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NSR database version of May 20, 2024.

Search: Author = A.Klimkiewicz

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2014LA09      Phys.Rev. C 89, 035806 (2014)

C.Langer, O.Lepyoshkina, Y.Aksyutina, T.Aumann, S.Beceiro Novo, J.Benlliure, K.Boretzky, M.Chartier, D.Cortina, U.Datta Pramanik, O.Ershova, H.Geissel, R.Gernhauser, M.Heil, G.Ickert, H.T.Johansson, B.Jonson, A.Kelic-Heil, A.Klimkiewicz, J.V.Kratz, R.Krucken, R.Kulessa, K.Larsson, T.Le Bleis, R.Lemmon, K.Mahata, J.Marganiec, T.Nilsson, V.Panin, R.Plag, W.Prokopowicz, R.Reifarth, V.Ricciardi, D.M.Rossi, S.Schwertel, H.Simon, K.Summerer, B.Streicher, J.Taylor, J.R.Vignote, F.Wamers, C.Wimmer, P.Z.Wu

Thermonuclear reaction 30S(p, γ)31Cl studied via Coulomb breakup of 31Cl

NUCLEAR REACTIONS Pb(31Cl, p), [31Cl secondary beam from 9Be(36Ar, X), E=825 MeV/nucleon primary reaction], E=650 MeV/nucleon; measured reaction products, fragment spectra, Eγ, Iγ at R3B-LAND-GSI facility. 31Cl; deduced levels, resonances, J, π, width, comparison with levels predicted in shell-model calculations. 30S(p, γ), T=0.08-2.00 GK; deduced thermonuclear reaction rates. Relevance to rp process in typical Type I x-ray burst conditions.

doi: 10.1103/PhysRevC.89.035806
Citations: PlumX Metrics

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


2013RO33      Phys.Rev.Lett. 111, 242503 (2013)

D.M.Rossi, P.Adrich, F.Aksouh, H.Alvarez-Pol, T.Aumann, J.Benlliure, M.Bohmer, K.Boretzky, E.Casarejos, M.Chartier, A.Chatillon, D.Cortina-Gil, U.Datta Pramanik, H.Emling, O.Ershova, B.Fernandez-Dominguez, H.Geissel, M.Gorska, M.Heil, H.T.Johansson, A.Junghans, A.Kelic-Heil, O.Kiselev, A.Klimkiewicz, J.V.Kratz, R.Krucken, N.Kurz, M.Labiche, T.Le Bleis, R.Lemmon, Yu.A.Litvinov, K.Mahata, P.Maierbeck, A.Movsesyan, T.Nilsson, C.Nociforo, R.Palit, S.Paschalis, R.Plag, R.Reifarth, D.Savran, H.Scheit, H.Simon, K.Summerer, A.Wagner, W.Walus, H.Weick, M.Winkler

Measurement of the Dipole Polarizability of the Unstable Neutron-Rich Nucleus 68Ni

NUCLEAR REACTIONS Pb(68Ni, 68Ni'), (68Ni, X), E=502.7 MeV/nucleon; measured reaction products, Eγ, Iγ, En, In. 68Ni; deduced σ(E), giant and pygmy dipole resonance parameters, E1 strength, neutron skin thickness. Comparison with available data.

doi: 10.1103/PhysRevLett.111.242503
Citations: PlumX Metrics


2012RO33      Prog.Theor.Phys.(Kyoto), Suppl. 196, 465 (2012)

D.M.Rossi, P.Adrich, F.Aksouh, H.Alvarez-Pol, T.Aumann, J.Benlliure, M.Bohmer, K.Boretzky, E.Casarejos, M.Chartier, A.Chatillon, D.Cortina-Gil, U.Datta Pramanik, H.Emling, O.Ershova, B.Fernando-Dominguez, H.Geissel, M.Gorska, M.Heil, H.Johansson, A.R.Junghans, O.Kiselev, A.Klimkiewicz, J.V.Kratz, N.Kurz, M.Labiche, T.Le Bleis, R.Lemmon, Y.A.Litvinov, K.Mahata, P.Maierbeck, A.Movsesyan, T.Nilsson, C.Nociforo, R.Palit, S.Paschalis, R.Plag, R.Reifarth, H.Simon, K.Summerer, A.Wagner, W.Walus, H.Weick, M.Winkler

Investigation of the Dipole Response in Exotic Nuclei - Experiments at the LAND-R3B Setup

NUCLEAR REACTIONS Pb(68Ni, X), E=500 MeV/nucleon; measured reaction products; deduced Coulomb excitation σ(θ), dipole strength.

doi: 10.1143/PTPS.196.465
Citations: PlumX Metrics


2012SC18      Eur.Phys.J. A 48, 191 (2012)

S.Schwertel, P.Maierbeck, R.Krucken, R.Gernhauser, T.Kroll, H.Alvarez-Pol, F.Aksouh, T.Aumann, K.Behr, E.A.Benjamim, J.Benlliure, V.Bildstein, M.Bohmer, K.Boretzky, M.J.G.Borge, A.Brunle, A.Burger, M.Caamano, E.Casarejos, A.Chatillon, L.V.Chulkov, D.Cortina-Gil, J.Enders, K.Eppinger, T.Faestermann, J.Friese, L.Fabbietti, M.Gascon, H.Geissel, J.Gerl, M.Gorska, P.G.Hansen, B.Jonson, R.Kanungo, O.Kiselev, I.Kojouharov, A.Klimkiewicz, T.Kurtukian, N.Kurz, K.Larsson, T.Le Bleis, K.Mahata, L.Maier, T.Nilsson, C.Nociforo, G.Nyman, C.Pascual-Izarra, A.Perea, D.Perez, A.Prochazka, C.Rodriguez-Tajes, D.Rossi, H.Schaffner, G.Schrieder, H.Simon, B.Sitar, M.Stanoiu, K.Summerer, O.Tengblad, H.Weick, S.Winkler, B.A.Brown, T.Otsuka, J.A.Tostevin, W.D.M.Rae

One-neutron knockout from 51-55Sc

NUCLEAR REACTIONS 9Be(55Sc, 54Sc), (54Sc, 53Sc), (53Sc, 52Sc), (52Sc, 51Sc), (51Sc, 50Sc), E≈420 MeV/nucleon; measured relativistic reaction products, Eγ, Iγ; deduced longitudinal momentum distribution, σ; calculated σ.

doi: 10.1140/epja/i2012-12191-5
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2348.


2010LE27      J.Phys.:Conf.Ser. 202, 012035 (2010)

T.Le Bleis, D.Rossi, A.Klimkiewicz, P.Adrich, K.Boretzky, F.Aksouh, H.Alvarez-Pol, T.Aumann, J.Benlliure, M.Boehmer, E.Casarejos, M.Chartier, A.Chatillon, D.Cortina-Gil, U.D.Pramanik, H.Emling, O.Ershova, B.Fernandez-Dominguez, H.Geissel, M.Gorska, M.Heil, H.Johansson, A.R.Junghans, O.Kiselev, J.V.Kratz, N.Kurz, M.Labiche, R.Lemmon, Y.Litvinov, K.Mahata, P.Maierbeck, T.Nilsson, C.Nociforo, R.Palit, S.Paschalis, R.Plag, R.Reifarth, H.Simon, K.Smmerer, A.Wagner, W.Walus, H.Weick, M.Winkler

Target dependence in the study of collective modes in stable and exotic Ni nuclei

NUCLEAR REACTIONS C, Sn, Pb(56Ni, 55Ni), (57Ni, 56Ni), (58Ni, 57Ni), (59Ni, 58Ni), (60Ni, 59Ni), (61Ni, 60Ni), (62Ni, 61Ni), (63Ni, 62Ni), (64Ni, 63Ni), (65Ni, 64Ni), (66Ni, 65Ni), (67Ni, 66Ni), (68Ni, 67Ni), (69Ni, 68Ni), (70Ni, 69Ni), (71Ni, 70Ni), (72Ni, 71Ni), E≈500 MeV/nucleon; measured En, In, Eγ, Eγ using LAND setup (LAND neutron detector, dipole ALADIN, CSI crystals for γ); deduced Coulex σ, nuclear σ, GDR, PDR σ. Preliminary.

doi: 10.1088/1742-6596/202/1/012035
Citations: PlumX Metrics


2009KL02      Acta Phys.Pol. B40, 589 (2009)

A.Klimkiewicz, N.Paar, P.Adrich, M.Fallot, K.Boretzky, T.Aumann, D.Cortina-Gil, U.Datta Pramanik, Th.W.Elze, H.Emling, H.Geissel, M.Hellstrom, K.L.Jones, J.V.Kratz, R.Kulessa, C.Nociforo, R.Palit, H.Simon, G.Surowka, K.Summerer, D.Vretenar, W.Walus

Collective Dipole Excitations in Neutron-Rich Nuclei from 132Sn Mass Region, the Nuclear Symmetry Energy and Neutron Skins

NUCLEAR REACTIONS Pb(130Sn, 130Sn'), (132Sn, 132Sn'), E not given;measured dipole strength distributions following projectile Coulomb excitation;deduced symmetry energy pressure, neutron skin thickness, pygmy strength. Comparison with calculations.


2009MA16      Phys.Lett. B 675, 22 (2009)

P.Maierbeck, R.Gernhauser, R.Krucken, T.Kroll, H.Alvarez-Pol, F.Aksouh, T.Aumann, K.Behr, E.A.Benjamim, J.Benlliure, V.Bildstein, M.Bohmer, K.Boretzky, M.J.G.Borge, A.Brunle, A.Burger, M.Caamano, E.Casarejos, A.Chatillon, L.V.Chulkov, D.Cortina-Gil, J.Enders, K.Eppinger, T.Faestermann, J.Friese, L.Fabbietti, M.Gascon, H.Geissel, J.Gerl, M.Gorska, P.G.Hansen, B.Jonson, R.Kanungo, O.Kiselev, I.Kojouharov, A.Klimkiewicz, T.Kurtukian, N.Kurz, K.Larsson, T.Le Bleis, K.Mahata, L.Maier, T.Nilsson, C.Nociforo, G.Nyman, C.Pascual-Izarra, A.Perea, D.Perez, A.Prochazka, C.Rodriguez-Tajes, D.Rossi, H.Schaffner, G.Schrieder, S.Schwertel, H.Simon, B.Sitar, M.Stanoiu, K.Summerer, O.Tengblad, H.Weick, S.Winkler, B.A.Brown, T.Otsuka, J.Tostevin, W.D.M.Rae

Structure of 55Ti from relativistic one-neutron knockout

NUCLEAR REACTIONS 9Be(48Ca, n47Ca), (56Ti, n55Ti), E=450 MeV/nucleon; measured σ, Eγ, Iγ, (recoil)γ-coin after Doppler correction, momentum distributions. 47Ca, 55Ti; deduced J, π, levels. Comparison with shell-model calculations. FRS with secondary beam and MINIBALL array.

doi: 10.1016/j.physletb.2009.03.049
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0614. Data from this article have been entered in the XUNDL database. For more information, click here.


2007KL05      Nucl.Phys. A788, 145c (2007)

A.Klimkiewicz, P.Adrich, K.Boretzky, M.Fallot, T.Aumann, D.Cortina-Gil, U.Datta Pramanik, Th.W.Elze, H.Emling, H.Geissel, M.Hellstroem, K.L.Jones, J.V.Kratz, R.Kulessa, Y.Leifels, C.Nociforo, R.Palit, H.Simon, G.Surowka, K.Summerer, S.Typel, W.Walus

Dipole response of neutron-rich Sn isotopes

NUCLEAR REACTIONS Be(238U, X), E=550 MeV/nucleon; measured fragment yields. 12C, 208Pb(129Sn, X), (130Sn, X), (131Sn, X), (132Sn, X), (133Sn, X), E≈ 500 MeV/nucleon; measured En, Eγ, nγ-coin; deduced electromagnetic dissociation σ(E). 129,130,131,132,133Sn deduced dipole strength distributions, B(E1), pygmy and giant dipole resonance parameters. Comparison with RPA calculations. 40,44,48Ca, 116,124Sn, 138Ba, 140Ce, 142Nd, 144Sm, 208Pb(γ, γ'), E not given; analyzed Eγ, Iγ. 40,44,48Ca, 116,124Sn, 138Ba, 140Ce, 142Nd, 144Sm, 208Pb deduced B(E1).

doi: 10.1016/j.nuclphysa.2007.01.075
Citations: PlumX Metrics


2007KL06      Phys.Rev. C 76, 051603 (2007)

A.Klimkiewicz, N.Paar, P.Adrich, M.Fallot, K.Boretzky, T.Aumann, D.Cortina-Gil, U.Datta Pramanik, Th.W.Elze, H.Emling, H.Geissel, M.Hellstrom, K.L.Jones, J.V.Kratz, R.Kulessa, C.Nociforo, R.Palit, H.Simon, G.Surowka, K.Summerer, D.Vretenar, W.Walus, for the LAND Collaboration

Nuclear symmetry energy and neutron skins derived from pygmy dipole resonances

NUCLEAR REACTIONS Be(238U, X)129Sn/130Sn/131Sn/132Sn/133Sb/134Sb, E=500 MeV/nucleon; measured pygmy dipole resonance strength, neutron skin thickness, symmetry parameters; deduced neutron separation energy, B(E1) using RQRPA approach. Compared to 116Sn, 140Ce, 142Nd, 144Sm, 208Pb.

doi: 10.1103/PhysRevC.76.051603
Citations: PlumX Metrics


2005AD29      Phys.Rev.Lett. 95, 132501 (2005)

P.Adrich, A.Klimkiewicz, M.Fallot, K.Boretzky, T.Aumann, D.Cortina-Gil, U.Datta Pramanik, Th.W.Elze, H.Emling, H.Geissel, M.Hellstrom, K.L.Jones, J.V.Kratz, R.Kulessa, Y.Leifels, C.Nociforo, R.Palit, H.Simon, G.Surowka, K.Summerer, W.Walus, and the LAND-FRS Collaboration

Evidence for Pygmy and Giant Dipole Resonances in 130Sn and 132Sn

NUCLEAR REACTIONS Be(238U, X), E not given; measured fragment yields. 12C, 208Pb(130Sn, nX), (132Sn, nX), E ≈ 500 MeV/nucleon; measured En, Eγ, nγ-coin; deduced Coulomb dissociation σ(E). 130,132Sn deduced dipole strength distributions, pygmy and giant dipole resonance parameters.

doi: 10.1103/PhysRevLett.95.132501
Citations: PlumX Metrics


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