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NSR database version of April 27, 2024.

Search: Author = B.Romeo

Found 7 matches.

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2023CA17      Eur.Phys.J. A 59, 273 (2023)

P.Capel, D.R.Phillips, A.Andis, M.Bagnarol, B.Behzadmoghaddam, F.Bonaiti, R.Bubna, Y.Capitani, P.-Y.Duerinck, V.Durant, N.Dopper, A.El Boustani, R.Farrell, M.Geiger, M.Gennari, N.Goldberg, J.Herko, T.Kirchner, L.-P.Kubushishi, Z.Li, S.S.Li Muli, A.Long, B.Martin, K.Mohseni, I.Moumene, N.Paracone, E.Parnes, B.Romeo, V.Springer, I.Svensson, O.Thim, N.Yapa

Effective field theory analysis of the Coulomb breakup of the one-neutron halo nucleus 19C

NUCLEAR REACTIONS 208Pb(19C, X)18C, E=67 MeV/nucleon; analyzed available data; deduced σ(θ), σ(E) using NLO Halo-EFT 18C-n potentials. A Halo-EFT description of the projectile within the Coulomb Corrected Eikonal approximation (CCE).

doi: 10.1140/epja/s10050-023-01181-7
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2023JO02      Phys.Lett. B 838, 137689 (2023)

L.Jokiniemi, B.Romeo, C.Brase, J.Kotila, P.Soriano, A.Schwenk, J.Menendez

Two-neutrino ββ decay of 136Xe to the first excited 0+ state in 136Ba

RADIOACTIVITY 136Xe(2β-); calculated nuclear matrix element for the two-neutrino ββ decay of 136Xe into the first excited state of 136Ba using the quasiparticle random-phase approximation (QRPA) framework, the nuclear shell model, the interacting boson model (IBM-2), and an effective field theory (EFT) for β and ββ decays; deduced T1/2.

doi: 10.1016/j.physletb.2023.137689
Citations: PlumX Metrics


2023JO04      Phys.Rev. C 107, 044305 (2023)

L.Jokiniemi, B.Romeo, P.Soriano, J.Menendez

Neutrinoless ββ-decay nuclear matrix elements from two-neutrino ββ-decay data

RADIOACTIVITY 48Ca, 76Ge, 82Se, 96Zr, 100Mo, 116Cd, 124Sn, 128,130Te, 136Xe(2β-); calculated 0νββ-decay and ββ-decay nuclear matrix elements (NME), correlations between obtained NMEs. Calculations with nuclear shell-model and proton-neutron quasiparticle random-phase approximation (pnQRPA) model with inclusion of two-body currents and the short-range operator. Obtained 0νββ NME using the correlation found in this work and measured ββ-decay NMEs.

doi: 10.1103/PhysRevC.107.044305
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2023RE09      Phys.Rev.Lett. 131, 052501 (2023)

B.M.Rebeiro, S.Triambak, P.E.Garrett, G.C.Ball, B.A.Brown, J.Menendez, B.Romeo, P.Adsley, B.G.Lenardo, R.Lindsay, V.Bildstein, C.Burbadge, R.Coleman, A.Diaz Varela, R.Dubey, T.Faestermann, R.Hertenberger, M.Kamil, K.G.Leach, C.Natzke, J.C.Nzobadila Ondze, A.Radich, E.Rand, H.-F.Wirth

138Ba(d, α) Study of States in 136Cs: Implications for New Physics Searches with Xenon Detectors

NUCLEAR REACTIONS 138Ba(d, α), E=22 MeV; measured reaction products, Eα, Iα; deduced energy levels, J, π, σ(θ), partial level scheme. Comparison with the shell-model results obtained with the GCN5082, SN100PN, and QX effective interactions. The Maier-Leibnitz Laboratorium in Garching, Germany.

doi: 10.1103/PhysRevLett.131.052501
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Data from this article have been entered in the XUNDL database. For more information, click here.


2022NO06      Phys.Rev. C 105, 055501 (2022)

P.Novella, M.Sorel, A.Uson, C.Adams, H.Almazan, V.Alvarez, B.Aparicio, A.I.Aranburu, L.Arazi, I.J.Arnquist, S.Ayet, C.D.R.Azevedo, K.Bailey, F.Ballester, J.M.Benlloch-Rodriguez, F.I.G.M.Borges, S.Bounasser, N.Byrnes, S.Carcel, J.V.Carrion, S.Cebrian, E.Church, C.A.N.Conde, T.Contreras, F.P.Cossio, A.A.Denisenko, G.Diaz, J.Diaz, T.Dickel, J.Escada, R.Esteve, A.Fahs, R.Felkai, L.M.P.Fernandes, P.Ferrario, A.L.Ferreira, F.W.Foss, E.D.C.Freitas, Z.Freixa, J.Generowicz, A.Goldschmidt, J.J.Gomez-Cadenas, R.Gonzalez, D.Gonzalez-Diaz, R.Guenette, R.M.Gutierrez, J.Haefner, K.Hafidi, J.Hauptman, C.A.O.Henriques, J.A.Hernando Morata, P.Herrero-Gomez, V.Herrero, J.Ho, Y.Ifergan, B.J.P.Jones, M.Kekic, L.Labarga, A.Laing, L.Larizgoitia, P.Lebrun, D.Lopez Gutierrez, N.Lopez-March, M.Losada, R.D.P.Mano, J.Martin-Albo, A.Martinez, G.Martinez-Lema, M.Martinez-Vara, A.D.McDonald, Z.E.Meziani, K.Mistry, F.Monrabal, C.M.B.Monteiro, F.J.Mora, J.Munoz Vidal, K.Navarro, D.R.Nygren, E.Oblak, M.Odriozola-Gimeno, B.Palmeiro, A.Para, J.Perez, M.Querol, A.Raymond, A.B.Redwine, J.Renner, L.Ripoll, I.Rivilla, Y.Rodriguez Garcia, J.Rodriguez, C.Rogero, L.Rogers, B.Romeo, C.Romo-Luque, F.P.Santos, J.M.F.dos Santos, A.Simon, C.Stanford, J.M.R.Teixeira, P.Thapa, J.F.Toledo, J.Torrent, J.F.C.A.Veloso, T.T.Vuong, R.Webb, J.T.White, K.Woodruff, N.Yahlali, for the NEXT Collaboration

Measurement of the 136Xe two-neutrino double-β-decay half-life via direct background subtraction in NEXT

RADIOACTIVITY 136Xe(2β-); measured Eβ, Iβ, ββ-coin; deduced event rate, T1/2 of two-neutrino double-β-decay. NEXT-White time-projection chamber loaded with Xenon operated at Laboratorio Subterraneo de Canfranc. Data from 2016-021 campaign.

doi: 10.1103/PhysRevC.105.055501
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Data from this article have been entered in the XUNDL database. For more information, click here.


2022PE11      Universe 8, 112 (2022)

J.Perez-Perez, J.C.Amare, I.Catalin Bandac, A.Bayo, S.Borjabad-Sanchez, J.M.Calvo-Mozota, L.Cid-Barrio, R.Hernandez-Antolin, B.Hernandez-Molinero, P.Novella, K.Pelczar, C.Pena-Garay, B.Romeo, A.Ortiz de Solorzano, M.Sorel, J.Torrent, A.Uson, A.Wojna-Pelczar, G.Zuzel

Radon Mitigation Applications at the Laboratorio Subterraneo de Canfranc (LSC)

RADIOACTIVITY 222Rn(α)[238U decay chain in the background]; measured γ spectra, and 222Rn concentration as a background in the context of ultra-low background in experiments for double-beta decay demonstrators NEXT-NEW and CROSS, and NEXT-100 for low background biology experiments at the underground Laboratorio Subterraneo de Canfranc (LSC).

doi: 10.3390/universe8020112
Citations: PlumX Metrics


2022RO16      Phys.Lett. B 827, 136965 (2022)

B.Romeo, J.Menendez, C.Pena-Garay

γγ decay as a probe of neutrinoless ββ decay nuclear matrix elements

RADIOACTIVITY 46,48,50,52,54,56,58Ti, 50,52,54,56,58Cr, 54,56,58,60Fe, 70,72,74,76Zn, 74,76,78,80Ge, 76,78,80,82Se, 82,84Kr, 124,126,128,130,132Te, 130,132,134Xe, 134,136Ba(2γ); calculated correlation between 2γ and neutrinoless double-beta decay nuclear matrix elements using nuclear shell model.

doi: 10.1016/j.physletb.2022.136965
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