NSR Query Results


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NSR database version of April 27, 2024.

Search: Author = T.Petruse

Found 4 matches.

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2024SO08      Nuovo Cim. C 47, 58 (2024)

P.-A.Soderstrom, A.Kusoglu, D.L.Balabanski, M.Brezeanu, D.Choudhury, A.Gavrilescu, R.A.Gucbtoiu, S.Ioannidis, G.Lorusso, M.Markova, R.Roy, D.Testov, S.Adachi, S.Aogaki, R.Borcea, F.Camera, P.Constantin, C.Costache, M.Cuciuc, F.C.L.Crespi, N.M.Florea, Y.Fujikawa, T.Furuno, A.Giaz, T.Kawabata, C.Mihai, R.E.Mihai, B.Million, D.Nichita, R.Niina, S.Okamoto, K.Sakanashi, L.Stan, A.Tamii, A.Turturica, S.Ujeniuc, O.Wieland, R.S.Ban, M.Ciemala, G.Ciocan, C.Clisu, I.Dinescu, D.Iancu, M.Kmiecik, V.Lelasseux, R.Lica, N.M.Marginean, C.Neaccbsu, H.Pai, P.Parlea, T.Petruse, A.Rotaru, C.O.Sotty, A.Spataru, A.N.State, M.Straticiuc, D.Tofan, S.Toma, T.Tozar, G.V.Turturica, C.A.Ur

From implementation to operation and the first measurements with the ELIGANT detectors from ELI-NP

NUCLEAR REACTIONS 112Sn(p, p'), E not given; measured reaction products, Ep, Ip; deduced preliminary level density. Comparison with three microscopic models. The ELIGANT-GN detectors at ROSPHERE.

doi: 10.1393/ncc/i2024-24058-3
Citations: PlumX Metrics


2024WI01      Nuovo Cim. C 47, 24 (2024)

O.Wieland, A.Bracco, F.Camera, S.Aogaki, D.L.Balabanski, E.Boicu, R.Borcea, M.Boromiza, I.Burducea, S.Calinescu, A.Coman, P.Constantin, C.Costache, M.Ciemala, Gh.Ciocan, C.Clisu, F.C.L.Crespi, M.Cuciuc, A.Dhal, N.Djourelov, N.M.Florea, I.Gheorghe, A.Giaz, D.Iancu, D.M.Kahl, M.Kmiecik, A.Kusoglu, R.Lica, N.Mvarginean, A.Maj, R.Marginean, C.Mihai, R.E.Mihai, B.Million, C.Neacsu, D.Nichita, C.Nitva, H.Pai, A.Pappalardo, T.Petruse, A.Rotaru, A.B.Serban, P.-A.Soderstrom, C.O.Sotty, L.Stan, A.N.State, I.Stiru, A.Stoica, D.A.Testov, S.Toma, T.Tozar, A.Turturica, G.V.Turturica, S.Ujeniuc, V.Vasilca, Y.Xu

Extra yield in hot Ni isotopes below the Giant Dipole Resonance

NUCLEAR REACTIONS 24Mg(32S, X)56Ni, E=90 MeV; 26Mg(34S, X)60Ni, E=79 MeV; 26Mg(36S, X)62Ni, E=78 MeV; measured reaction products, Eγ, Iγ; deduced yields, linearized measured γ-ray yields, the tail of the Giant Dipole Resonance which may be attributed to a Pygmy Dipole Resonance in an excited nucleus with statistical model using a Monte Carlo approach. The IFIN 9 MV Tandem facility.

doi: 10.1393/ncc/i2024-24024-1
Citations: PlumX Metrics


2023GU07      Eur.Phys.J. A 59, 65 (2023)

G.L.Guardo, T.Petruse, D.Lattuada, M.La Cognata, D.L.Balabanski, E.Aciksoz, L.Acosta, L.Capponi, D.Carbone, S.Cherubini, D.Choudhury, G.D'Agata, A.Di Pietro, P.Figuera, M.Gulino, A.I.Kilik, M.La Commara, L.Lamia, C.Matei, S.Palmerini, R.G.Pizzone, G.G.Rapisarda, S.Romano, M.L.Sergi, P.-A.Soderstrom, R.Sparta, A.Tumino, S.Vinals

Direct measurement of the 19F(p, α0)16O reaction at Ecm= 0.4-0.9 using the LHASA detector array

NUCLEAR REACTIONS 1H(19F, α), E(cm)=0.4-0.9 MeV; measured reaction products, Eα, Iα; deduced σ(θ), S-factor. Comparison with NACRE compilation, available data. INFN-Laboratori Nazionali del Sud, Catania (Italy).

doi: 10.1140/epja/s10050-023-00957-1
Citations: PlumX Metrics

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


2020SO26      Commun. Phys. 11, 3242 (2020)

P.-A.Soderstrom, L.Capponi, E.Aciksoz, T.Otsuka, N.Tsoneva, Y.Tsunoda, D.L.Balabanski, N.Pietralla, G.L.Guardo, D.Lattuada, H.Lenske, C.Matei, D.Nichita, A.Pappalardo, T.Petruse

Electromagnetic character of the competitive γγ/γ-decay from 137mBa

RADIOACTIVITY 137Cs(β-), 137Ba(IT); measured decay products, Eγ, Iγ, γ-γ-coin.; deduced γ-ray energies, widths and nuclear static dipole polarisabilities, angular correlation of the two photons emitted in the double-γ decay, Energy-sharing distribution for the two photons in the double-γ decay, an improved value on the double-photon versus single-photon branching ratio. Comparison with calculations. CeBr3 detectors from ELIGANT, the ELI Gamma Above Neutron Threshold (ELIGANT) detector system.

doi: 10.1038/s41467-020-16787-4
Citations: PlumX Metrics

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


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