NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = I.Rotter Found 42 matches. 2004RO25 Acta Phys.Pol. B35, 1269 (2004) Extension of R Matrix Theory
2001RO24 Phys.Rev. C64, 034301 (2001) Correlations in Quantum Systems and Branch Points in the Complex Plane
doi: 10.1103/PhysRevC.64.034301
2000DR10 Phys.Rev. C62, 024313 (2000) S.Drozdz, J.Okolowicz, M.P.Ploszajczak, I.Rotter Statistical Aspects of Nuclear Coupling to Continuum NUCLEAR STRUCTURE 24Mg; calculated matrix elements, eigenvalues for coupling between bound and continuum states. Statistical model.
doi: 10.1103/PhysRevC.62.024313
2000RO27 Trans.Bulg.Nucl.Soc. 5, 128 (2000) Spectroscopic Studies in Open Quantum Systems
1999MU06 Phys.Rev. C59, 2040 (1999) S.E.Muraviev, I.Rotter, S.Shlomo, M.H.Urin 4(h-bar)ω Isoscalar Monopole Giant Resonance in 208Pb and Resonance Trapping NUCLEAR STRUCTURE 208Pb; calculated 4(h-bar)ω isoscalar giant monopole resonance strength function; deduced continuum coupling role, resonance trapping effect. Continuum-RPA approach.
doi: 10.1103/PhysRevC.59.2040
1999PE01 Phys.Rev. C59, 164 (1999) Doorway Concept at High Excitation Energy
doi: 10.1103/PhysRevC.59.164
1999ST32 Phys.Rev. C60, 064321 (1999) Ch.Stoyanov, I.Rotter, N.Van Giai Trapping Effect and High-Lying Single-Particle Modes NUCLEAR STRUCTURE 209Pb; calculated neutron single-particle strength distributions; deduced continuum coupling effects. Quasiparticle-phonon model.
doi: 10.1103/PhysRevC.60.064321
1998MU29 Nuovo Cim. 111A, 705 (1998) M.Muller, S.E.Muraviev, I.Rotter, V.V.Sokolov Interfering States and Narrow Resonances at High Excitation Energy NUCLEAR STRUCTURE 208Pb; calculated isoscalar multipole giant resonance strength function; deduced narrow states, role of one-particle continuum. Continuum RPA.
1998RO37 Acta Phys.Pol. B29, 3493 (1998) Phase Transitions at High Level Density and Giant Resonances in Hot Nuclei NUCLEAR STRUCTURE 208Pb; calculated isoscalar monopole giant resonance E, Γ, configurations. Continuum RPA.
1997SO13 Phys.Rev. C56, 1031 (1997) V.V.Sokolov, I.Rotter, D.V.Savin, M.Muller Interfering Doorway States and Giant Resonances. I. Resonance Spectrum and Multipole Strengths
doi: 10.1103/PhysRevC.56.1031
1997SO14 Phys.Rev. C56, 1044 (1997) V.V.Sokolov, I.Rotter, D.V.Savin, M.Muller Interfering Doorway States and Giant Resonances. II. Transition Strengths
doi: 10.1103/PhysRevC.56.1044
1996PE07 Phys.Rev. C53, 3002 (1996) Resonance Phenomena Near Thresholds NUCLEAR STRUCTURE 16O; calculated resonances, nucleon decay characteristics; deduced trapping effect role.
doi: 10.1103/PhysRevC.53.3002
1995IS01 Phys.Rev. C51, 1842 (1995) Radial Pattern of Nuclear Decay Processes NUCLEAR STRUCTURE 16O; calculated 1- resonances partial widths radial profile; deduced correlation to T1/2. Continuum shell model.
doi: 10.1103/PhysRevC.51.1842
1994IS02 J.Phys.(London) G20, 775 (1994) Self-Organization in the Nuclear System: II. Formation of a new order
doi: 10.1088/0954-3899/20/5/011
1994MU15 Acta Phys.Pol. B25, 711 (1994) Selforganization and Disorder in an Open Quantum System
1993HE07 Nucl.Phys. A556, 107 (1993) R.-D.Herzberg, P.von Brentano, I.Rotter Evidence for Trapping and Collectivization of Resonances at Strong Coupling NUCLEAR STRUCTURE 53Cr; analyzed neutron resonance data; deduced trapping, collectivization evidence.
doi: 10.1016/0375-9474(93)90240-X
1993IS08 J.Phys.(London) G19, 2045 (1993) Self-Organization in the Nuclear System: I. The Slaving Principle NUCLEAR STRUCTURE 16O; calculated transition from low to high level density; deduced slaving principle evidence. Many-body system, continuum channels, self-organization point of view.
doi: 10.1088/0954-3899/19/12/010
1993SI26 Roum.J.Phys. 38, 55 (1993) I.Silisteanu, M.Ivascu, I.Rotter The Excitation of Collective Modes in Heavy Fragment Radioactivity RADIOACTIVITY 221Fr, 221,222,223,224,226Ra, 225Ac(14C); 231Pa(23F); 230,232Th, 231Pa, 234,232,233U(24Ne); 233U(25Ne); 234U(26Ne); 234U, 238Pu(28Mg); 237Np, 238Pu(30Mg); 238Pu(32Si); 241Am(34Si); calculated cluster decay resonance width, decay T1/2. Collective mode excitation, microscopic, macroscopic method.
1991IS04 Phys.Rev. C44, 721 (1991) Radial Characteristics for Nuclear States with Weakly Bound Nucleons NUCLEAR REACTIONS 16O(γ, p), (γ, n), E=22 MeV; calculated σ radial profiles. Continuum shell model. NUCLEAR STRUCTURE 16O; calculated resonances, Γ. Shell model.
doi: 10.1103/PhysRevC.44.721
1989RO03 J.Phys.(London) G15, 251 (1989) Particle Decay and Fission NUCLEAR STRUCTURE 13N; analyzed model level widths. 12C; analyzed α-widths, S(α).
doi: 10.1088/0954-3899/15/2/013
1989RO08 J.Phys.(London) G15, 1007 (1989) Fluctuations in the Cross Section and the Dibaryon NUCLEAR REACTIONS 15N(p, p), (p, p'), E=25-41 MeV; calculated σ(E); deduced resonance to fluctuation transition. Microscopic model.
doi: 10.1088/0954-3899/15/7/009
1988RO09 J.Phys.(London) G14, 857 (1988) Order Out of Chaos in Atomic Nuclei NUCLEAR REACTIONS 15N(p, p), 15O(n, n), E not given; calculated 16O resonance parameters.
doi: 10.1088/0305-4616/14/7/006
1986KL06 J.Phys.(London) G12, 821 (1986) On the Interplay between Giant Resonances and Background NUCLEAR REACTIONS, ICPND 15N(p, p), (p, p'), E ≈ 30-33 MeV; calculated GDR excitation σ(E); deduced level correlation near resonance. S-matrix approach.
doi: 10.1088/0305-4616/12/9/007
1986RO26 J.Phys.(London) G12, 1407 (1986) Self-Organisation in Nuclei NUCLEAR REACTIONS 15N(p, p), (p, p'), E=25-41 MeV; calculated σ(E). Self-organizing systems, quantum fluctuations. NUCLEAR STRUCTURE 16O; calculated resonances, widths. Continuum shell model.
doi: 10.1088/0305-4616/12/12/018
1985KL04 Phys.Rev. C32, 1742 (1985) Spectroscopic Properties of Highly Excited States NUCLEAR REACTIONS 15N(p, p'), E=25-41 MeV; calculated σ(E) vs < Γ >/< D >. 16O deduced resonance spectroscopic properties. Continuum shell model.
doi: 10.1103/PhysRevC.32.1742
1984RO05 Phys.Rev. C29, 1119 (1984) Comment on a Discrepancy between Proton- and Alpha-Induced Cluster Knockout Reactions on 16O NUCLEAR REACTIONS 16O(p, pα), (α, 2α), E not given; calculated knockout spectroscopic factors. Continuum shell model.
doi: 10.1103/PhysRevC.29.1119
1982KL06 J.Phys.(London) G8, 955 (1982) On Resonance Phenomena in Nuclear Reaction Cross Sections NUCLEAR REACTIONS 52Cr(p, γ), (p, p'γ), E=4.14-4.2 MeV; measured Eγ, Iγ, γ(θ), σ(θ). 52Cr(p, p), E=4.59-4.72 MeV; measured σ(θ) vs E. 53Mn deduced resonances, Γp, Γ, L, J, possible IAR. 15N(n, n), E=14-18 MeV; calculated σ(E). Continuum shell model, correlation analysis.
doi: 10.1088/0305-4616/8/7/012
1982KL09 Nucl.Phys. A391, 137 (1982) Gamow-Teller Resonances and Nuclear Structure NUCLEAR REACTIONS 15N(p, p), (p, p'), E not given; calculated 1- resonances, Γ with, without external mixing; deduced resonance localization in presence of fragmentation of IAR, Gamow-Teller resonances. Continuum shell model.
doi: 10.1016/0375-9474(82)90223-8
1979HO17 Nucl.Phys. A330, 109 (1979) Continuum Shell-Model Investigation of the Photoexcited Giant Dipole Resonance in the Non-Magic Nucleus 13C NUCLEAR REACTIONS 13C(γ, n), E=10-35 MeV; 12C(γ, p), E=20-35 MeV; calculated σ(E). Continuum shell model, 3 particle-2 hole configurations.
doi: 10.1016/0375-9474(79)90540-2
1979KA13 J.Phys.(London) G5, 747 (1979) Coulomb Energy Anomaly and Charge-Dependent Nuclear Forces NUCLEAR STRUCTURE 15N, 15O; calculated Coulomb energy anomaly. Continuum shell-model, coupling discrete to continuum states.
doi: 10.1088/0305-4616/5/6/003
1979RO04 J.Phys.(London) G5, 685 (1979) On Structures in the Energy Dependence of Nuclear Reaction Cross Sections NUCLEAR REACTIONS 16O(γ, n0), E=21-26 MeV; 15N(n, n0), (n, n'), E=15-17 MeV; calculated σ; deduced role of nuclear molecular states, dependence of ratio Γ/D on structure. Coupled channels formalism.
doi: 10.1088/0305-4616/5/5/009
1978BA52 Nucl.Phys. A307, 285 (1978) Continuum Shell-Model Calculation of an Excited-State GDR Observed in the Reaction 15N(p, γ2) NUCLEAR REACTIONS 15N(p, γ), E=10-24 MeV; calculated σ(E) for an excited-state GDR.
doi: 10.1016/0375-9474(78)90618-8
1978RO05 Nucl.Phys. A297, 237 (1978) Threshold Effects in Nuclear Reactions and the Line Shape of Resonances NUCLEAR REACTIONS 15N(n, n), 16O(γ, n), (γ, p); calculated σ(θ), threshold effects.
doi: 10.1016/0375-9474(78)90274-9
1977BA02 Nucl.Phys. A275, 111 (1977) Coupled Channels Calculations in the Continuum Shell Model with Complicated Configurations NUCLEAR REACTIONS 15N(p, n), E=3.75-7.5 MeV; calculated σ. 16O calculated resonances.
doi: 10.1016/0375-9474(77)90279-2
1977HO32 Nukleonika 22, 1175 (1977) On the Role of Complicated Configurations in Giant Resonances of Light Nuclei Investigated in the Frame of the Continuum Shell Model NUCLEAR REACTIONS 13C(γ, np), E=10-35 MeV; calculated σ(E). 15N(p, γ), E=12-20 MeV; calculated σ(E, θ). Continuum shell model, GDR excitation.
1977RO09 Phys.Lett. 67B, 385 (1977) On Intermediate Structures in Heavy Ion Reactions NUCLEAR REACTIONS 15N(n, n'), E=15.5-16.5 MeV; calculated σ.
doi: 10.1016/0370-2693(77)90425-7
1976BA48 Yad.Fiz. 24, 508 (1976); Sov.J.Nucl.Phys. 24, 264 (1976) H.W.Barz, I.Birke, H.U.Jager, H.R.Kissener, I.Rotter, J.Hohn Shell-Model Calculations for the 16O + γ Reaction with and Without Allowance for the Continuous Spectrum NUCLEAR REACTIONS 16O(γ, n), (γ, p), (γ, X), E ≤ 26 MeV; calculated σ. Shell model.
1976RO16 Yad.Fiz. 24, 513 (1976); Sov.J.Nucl.Phys. 24, 266 (1976) On Threshold Effects in Nuclear Reactions NUCLEAR REACTIONS 15N(n, n'), E ≈ threshold; calculated σ; deduced threshold effects. Shell model.
1975BA26 Nukleonika 20, 413 (1975) The Calculation of Resonance Parameters in the Continuum Shell Model NUCLEAR REACTIONS 15N(n, n), E=14.2-15.6 MeV; calculated σ, resonance parameters.
1975RO31 Fiz.Elem.Chastits At.Yadra 6, 435 (1975); Sov.J.Particles Nucl. 6, 175 (1976) I.Rotter, H.W.Barz, R.Wunsch, J.Hohn Coupled-Channels Method of Calculations in the Shell Model with Allowance for the Continuous Spectrum NUCLEAR REACTIONS 15N(n, n), E=13-17 MeV; 15N(p, n), E=7.5-8.5 MeV; 16O(μ-, X); calculated σ.
1971BA95 Phys.Lett. 37B, 4 (1971) Shell-Model Aspects in Coupled Channel Calculations Using Feshbach Projection Technique NUCLEAR REACTIONS 15N(n, n), E=1-11 MeV; calculated σ(θ). 16N calculated resonances, level-width. Coupled-channel approximation, Feshbach projection method.
doi: 10.1016/0370-2693(71)90553-3
1968ZH05 Izv.Akad.Nauk SSSR, Ser.Fiz. 32, 1714 (1968); Bull.Acad.Sci.USSR, Phys.Ser. 32, 1579 (1969) M.A.Zhusupov, O.Lkhagva, I.Rotter Cluster Reduced Widths for 14N and 15N NUCLEAR STRUCTURE 14,15N; calculated cluster reduced width.
Back to query form |