NSR Query Results


Output year order : Descending
Format : Normal

NSR database version of April 11, 2024.

Search: Author = M.Grinberg

Found 23 matches.

Back to query form



2004KA62      Phys.Rev. C 70, 064307 (2004)

L.Kaubler, H.Schnare, R.Schwengner, H.Prade, F.Donau, P.von Brentano, J.Eberth, J.Enders, A.Fitzler, C.Fransen, M.Grinberg, R.-D.Herzberg, H.Kaiser, P.von Neumann-Cosel, N.Pietralla, A.Richter, G.Rusev, Ch.Stoyanov, I.Wiedenhover

Dipole and quadrupole excitations in 88Sr up to 6.8 MeV

NUCLEAR REACTIONS 88Sr(γ, γ'), E=6.8 MeV bremsstrahlung; measured Eγ, Iγ. 88Sr deduced levels, J, π, configurations, B(E1), B(M1), B(E2). Comparison with model predictions.

doi: 10.1103/PhysRevC.70.064307
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0775. Data from this article have been entered in the XUNDL database. For more information, click here.


2002KA25      Phys.Rev. C65, 054315 (2002)

L.Kaubler, K.D.Schilling, R.Schwengner, F.Donau, E.Grosse, D.Belic, P.von Brentano, M.Bubner, C.Fransen, M.Grinberg, U.Kneissl, C.Kohstall, A.Linnemann, P.Matschinsky, A.Nord, N.Pietralla, H.H.Pitz, M.Scheck, F.Stedile, V.Werner

Influence of the N = 50 Neutron Core on Dipole Excitations in 87Rb

NUCLEAR REACTIONS 87Rb(γ, γ'), E=4.0 MeV bremsstrahlung; measured Eγ, Iγ. 87Rb deduced levels, J, π, configurations, excitation B(M1), B(E1), widths. Comparison with shell model predictions.

doi: 10.1103/PhysRevC.65.054315
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0774. Data from this article have been entered in the XUNDL database. For more information, click here.


2001ST21      Yad.Fiz. 64, No 6, 1223 (2001); Phys.Atomic Nuclei 64, 1147 (2001)

Ch.Stoyanov, N.Lo Iudice, N.Tsoneva, M.Grinberg

Properties of the Low-Lying Excited States in Even-Even Nuclei Around the Closed Shell N = 82

NUCLEAR STRUCTURE 136Ba, 144Nd; calculated levels, J, π, B(E2), B(M1). Quasiparticle phonon model.

doi: 10.1134/1.1383632
Citations: PlumX Metrics


2000GR02      Phys.Rev. C61, 024317 (2000)

M.Grinberg, Ch.Protochristov, W.Andrejtscheff, G.Lo Bianco, G.Falconi

Collective Vibrational Bands Built on Two-Quasiparticle Excitations in Te Isotopes

NUCLEAR STRUCTURE 114,116,118,120,122,124,126,128,130Te; analyzed levels, J, π; deduced vibrational bands configurations. Quasiparticle-phonon model.

doi: 10.1103/PhysRevC.61.024317
Citations: PlumX Metrics


2000KA08      Eur.Phys.J. A 7, 15 (2000)

L.Kaubler, H.Schnare, R.Schwengner, P.von Brentano, F.Donau, J.Eberth, J.Enders, A.Fitzler, C.Fransen, M.Grinberg, E.Grosse, R.-D.Herzberg, H.Kaiser, P.von Neumann-Cosel, N.Pietralla, H.Prade, A.Richter, S.Skoda, Ch.Stoyanov, H.-G.Thomas, H.Tiesler, D.Weisshaar, I.Wiedenhover

Is the 4.742 MeV State in 88Sr the 1- Two-Phonon State ?

NUCLEAR REACTIONS 88Sr, 11B, 12,13C(γ, γ'), E=6.7 MeV bremsstrahlung; measured Eγ, Iγ, γ polarization. 88Sr deduced levels, J, π, B(λ), no two-phonon state.

doi: 10.1007/s100500050004
Citations: PlumX Metrics


2000ST05      Nucl.Phys. A669, 14 (2000)

E.A.Stefanova, T.Kutsarova, I.Deloncle, M.-G.Porquet, M.Grinberg, E.Gueorguieva, Ts.Venkova, A.Minkova, F.Azaiez, S.Bouneau, C.Bourgeois, J.Duprat, B.J.P.Gall, C.Gautherin, F.Hoellinger, R.Lucas, H.Sergolle, N.Schulz, A.Wilson, Ch.Stoyanov

High-Spin States of 3888Sr50: Breaking of the neutron core

NUCLEAR REACTIONS 176Yb(28Si, F)88Sr, E=145 MeV; measured Eγ, Iγ, γγ-coin following compound nucleus fission. 88Sr deduced high-spin levels, possible J, π, configurations. Eurogam2 array. Comparison with neighboring isotones, quasiparticle-phonon model calculations.

doi: 10.1016/S0375-9474(99)00566-7
Citations: PlumX Metrics

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


1999SC19      Nucl.Phys. A652, 339 (1999)

W.Schauer, C.Doll, T.von Egidy, R.Georgii, J.Ott, H.-F.Wirth, A.Gollwitzer, G.Graw, R.Hertenberger, B.Valnion, M.Grinberg, Ch.Stoyanov

Study of 122Te with Charged Particle Reactions

NUCLEAR REACTIONS 122Te(d, d'), E=26 MeV; 123Te(d, t), E=28 MeV; 123Te(3He, α), E=32 MeV; 121Sb(3He, d), E=32 MeV; measured particle spectra, σ(θ). 122Te deduced levels, J, π, intruder band. Interacting boson model and quasiparticle phonon model calculations.

doi: 10.1016/S0375-9474(98)00643-5
Citations: PlumX Metrics


1999ST13      Nucl.Phys. A649, 93c (1999)

Ch.Stoyanov, V.Yu.Ponomarev, N.Tsoneva, M.Grinberg

The Influence of the GDR on the Low-Energy E1 Transitions in Spherical Nuclei

NUCLEAR STRUCTURE 120Sn, 144Sm, 144Nd; calculated hindered transitions B(E1); deduced two-phonon, GDR components. Comparison with data.

doi: 10.1016/S0375-9474(99)00045-7
Citations: PlumX Metrics


1998GR23      Fiz.Elem.Chastits At.Yadra 29, 1456 (1998); Phys.Part.Nucl. 29, 606 (1998)

M.Grinberg, Ch.Stoyanov, N.Tsoneva

Interplay of Collective and Noncollective Modes at Low Excitation Energy in Spherical Nuclei

NUCLEAR STRUCTURE 144Nd, 144,146Sm, 124Te; calculated levels, J, π; deduced configurations. 138Ba, 140Ce, 142,144Nd, 144,146Sm, 124Te; calculated B(λ). 144Nd, 146Sm, 124Te; calculated transitions δ. Quasiparticle phonon model.


1998KA60      Nucl.Phys. A643, 259 (1998)

D.Karadjov, V.V.Voronov, F.Catara, M.Grinberg, A.P.Severyukhin

Effects of the Ground State Correlations on the Structure of Vibrational States

NUCLEAR STRUCTURE 68Zn; calculated vibrational states energies, up-transition B(λ), transition charge density; deduced ground state correlations effects. Extended RPA.

doi: 10.1016/S0375-9474(98)00563-6
Citations: PlumX Metrics


1998PO07      Nucl.Phys. A635, 470 (1998)

V.Yu.Ponomarev, Ch.Stoyanov, N.Tsoneva, M.Grinberg

Boson Forbidden Low-Energy E1-Transitions in Spherical Nuclei

NUCLEAR STRUCTURE 120Sn, 144Sm, 144Nd; calculated transitions B(E1); deduced core dipole polarization effects. Quasiparticle phonon model.

doi: 10.1016/S0375-9474(98)00187-0
Citations: PlumX Metrics


1998TS05      Yad.Fiz. 61, No 5, 816 (1998); Phys.Atomic Nuclei 61, 734 (1998)

N.Tsoneva, A.I.Vdovin, Ch.Stoyanov, M.Grinberg

Magnetic Polarization and Two-Phonon States

NUCLEAR STRUCTURE 142Ce, 144Sm; calculated two-phonon states wave functions, B(M2); deduced magnetic core polarization effect.


1997OT02      Nucl.Phys. A625, 598 (1997)

J.Ott, C.Doll, T.von Egidy, R.Georgii, M.Grinberg, W.Schauer, R.Schwengner, H.-F.Wirth

The Nuclear Structure of 126Te Studied with (d, p), (d, 3He) and (d, d') Reactions

NUCLEAR REACTIONS 125Te(d, p), E=26 MeV; 126Te(d, d'), E=24 MeV; 127I(d, 3He), E=27, 28 MeV; measured particle spectra. 126Te deduced levels. Other data input. Quasiparticle-Phonon model calculation.

doi: 10.1016/S0375-9474(97)00494-6
Citations: PlumX Metrics


1997SC15      Nucl.Phys. A620, 277 (1997); Erratum Nucl.Phys. A624, 776 (1997)

R.Schwengner, G.Winter, W.Schauer, M.Grinberg, F.Becker, P.von Brentano, J.Eberth, J.Enders, T.von Egidy, R.-D.Herzberg, N.Huxel, L.Kaubler, P.von Neumann-Cosel, N.Nicolay, J.Ott, N.Pietralla, H.Prade, S.Raman, J.Reif, A.Richter, C.Schlegel, H.Schnare, T.Servene, S.Skoda, T.Steinhardt, C.Stoyanov, H.G.Thomas, I.Wiedenhover, A.Zilges

Two-Phonon J = 1 States in Even-Mass Te Isotopes with A = 122-130

NUCLEAR REACTIONS 126,122Te(γ, γ'), E=4.5 MeV bremsstrahlung; 130Te(γ, γ'), E=5.5 MeV bremsstrahlung; measured Eγ, Iγ(θ). 122,126,130Te deduced levels, J, Γ, B(λ). Enriched targets, Ge detectors.

doi: 10.1016/S0375-9474(97)00169-3
Citations: PlumX Metrics


1997SC25      Z.Phys. A358, 197 (1997)

R.Schwengner, W.Schauer, G.Winter, P.von Brentano, J.Eberth, J.Enders, J.Enders, T.von Egidy, M.Grinberg, R.-D.Herzberg, N.Huxel, L.Kaubler, P.von Neumann-Cosel, N.Nicolay, J.Ott, N.Pietralla, H.Prade, S.Raman, J.Reif, A.Richter, C.Schlegel, H.Schnare, T.Servene, S.Skoda, C.Stoyanov, H.G.Thomas, I.Wiedenhover, A.Zilges

Dipole Excitations in 122Te, 126Te and 130Te

NUCLEAR REACTIONS 122,126,130Te(γ, γ'), E=4.5-5.5 MeV bremsstrahlung; measured Eγ, Iγ. 122,126,130Te deduced levels, J, π, transition γ multipolarity, widths, one-, two-phonon vibrational structure. Quasiparticle-phonon model analysis.

doi: 10.1007/s002180050306
Citations: PlumX Metrics


1996GR02      Nucl.Phys. A597, 355 (1996)

M.Grinberg, R.Piepenbring, K.V.Protasov, B.Silvestre-Brac

Collective and Non-Collective Multiphonon States in Even-Even Spherical Nuclei

doi: 10.1016/0375-9474(95)00482-3
Citations: PlumX Metrics


1996PR01      Phys.Rev. C53, 1646 (1996)

K.V.Protasov, B.Silvestre-Brac, R.Piepenbring, M.Grinberg

Multiphonon Theory: Wick's theorem and recursion formulas for coupled phonons

doi: 10.1103/PhysRevC.53.1646
Citations: PlumX Metrics


1995GE02      Phys.Lett. 351B, 82 (1995)

R.Georgii, P.von Neumann-Cosel, T.von Egidy, M.Grinberg, V.A.Khitrov, J.Ott, P.Prokofev, A.Richter, W.Schauer, C.Schlegel, R.Schulz, L.J.Simonova, Ch.Stoyanov, A.M.Sukhovoj, A.V.Voinov

Unusual Neutron-Capture Gamma-Ray Cascade in 124Te: A fingerprint of octupole-coupled multiphonon states

NUCLEAR REACTIONS 123Te(n, γ), E=thermal; measured γγ-coin, Eγ, Iγ. 124Te(γ, γ'), E=3.5 MeV bremsstrahlung; measured Eγ, Iγ. 124Te deduced levels, transitions, B(λ), configuration. Quasiparticle-phonon model.

doi: 10.1016/0370-2693(95)00400-F
Citations: PlumX Metrics


1995GE06      Nucl.Phys. A592, 307 (1995)

R.Georgii, T.von Egidy, J.Klora, H.Lindner, U.Mayerhofer, J.Ott, W.Schauer, P.von Neumann-Cosel, A.Richter, C.Schlegel, R.Schulz, V.A.Khitrov, A.M.Sukhovoj, A.V.Vojnov, J.Berzins, V.Bondarenko, P.Prokofjevs, L.J.Simonova, M.Grinberg, Ch.Stoyanov

Complete Level Scheme of 124Te up to 3 MeV

NUCLEAR REACTIONS 123Te(d, p), E=22 MeV; 125Te(d, t), E=22 MeV; 123Sb(3He, d), E=33 MeV; 124Te(p, p'), E=24 MeV; measured particle spectra. 123Te(n, γ), E=thermal; measured Eγ, Iγ, γγ-coin. 124Te(γ, γ'), E=3.5, 5 MeV; measured Eγ. 124Te deduced levels, γ-multipolarity, branching ratios, Γ0, Γ1, T1/2. Quasiparticle-phonon model calculation.

doi: 10.1016/0375-9474(95)00311-N
Citations: PlumX Metrics


1994GR12      Nucl.Phys. A573, 231 (1994)

M.Grinberg, Ch.Stoyanov

Distribution of Two-Phonon Strength in Even N = 82 Nuclei

NUCLEAR STRUCTURE 138Ba, 140Ce, 142Nd, 144Sm; calculated levels, B(λ). Quasiparticle phonon model.

doi: 10.1016/0375-9474(94)90169-4
Citations: PlumX Metrics


1993GR08      J.Phys.(London) G19, 1179 (1993)

M.Grinberg, T.K.Dinh, Ch.Protochristov, I.Penev, C.Stoyanov, W.Andrejtscheff

Level Structure and Transition Probabilities in 140Ce

RADIOACTIVITY 140La(β-); measured Eγ, Iγ, βγ-coin. 140Ce deduced levels, J, π, γ-multipolarity, B(λ), δ, T1/2, branching ratio. Quasiparticle-phonon model.

doi: 10.1088/0954-3899/19/8/008
Citations: PlumX Metrics


1992AD04      Z.Phys. A343, 381 (1992)

J.Adam, J.Dobes, B.Kracik, P.Navratil, P.Tlusty, S.Batsev, T.K.Dinh, M.Grinberg, O.Stoyanova, Ch.Stoyanov

Structure of the 146Sm States from the 146Eu Decay

RADIOACTIVITY 146Gd(β+), (EC); 146Eu(β+), (EC); measured Eγ, Iγ, γγ-coin; deduced log ft. 146Sm deduced levels, J, π, δ, γ-multipolarity. Interacting boson, quasiparticle phonon models.

NUCLEAR STRUCTURE 146Sm; calculated levels, B(λ), δ. Interacting boson, quasiparticle phonon models.

doi: 10.1007/BF01289814
Citations: PlumX Metrics


1992DI01      J.Phys.(London) G18, 329 (1992)

T.K.Dinh, M.Grinberg, C.Stoyanov

Interplay of Collective and Non-Collective Modes in Low-Lying Quadrupole States of 140Ba, 142Ce, 144Nd and 146Sm

NUCLEAR STRUCTURE 140Ba, 142Ce, 144Nd, 146Sm; calculated levels, B(λ), μ, quadrupole moment, δ. Quasiparticle-phonon model.

doi: 10.1088/0954-3899/18/2/014
Citations: PlumX Metrics


Back to query form