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NSR database version of May 24, 2024.

Search: Author = A.Mercenne

Found 12 matches.

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2024BU02      Phys.Rev. C 109, 014616 (2024)

M.Burrows, K.D.Launey, A.Mercenne, R.B.Baker, G.H.Sargsyan, T.Dytrych, D.Langr

Ab initio translationally invariant nucleon-nucleus optical potentials

doi: 10.1103/PhysRevC.109.014616
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2023HE08      J.Phys.(London) G50, 060501 (2023)

C.Hebborn, F.M.Nunes, G.Potel, W.H.Dickhoff, J.W.Holt, M.C.Atkinson, R.B.Baker, C.Barbieri, G.Blanchon, M.Burrows, R.Capote, P.Danielewicz, M.Dupuis, C.Elster, J.E.Escher, L.Hlophe, A.Idini, H.Jayatissa, B.P.Kay, K.Kravvaris, J.J.Manfredi, A.Mercenne, B.Morillon, G.Perdikakis, C.D.Pruitt, G.H.Sargsyan, I.J.Thompson, M.Vorabbi, T.R.Whitehead

Optical potentials for the rare-isotope beam era

doi: 10.1088/1361-6471/acc348
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2023LI52      Phys.Rev. C 108, 044616 (2023)

J.P.Linares Fernandez, N.Michel, M.Ploszajczak, A.Mercenne

Description of 7Be and 7Li within the Gamow shell model

doi: 10.1103/PhysRevC.108.044616
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2023ME01      Phys.Rev. C 107, L011603 (2023)

A.Mercenne, N.Michel, J.P.Linares Fernandez, M.Ploszajczak

Gamow shell model description of the 40Ca(d, p) transfer reaction

NUCLEAR REACTIONS 40Ca(d, p), E(cm)=1.853 MeV;40Ca(p, p), E(cm)=9.61 MeV; 40Ca(n, n), E(cm)=2.69 MeV; calculated σ(θ). Combined approach involving Gamow shell-model and coupled-channel method (GSM-CC). Comparison to experimental data.

NUCLEAR STRUCTURE 42Ca, 42Sc, 42Ti; calculated low-energy states, J, π. 41,42Ca; calculated S(n). 41,42Sc, 42Ti; calculated S(p). 42Ca; calculated S(2n). 42Sc; calculated S(d). 42Ti; calculated S(2p). Comparison to experimental data.

doi: 10.1103/PhysRevC.107.L011603
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2023SA50      Phys.Rev. C 108, 054303 (2023)

G.H.Sargsyan, K.D.Launey, R.M.Shaffer, S.T.Marley, N.Dudeck, A.Mercenne, T.Dytrych, J.P.Draayer

Ab initio single-neutron spectroscopic overlaps in lithium isotopes

doi: 10.1103/PhysRevC.108.054303
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2022GI05      Phys.Rev. C 105, L051301 (2022)

V.Girard Alcindor, A.Mercenne, I.Stefan, F.de Oliveira Santos, N.Michel, M.Ploszajczak, M.Assie, A.Lemasson, E.Clement, F.Flavigny, A.Matta, D.Ramos, M.Rejmund, J.Dudouet, D.Ackermann, P.Adsley, M.Assuncao, B.Bastin, D.Beaumel, G.Benzoni, R.Borcea, A.J.Boston, D.Brugnara, L.Caceres, B.Cederwall, I.Celikovic, V.Chudoba, M.Ciemala, J.Collado, F.C.L.Crespi, G.D'Agata, G.De France, F.Delaunay, C.Diget, C.Domingo-Pardo, J.Eberth, C.Fougeres, S.Franchoo, F.Galtarossa, A.Georgiadou, J.Gibelin, S.Giraud, V.Gonzalez, N.Goyal, A.Gottardo, J.Goupil, S.Grevy, V.Guimaraes, F.Hammache, L.J.Harkness-Brennan, H.Hess, N.Jovancevic, D.S.Judson Oliver, O.Kamalou, A.Kamenyero, J.Kiener, W.Korten, S.Koyama, M.Labiche, L.Lalanne, V.Lapoux, S.Leblond, A.Lefevre, C.Lenain, S.Leoni, H.Li, A.Lopez-Martens, A.Maj, I.Matea, R.Menegazzo, D.Mengoni, A.Meyer, B.Million, B.Monteagudo, P.Morfouace, J.Mrazek, M.Niikura, J.Piot, Zs.Podolyak, C.Portail, A.Pullia, B.Quintana, F.Recchia, P.Reiter, K.Rezynkina, T.Roger, J.S.Rojo, F.Rotaru, M.D.Salsac, A.M.Sanchez-Benitez, E.Sanchis, M.Senyigit, N.de Sereville, M.Siciliano, J.Simpson, D.Sohler, O.Sorlin, M.Stanoiu, C.Stodel, D.Suzuki, C.Theisen, D.Thisse, J.C.Thomas, P.Ujic, J.J.Valiente-Dobon, M.Zielinska

New narrow resonances observed in the unbound nucleus 15F

NUCLEAR REACTIONS 1H(14O, p), E=7.64 MeV/nucleon; 1H(14O, 2p), E=7.42 MeV/nucleon; measured reaction products Ep, Ip, Eγ, Iγ, protons angular distributions, pp-coin, γγ-coin, pγ-coin; deduced σ(θ), resonances properties of 14O+p system - energy, spin and width, spectroscopic factors, major amplitudes of channels. 15F; deduced levels, J, π, configurations. Data has been analyzed and interpreted in the framework of the Gamow shell model (GSM) with the coupled-channel representation (GSMCC). Beam provided by SPIRAL1 facility (GANIL). Detectors: MUST2 (telescope composed of DSSD and CsI array) for (14O, p) reaction and MUGAST array (MUST2+VAMOS magnetic spectrometer+AGATA HPGE-array).

doi: 10.1103/PhysRevC.105.L051301
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Data from this article have been entered in the XUNDL database. For more information, click here.


2022MO10      Phys.Rev. C 105, 034306 (2022)

O.M.Molchanov, K.D.Launey, A.Mercenne, G.H.Sargsyan, T.Dytrych, J.P.Draayer

Machine learning approach to pattern recognition in nuclear dynamics from the ab initio symmetry-adapted no-core shell model

NUCLEAR STRUCTURE 4He, 16O, 20Ne, 24Si, 20,22,24,26,28,30,32,34,36,38,40,42Mg, 166,168Er, 236U; calculated probability amplitudes of dominant configurations for ground states, shape coexistence and structure patterns using machine learning on ab initio symmetry-adapted no-core shell model calculations. Neural networks with training sets that include only the s- and p-shell nuclei.

doi: 10.1103/PhysRevC.105.034306
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2022SA23      Phys.Rev.Lett. 128, 202503 (2022)

G.H.Sargsyan, K.D.Launey, M.T.Burkey, A.T.Gallant, N.D.Scielzo, G.Savard, A.Mercenne, T.Dytrych, D.Langr, L.Varriano, B.Longfellow, T.Y.Hirsh, J.P.Draayer

Impact of Clustering on the 8Li β Decay and Recoil Form Factors

RADIOACTIVITY 8Li(β-), 8Be(2α); analyzed available data; calculated 8Be low-lying 0+ states, unprecedented constraints on recoil corrections, strong correlation between them and the 8Li ground state quadrupole moment using large-scale ab initio calculations.

doi: 10.1103/PhysRevLett.128.202503
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2019ME01      Phys.Rev. C 99, 044606 (2019)

A.Mercenne, N.Michel, M.Ploszajczak

Gamow shell model description of 4He (d, d) elastic scattering reactions

NUCLEAR REACTIONS 4He(d, d), E=0-12 MeV; calculated phase shifts, differential σ(E, θ) using Gamow shell model (GSM) in coupled-channel (GSM-CC) representation. Comparison with experimental data.

NUCLEAR STRUCTURE 6Li; calculated levels, J, π, and widths of T=0 states using Gamow shell model in coupled-channel approach (GSM-CC). Comparison with experimental data.

doi: 10.1103/PhysRevC.99.044606
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2017ME03      Phys.Rev. C 95, 024324 (2017)

A.Mercenne, N.Michel, J.Dukelsky, M.Ploszajczak

Solution of a pairing problem in the continuum

NUCLEAR STRUCTURE 14,16,18,20C; calculated binding energies, levels, J, π, configurations. Generalized Richardson solution for fermions interacting with the pairing interaction from rational Gaudin model in the Berggren ensemble. Accurate solutions for the Gamow shell model. Comparison with experimental data.

doi: 10.1103/PhysRevC.95.024324
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2016DE15      Phys.Lett. B 758, 26 (2016)

F.de Grancey, A.Mercenne, F.de Oliveira Santos, T.Davinson, O.Sorlin, J.C.Angeique, M.Assie, E.Berthoumieux, R.Borcea, A.Buta, I.Celikovic, V.Chudoba, J.M.Daugas, G.Dumitru, M.Fadil, S.Grevy, J.Kiener, A.Lefebvre-Schuhl, N.Michel, J.Mrazek, F.Negoita, J.Okolowicz, D.Pantelica, M.G.Pellegriti, L.Perrot, M.Ploszajczak, G.Randisi, I.Ray, O.Roig, F.Rotaru, M.G.Saint Laurent, N.Smirnova, M.Stanoiu, I.Stefan, C.Stodel, K.Subotic

An above-barrier narrow resonance in 15F

NUCLEAR REACTIONS 1H(14O, p), (14O, X)15F, E=95 MeV/nucleon; measured reaction products, Ep, Ip; deduced σ(θ), resonance energy and width, level scheme, J, π. Comparison with Gamow shell model calculations.

doi: 10.1016/j.physletb.2016.04.051
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2323. Data from this article have been entered in the XUNDL database. For more information, click here.


2016ME19      Acta Phys.Pol. B47, 967 (2016)

A.Mercenne, N.Michel, M.Ploszajczak

Approximate Solution of the Pairing Hamiltonian in the Berggren Basis

doi: 10.5506/APhysPolB.47.967
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