, T.Vertse Partial Decay Widths from Giant Resonances in 208Pb NUCLEAR STRUCTURE 208Pb; calculated giant resonance partial decay width. Continuum RPA.
doi: 10.1016/0370-2693(93)91695-J
1992DU03 Phys.Rev. C46, 558 (1992) G.G.Dussel, R.J.Liotta, H.Sofia, T.Vertse Temperature Dependent Resonant Random Phase Approximation NUCLEAR STRUCTURE 208Pb; calculated giant resonance escape widths; deduced thermal fluctuations role. Temperature dependent, resonant RPA.
doi: 10.1103/PhysRevC.46.558
1990VE15 Phys.Rev. C42, 2605 (1990) T.Vertse, P.Curutchet, R.J.Liotta Approximate Treatment of the Continuum NUCLEAR STRUCTURE Z=82; calculated single particle, particle-hole response functions. Square well plus Coulomb potential, Green function pole expansion.
doi: 10.1103/PhysRevC.42.2605
1989CU01 Phys.Rev. C39, 1020 (1989) P.Curutchet, T.Vertse, R.J.Liotta Resonant Random Phase Approximation NUCLEAR STRUCTURE 208Pb; calculated multipole giant resonace excitation. Resonant RPA.
doi: 10.1103/PhysRevC.39.1020
1989VE09 Acta Phys.Acad.Sci.Hung. 65, 305 (1989) T.Vertse, P.Curutchet, R.J.Liotta, J.Bang On the Role of Anti-Bound States in the RPA Description of the Giant Monopole Resonance NUCLEAR STRUCTURE 16O; calculated giant monopole resonance escape widths. Resonant RPA.
1988VE02 Phys.Rev. C37, 876 (1988) T.Vertse, P.Curutchet, O.Civitarese, L.S.Ferreira, R.J.Liotta Application of Gamow Resonances to Continuum Nuclear Spectra NUCLEAR STRUCTURE 208Pb; calculated neutron, proton Gamow resonances.
doi: 10.1103/PhysRevC.37.876
1987DR11 Z.Phys. A328, 61 (1987) O.Dragun, R.J.Liotta, T.Vertse Study of Pairing Deformations by Means of Two-Particle Transfer Reactions NUCLEAR REACTIONS 208Pb(16O, 18O), E=69, 73, 86 MeV; 208Pb(p, t), E=22-80 MeV; 64Ni(16O, 18O), E=50, 57, 65 MeV; 58,60Ni(16O, 18O), E=50, 57, 60 MeV; 60Ni(p, t), E=27 MeV; 62Ni(p, t), E=27-46.5 MeV; 204,206Pb(p, t), E=26, 30 MeV; analyzed σ(θ); deduced pairing deformation parameters. 208Pb(16O, 12C), E=93 MeV; analyzed σ(θ); deduced model applicability. Macroscopic DWBA.
1986BA63 Z.Phys. A325, 399 (1986) V.Barci, H.El-Samman, A.Gizon, J.Gizon, R.Kossakowski, B.M.Nyako, T.Vertse, S.Elfstrom, D.Jerrestam, W.Klamra, Th.Lindblad, T.Bengtsson Effective Moment of Inertia in 132Ce, 134Nd and 136Nd NUCLEAR STRUCTURE 132Ce, 134,136Nd; calculated effective moments of inertia. Cranking Nilsson-Strutinsky model. NUCLEAR REACTIONS 96Zr, 98,100Mo(40Ar, X), E=160-189 MeV; measured continuum Eγ, Iγ, σ(Eγ, E), γ(θ). 132Ce, 134,136Nd deduced moments of inertia. NaI(Tl) detectors. Cranking Nilsson-Strutinsky model.
1986HE02 Nucl.Phys. A448, 441 (1986) M.W.Herzog, O.Civitarese, L.Ferreira, R.J.Liotta, T.Vertse, L.J.Sibanda Two-Particle Transfer Reactions Leading to Giant Pairing Resonances NUCLEAR REACTIONS 208Pb(3He, n), E=33 MeV; 208Pb(t, p), E=20-100 MeV; calculated residual level relative σ, integrand function vs θ. NUCLEAR STRUCTURE 210Pb; calculated ground state, pairing giant resonance pairing density function. 210Po; calculated two-particle wave functions, low-lying levels.
doi: 10.1016/0375-9474(86)90337-4
1985HE26 Phys.Lett. 165B, 35 (1985) M.W.Herzog, R.J.Liotta, T.Vertse Hole Pairing Giant Resonance NUCLEAR REACTIONS 208Pb(p, t), E ≈ 20-100 MeV; calculated residual 0+ state relative excitation σ. 206Pb deduced hole pairing giant resonance. Two-hole pairing collective TDA.
doi: 10.1016/0370-2693(85)90685-9
1984HI02 Phys.Scr. 29, 47 (1984) L.Hildingsson, J.Bialkowski, J.Gizon, S.A.Hjorth, D.Jerrestam, A.Johnson, W.Klamra, Th.Lindblad, T.Vertse Gamma-Gamma Energy Correlation Studies in Cerium Isotopes NUCLEAR REACTIONS 122,128,130Te(12C, xn), E=100 MeV; measured γγ-energy correlation. 130,134,136Ce deduced high-spin state γ-decay characteristics.
doi: 10.1088/0031-8949/29/1/007
1984KL11 Nucl.Phys. A431, 367 (1984) W.Klamra, J.Bialkowski, L.Hildingsson, D.Jerrestam, A.Johnson, J.Kownacki, Th.Lindblad, J.Nyberg, T.Vertse, T.Bengtsson Experimental Moments of Inertia in Pd and Cd Isotopes and Their Interpretation with the Extended Nilsson-Strutinsky Model NUCLEAR REACTIONS 100Mo(12C, xnypzα), E=118 MeV; measured γγ-coin, γ-multiplicity; deduced energy-energy correlation spectrum. 104,106Pd, 106Cd deduced moment of inertia, high-spin state properties, configurations.
doi: 10.1016/0375-9474(84)90180-5
1983PA06 Nucl.Phys. A402, 114 (1983) K.F.Pal, R.G.Lovas, M.A.Nagarajan, B.Gyarmati, T.Vertse Microscopic Description of 7Li and 7Be for the DWBA Treatment of Cluster Transfer Reactions NUCLEAR REACTIONS 12C(7Li, t), E=34 MeV; calculated σ(θ); deduced potential parameters. Finite range DWBA, generator coordinate cluster for projectile, schematic nucleon-nucleon forces.
doi: 10.1016/0375-9474(83)90564-X
1982GY02 Phys.Rev. C26, 2674 (1982) Shape of the α Potentials in the Distorted-Wave Born Approximation Description of α Transfer NUCLEAR REACTIONS 16O(6Li, d), E=20, 75.4 MeV; calculated σ(θ). 20Ne levels deduced relative σ. Exact finite-range DWBA, different α-particle form factors.
doi: 10.1103/PhysRevC.26.2674
1982KL10 Nucl.Phys. A391, 184 (1982) W.Klamra, J.Bialkowski, C.J.Herrlander, L.Hildingsson, D.Jerrestam, A.Johnson, A.Kerek, J.Kownacki, A.Kallberg, Th.Lindblad, C.G.Linden, T.Vertse Gamma-Gamma Energy Correlations and Moment of Inertia in Light Xe Isotopes NUCLEAR REACTIONS 114,116Cd(12C, xn), E=118 MeV; measured γγ-coin; deduced energy-energy correlation spectra. 118,120,122Xe deduced moment of inertia.
doi: 10.1016/0375-9474(82)90226-3
1982LI05 Nucl.Phys. A378, 364 (1982) Th.Lindblad, L.Hildingsson, D.Jerrestam, A.Kallberg, A.Johnson, C.J.Herrlander, W.Klamra, A.Kerek, C.G.Linden, J.Kownacki, J.Bialkowski, T.Vertse On the Moment of Inertia in Deformed Ba-Xe Nuclei as Deduced from Gamma-Gamma Energy Correlation Experiments NUCLEAR REACTIONS 114,116,118,120,122Sn(12C, xn), (12C, αxn), E=118 MeV; measured γγ-coin; deduced energy-energy correlation spectra, moment of inertia.
doi: 10.1016/0375-9474(82)90599-1
1981AP02 Acta Phys.Acad.Sci.Hung. 51, 171 (1981) DWBA Calculation of the Cross Section of the 12C(6Li, d)16O [O+2, 6.05 MeV] Reaction NUCLEAR REACTIONS 12C(6Li, d), E=18 MeV; analyzed σ(θ). 16O level deduced Sα, normalization. Exact finite-range DWBA analysis.
doi: 10.1007/BF03155575
1981BI02 Nucl.Phys. A357, 261 (1981) J.Bialkowski, B.Fant, C.J.Herrlander, L.Hildingsson, A.Johnson, W.Klamra, J.Kownacki, A.Kallberg, Th.Lindblad, C.G.Linden, T.Lonnroth, J.Sztarkier, T.Vertse, K.Wikstrom Gamma-Gamma Energy Correlations and Moment of Inertia in 130Ce NUCLEAR REACTIONS 124Te(12C, 6n), E=118 MeV; measured γγ-coin; deduced energy-energy correlation spectrum. 130Ce deduced collective moment of inertia.
doi: 10.1016/0375-9474(81)90638-2
1981GY01 Phys.Lett. 104B, 177 (1981) On the Shape of the Alpha-Potential in Direct Alpha-Transfer NUCLEAR REACTIONS 16O(6Li, d), E=20 MeV; 16O(α, α), E=23.2 MeV; calculated σ(θ); deduced alpha potential shape independence. DWBA, alpha transfer.
doi: 10.1016/0370-2693(81)90585-2
1981GY02 J.Phys.(London) G7, L209 (1981) B.Gyarmati, R.G.Lovas, T.Vertse, P.E.Hodgson Low-Energy Behaviour of the Real Depth of the Proton Optical Potential NUCLEAR REACTIONS 116Sn(p, p), (n, n), E=5-25 MeV; calculated σ(E); deduced collective effects on optical potential real term energy dependence. Model calculation, elastic to inelastic channel coupling.
doi: 10.1088/0305-4616/7/9/005
1980AP02 Phys.Rev. C21, 779 (1980) Configuration Mixing Effect in the 12C(6Li, d)16O* α-Transfer Reaction NUCLEAR REACTIONS 12C(6Li, d), E=18, 20, 28 MeV; calculated σ(θ). 16O levels deduced configuration mixing. Zero range DWBA, CCBA, microscopic form factors.
doi: 10.1103/PhysRevC.21.779
1979GY02 J.Phys.(London) G5, 1225 (1979) B.Gyarmati, T.Vertse, L.Zolnai, A.I.Baryshnikov, A.F.Gurbich, N.N.Titarenko, E.L.Yadrovsky Low-Energy Behaviour of the Proton Optical Potential of Sn NUCLEAR REACTIONS 116,120Sn(p, p), E=4-9 MeV; measured σ(θ); deduced optical-model parameters, energy dependence of real depth.
doi: 10.1088/0305-4616/5/9/007
1976GY01 ATOMKI Kozlem. 18, 31 (1976) B.Gyarmati, T.Vertse, G.Y.Tertychny, E.L.Yadrovsky On the Complex Optical Potential in the Lane-Model NUCLEAR STRUCTURE 209Bi; calculated IAR in microscopic model, Lane model.
1976VA20 Nucl.Phys. A270, 200 (1976) A.Valek, T.Vertse, B.Schlenk, I.Hunyadi A Study of the 14N(d, p)15N Reaction at Low Bombarding Energies NUCLEAR REACTIONS 14N(d, p), E=.309-.638 MeV; measured σ(E, Ep, θ). 15N levels deduced astrophysical S(E). Natural target.
doi: 10.1016/0375-9474(76)90135-4
1974VE03 Nucl.Phys. A223, 207 (1974) T.Vertse, A.Dudek-Ellis, P.J.Ellis, T.A.Belote, D.Roaf Inelastic Processes in the 19F(3He, d)20Ne Reaction NUCLEAR REACTIONS 19F(3He, d), (3He, 3He'), (3He, 3He), E=16.00 MeV; measured σ(Ed, θ), σ(E(3He), θ). 20Ne levels deduced effect of inelastic processes on S.
doi: 10.1016/0375-9474(74)90287-5
1972GY01 Nucl.Phys. A182, 315 (1972) Easy Method for Calculating the Resonance Parameters of the Isobaric Analogue Resonance NUCLEAR REACTIONS 208Pb(p, p), analyzed isobaric analog resonances. 209Bi deduced isobaric analog resonance parameters.
doi: 10.1016/0375-9474(72)90280-1
1972GY02 Phys.Lett. 41B, 110 (1972) B.Gyarmati, F.Krisztinkovics, T.Vertse On the Expectation Value in Gamow State
doi: 10.1016/0370-2693(72)90438-8
1971VE11 Fiz.Szemble 21, 142 (1971) Az Isobar Analog Rezonanciak Fenomenologikus Leirasa
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