NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = S.Quaglioni Found 57 matches. 2023HL01 Phys.Rev. C 107, 014315 (2023) L.Hlophe, K.Kravvaris, S.Quaglioni Quantifying uncertainties due to irreducible three-body forces in deuteron-nucleus reactions NUCLEAR REACTIONS 2H(α, α), E(cm)<1.8 MeV; calculated elastic scattering σ(θ, E), phase shifts. Ab initio no-core shell model coupled with the resonating group method (NCSM/RGM) and Faddeev type equations. Studied the irreducible n-p-α three-body forces arising from antisymmetrization effects and quantified its impact on observables of the d+α system. Comparison to available experimental data. NUCLEAR STRUCTURE 2H, 4He, 6Li; calculated ground-state energy. Comparison of Faddeev calculations with no-core shell model coupled with the resonating group method (NCSM/RGM).
doi: 10.1103/PhysRevC.107.014315
2023KR09 Phys.Lett. B 845, 138156 (2023) K.Kravvaris, P.Navratil, S.Quaglioni, C.Hebborn, G.Hupin Ab initio informed evaluation of the radiative capture of protons on 7Be NUCLEAR REACTIONS 7Be(p, γ), E(cm)<10 MeV; analyzed available data; deduced eigenphase shifts, S-factors using a set of first-principle (or, ab initio) calculations to provide an independent prediction of the low-energy S-factor with quantified uncertainties.
doi: 10.1016/j.physletb.2023.138156
2023LU15 Eur.Phys.J. A 59, 196 (2023) P.Luchi, F.Turro, S.Quaglioni, X.Wu, V.Amitrano, K.Wendt, J.L.DuBois, F.Pederiva Control optimization for parametric Hamiltonians by pulse reconstruction
doi: 10.1140/epja/s10050-023-01108-2
2022AT02 Phys.Rev. C 105, 054316 (2022) M.C.Atkinson, P.Navratil, G.Hupin, K.Kravvaris, S.Quaglioni Ab initio calculation of the β decay from 11Be to a 10Be + p resonance RADIOACTIVITY 11Be(β-p); calculated β-delayed proton emission branching ratio, Gamow-teller transitions strength. Ab-initio no-core shell model with continuum (NCSMC). Comparison to experimental data. NUCLEAR STRUCTURE 11Be, 11B; calculated levels, J, π, diagonal phase and eigenphase shifts in 10Be+p system, spectroscopic factors, resonances. Comparison to experimental data.
doi: 10.1103/PhysRevC.105.054316
2022HE12 Phys.Rev.Lett. 129, 042503 (2022) C.Hebborn, G.Hupin, K.Kravvaris, S.Quaglioni, P.Navratil, P.Gysbers Ab Initio Prediction of the 4He(d, γ)6Li Big Bang Radiative Capture NUCLEAR REACTIONS 4He(d, γ)6Li, E<1 MeV; calculated S-factor, thermonuclear reaction rates, ground-state properties. The ab initio no-core shell model with continuum. Comparison with available data.
doi: 10.1103/PhysRevLett.129.042503
2021CH45 Phys.Rev. C 104, 024325 (2021) R.J.Charity, T.B.Webb, J.M.Elson, D.E.M.Hoff, C.D.Pruitt, L.G.Sobotka, P.Navratil, G.Hupin, K.Kravvaris, S.Quaglioni, K.W.Brown, G.Cerizza, J.Estee, W.G.Lynch, J.Manfredi, P.Morfouace, C.Santamaria, S.Sweany, M.B.Tsang, T.Tsang, K.Zhu, S.A.Kuvin, D.McNeel, J.Smith, A.H.Wuosmaa, Z.Chajecki Using spin alignment of inelastically excited nuclei in fast beams to assign spins: The spectroscopy of 13O as a test case NUCLEAR REACTIONS 9Be(13O, 13O'), E=69.5 MeV/nucleon, [secondary 13O beam from 9Be(16O, X), E=150 MeV/nucleon primary reaction, followed by separation of fragments using A1900 fragment separator at NSCL-MSU facility]; measured charged particles, angular distribution of protons in 1p- and 2p-decays of the excited states of 13O using High Resolution Array (HiRA) of 14 ΔE-E (Si-CsI(Tl)) telescopes; deduced invariant-mass distributions of the p+12N and 2p+11C events from the decay of 13O excited states. 13O; deduced levels, resonances, J, π, Γ, E(p), possibly rotational bands built on deformed cluster configurations predicted by antisymmetrized molecular dynamics (AMD) calculations. Comparison of p(θ) data with DWBA using FRESCO code, and level structure of 13O with ab initio no-core shell model with continuum (NCSMC), and with the structure of 13B mirror nucleus.
doi: 10.1103/PhysRevC.104.024325
2021HO15 Phys.Lett. B 822, 136710 (2021) M.Holl, R.Kanungo, Z.H.Sun, G.Hagen, J.A.Lay, A.M.Moro, P.Navratil, T.Papenbrock, M.Alcorta, D.Connolly, B.Davids, A.Diaz Varela, M.Gennari, G.Hackman, J.Henderson, S.Ishimoto, A.I.Kilic, R.Krucken, A.Lennarz, J.Liang, J.Measures, W.Mittig, O.Paetkau, A.Psaltis, S.Quaglioni, J.S.Randhawa, J.Smallcombe, I.J.Thompson, M.Vorabbi, M.Williams Proton inelastic scattering reveals deformation in 8He NUCLEAR REACTIONS 1H(8He, p), E=8.25 MeV/nucleon; measured reaction products, Ep, Ip. 8He; deduced σ(θ), resonance parameters, first 2+ state, quadrupole deformation parameter. Comparison with no-core shell model predictions. Charged particle spectroscopy station IRIS at TRIUMF in Canada.
doi: 10.1016/j.physletb.2021.136710
2021MC03 Phys.Rev. C 103, 035801 (2021) C.McCracken, P.Navratil, A.McCoy, S.Quaglioni, G.Hupin Microscopic investigation of the 8Li(n, γ)9Li reaction NUCLEAR STRUCTURE 8,9Li; calculated ground-state energies, levels, J, π, quadrupole and magnetic moments, B(M1). 9Li; calculated energies of bound-states and low-lying resonances with respect to the 8Li+n threshold, 8Li+n eignestates and eigenphase shifts, 3/2- g.s. cluster form factors and asymptotic normalization coefficients (ANCs). No-core shell model with continuum (NCSMC) with chiral nucleon-nucleon and three-nucleon interactions. Comparison with experimental data. NUCLEAR REACTIONS 8Li(n, γ)9Li, E<1.3 MeV; calculated capture σ(E) using NCSMC-phenomenological approach, and compared with experimental data from the NSCL-MSU Coulomb-dissociation experiment reported by 1998Ze01. 8Li(n, γ)9Li, T9=0.01-5; calculated astrophysical reaction rates from capture cross sections using NCSMC-phenomenological approach.
doi: 10.1103/PhysRevC.103.035801
2021NO04 Phys.Rev.Lett. 126, 182502 (2021) S.Novario, P.Gysbers, J.Engel, G.Hagen, G.R.Jansen, T.D.Morris, P.Navratil, T.Papenbrock, S.Quaglioni Coupled-Cluster Calculations of Neutrinoless Double-β Decay in 48Ca RADIOACTIVITY 48Ca(2β-); calculated nuclear matrix element for the neutrinoless ββ-decay using coupled-cluster theory and nuclear interactions from chiral effective field theory.
doi: 10.1103/PhysRevLett.126.182502
2020KR08 Phys.Rev. C 102, 024616 (2020) K.Kravvaris, K.R.Quinlan, S.Quaglioni, K.A.Wendt, P.Navratil Quantifying uncertainties in neutron-α scattering with chiral nucleon-nucleon and three-nucleon forces NUCLEAR REACTIONS 4He(n, n), (n, X)5He*, E(cm)<10.5 MeV; calculated phase shifts from third to fifth order of the chiral expansion in comparison to the empirical phase shifts obtained from R-matrix analysis of A=5 reaction data, phase shifts from the Gaussian process model (GPM) with local/nonlocal 3N force, Bayesian posterior distributions of low-energy constants for the contact plus one-pion exchange using the binding energies of 3H and 4He and the charge radius of 4He, positions and widths of n-α resonances. 4,5He; calculated ground-state energy, point-proton radius and charge radius, and associated chiral uncertainties using the chiral interaction models. Computation of structure and reaction observables for three-, four-, and five-nucleon systems within the ab initio frameworks of the no-core shell model and no-core shell model with continuum. Overall uncertainty budget of many-body calculations using Bayesian statistics. Comparison with experimental data.
doi: 10.1103/PhysRevC.102.024616
2019BO10 Phys.Rev. C 100, 024617 (2019) A.Bonaccorso, F.Cappuzzello, D.Carbone, M.Cavallaro, G.Hupin, P.Navratil, S.Quaglioni Application of an ab initio S matrix to data analysis of transfer reactions to the continuum populating 11Be NUCLEAR REACTIONS 9Be(18O, 16O)11Be, E=84 MeV; measured reaction products, 16O ejectiles; deduced differential cross section. Results compared to an ab initio no-core shell model calculation for continuum states. 11Be; deduced levels, wave functions of the n+10Be system. Experiment performed at the Tandem Van de Graaff facility of the Istituto Nazionale di Fisica Nucleare Laboratori Nazionali el Sud, Italy, using MAGNEX magnetic spectrometer to momentum analyze 16O particles.
doi: 10.1103/PhysRevC.100.024617
2019GY02 Nat.Phys. 15, 428 (2019) P.Gysbers, G.Hagen, J.D.Holt, G.R.Jansen, T.D.Morris, P.Navratil, T.Papenbrock, S.Quaglioni, A.Schwenk, S.R.Stroberg, K.A.Wendt Discrepancy between experimental and theoretical β-decay rates resolved from first principles NUCLEAR STRUCTURE 3H, 6Li, 7Be, 8He, 10C, 14O, 19,24Ne, 37K, 25,28Al, 24,26Na, 30Mg, 33,34P, 42,43,46Sc, 42,45Ti, 45,47V, 100Sn; calculated the Gamow–Teller strength for β decay.
doi: 10.1038/s41567-019-0450-7
2019VO06 Phys.Rev. C 100, 024304 (2019) M.Vorabbi, P.Navratil, S.Quaglioni, G.Hupin 7Be and 7Li nuclei within the no-core shell model with continuum NUCLEAR STRUCTURE 7Be, 7Li; calculated levels, resonances, J, π, cluster form factors of ground states, widths, phase shifts of 3He+4He and 6Li+p scattering for 7Be, and 3H+4He, 6Li+n, and 6He+p for 7Li. No-core shell model with continuum. Comparison with experimental data. Relevance to primordial nucleosynthesis, nuclear astrophysics, and fusion energy generation.
doi: 10.1103/PhysRevC.100.024304
2018CH12 Nucl.Data Sheets 148, 189 (2018) M.B.Chadwick, R.Capote, A.Trkov, M.W.Herman, D.A.Brown, G.M.Hale, A.C.Kahler, P.Talou, A.J.Plompen, P.Schillebeeckx, M.T.Pigni, L.Leal, Y.Danon, A.D.Carlson, P.Romain, B.Morillon, E.Bauge, F.-J.Hambsch, S.Kopecky, G.Giorginis, T.Kawano, J.Lestone, D.Neudecker, M.Rising, M.Paris, G.P.A.Nobre, R.Arcilla, O.Cabellos, I.Hill, E.Dupont, A.J.Koning, D.Cano-Ott, E.Mendoza, J.Balibrea, C.Paradela, I.Duran, J.Qian, Z.Ge, T.Liu, L.Hanlin, X.Ruan, W.Haicheng, M.Sin, G.Noguere, D.Bernard, R.Jacqmin, O.Bouland, C.De Saint Jean, V.G.Pronyaev, A.V.Ignatyuk, K.Yokoyama, M.Ishikawa, T.Fukahori, N.Iwamoto, O.Iwamoto, S.Kunieda, C.R.Lubitz, M.Salvatores, G.Palmiotti, I.Kodeli, B.Kiedrowski, D.Roubtsov, I.Thompson, S.Quaglioni, H.I.Kim, Y.O.Lee, U.Fischer, S.Simakov, M.Dunn, K.Guber, J.I.Marquez Damian, F.Cantargi, I.Sirakov, N.Otuka, A.Daskalakis, B.J.McDermott, S.C.van der Marck CIELO Collaboration Summary Results: International Evaluations of Neutron Reactions on Uranium, Plutonium, Iron, Oxygen and Hydrogen NUCLEAR REACTIONS 1H, 16O, 56Fe, 235,238U, 239Pu(n, X), E<20 MeV; analyzed available data; calculated σ, σ(θ), σ(θ, E).
doi: 10.1016/j.nds.2018.02.003
2018GA21 Phys.Rev.Lett. 121, 042501 (2018) M.Gatu-Johnson, C.J.Forrest, D.B.Sayre, A.Bacher, J.-L.Bourgade, C.R.Brune, J.A.Caggiano, D.T.Casey, J.A.Frenje, V.Yu.Glebov, G.M.Hale, R.Hatarik, H.W.Herrmann, R.Janezic, Y.H.Kim, J.P.Knauer, O.Landoas, D.P.McNabb, M.W.Paris, R.D.Petrasso, J.E.Pino, S.Quaglioni, B.Rosse, J.Sanchez, T.C.Sangster, H.Sio, W.Shmayda, C.Stoeckl, I.Thompson, A.B.Zylstra Experimental Evidence of a Variant Neutron Spectrum from the T(t, 2n)α Reaction at Center-of-Mass Energies in the Range of 16-50 KeV NUCLEAR REACTIONS 3H(t, 2n), E(cm)=16-50 keV; measured reaction products, En, In; deduced neutron spectra inferred from R-matrix analysis of the measured NTOF-spectra.
doi: 10.1103/PhysRevLett.121.042501
2018QU02 Phys.Rev. C 97, 034332 (2018) S.Quaglioni, C.Romero-Redondo, P.Navratil, G.Hupin Three-cluster dynamics within the ab initio no-core shell model with continuum: How many-body correlations and α clustering shape 6He NUCLEAR STRUCTURE 6He; calculated ground-state energy, levels, J, π, matter and point-proton radii, S(2n); analyzed role of 4He+n+n clustering and many-body correlations in the ground and low-lying continuum states of the Borromean 6He nucleus. 4He; calculated ground-state energy, matter and point-proton radii. Extended ab initio no-core shell model (NCSM) with SRG-N3LONN potential to include bound and continuum nuclear systems in the proximity of a three-body breakup threshold. Comparison with available experimental data.
doi: 10.1103/PhysRevC.97.034332
2018VO02 Phys.Rev. C 97, 034314 (2018) M.Vorabbi, A.Calci, P.Navratil, M.K.G.Kruse, S.Quaglioni, G.Hupin Structure of the exotic 9He nucleus from the no-core shell model with continuum NUCLEAR STRUCTURE 9He; calculated n+8He continuum by ab initio no-core shell model with continuum (NCSMC) formalism and chiral nucleon-nucleon interactions at N4LO; deduced unbound character of 9He, and two resonant states, J, π. Comparison with structure of 10Li and 11B. 4,6,8He; calculated ground-state energies by NCSM using the SRG-evolved N4LO nucleon-nucleon potential. Comparison with available experimental data.
doi: 10.1103/PhysRevC.97.034314
2017KU11 Phys.Rev.Lett. 118, 262502 (2017) A.Kumar, R.Kanungo, A.Calci, P.Navratil, A.Sanetullaev, M.Alcorta, V.Bildstein, G.Christian, B.Davids, J.Dohet-Eraly, J.Fallis, A.T.Gallant, G.Hackman, B.Hadinia, G.Hupin, S.Ishimoto, R.Krucken, A.T.Laffoley, J.Lighthall, D.Miller, S.Quaglioni, J.S.Randhawa, E.T.Rand, A.Rojas, R.Roth, A.Shotter, J.Tanaka, I.Tanihata, C.Unsworth Nuclear Force Imprints Revealed on the Elastic Scattering of Protons with 10C NUCLEAR REACTIONS 10C(p, p), E(cm)=4.15, 4.4 eV; measured reaction products, Ep, Ip; deduced σ(θ). Comparison with ab initio no-core shell model with continuum calculations.
doi: 10.1103/PhysRevLett.118.262502
2016CA39 Phys.Rev.Lett. 117, 242501 (2016) A.Calci, P.Navratil, R.Roth, J.Dohet-Eraly, S.Quaglioni, G.Hupin Can Ab Initio Theory Explain the Phenomenon of Parity Inversion in 11Be? NUCLEAR STRUCTURE 11Be; calculated J, π, B(E1). Comparison with experimental data.
doi: 10.1103/PhysRevLett.117.242501
2016DO04 Phys.Lett. B 757, 430 (2016) J.Dohet-Eraly, P.Navratil, S.Quaglioni, W.Horiuchi, G.Hupin, F.Raimondi 3He(α, γ)7Be and 3H(α, γ)7Li astrophysical S factors from the no-core shell model with continuum NUCLEAR REACTIONS 3He, 3H(α, γ), E<4 MeV; calculated S-factors, σ using no-core shell model. Comparison with available data.
doi: 10.1016/j.physletb.2016.04.021
2016NA12 Phys.Scr. 91, 053002 (2016) P.Navratil, S.Quaglioni, G.Hupin, C.Romero-Redondo, A.Calci Unified ab initio approaches to nuclear structure and reactions NUCLEAR REACTIONS 7Be(p, γ), 3H(d, n), E<20 MeV; calculated S-factors, elastic phase shifts, σ.
doi: 10.1088/0031-8949/91/5/053002
2016RA17 Phys.Rev. C 93, 054606 (2016) F.Raimondi, G.Hupin, P.Navratil, S.Quaglioni Deuteron-induced nucleon transfer reactions within an ab initio framework: First application to p-shell nuclei NUCLEAR REACTIONS 7Li(d, d), E=0.6-1.8 MeV; 7Li(d, p), E=0.25-2.5 MeV; calculated differential and integrated σ(E), eigenphase shifts, resonant phase shifts, contribution of dominant partial waves. Ab initio method using no-core shell model (NCS) and microscopic-cluster states in the framework of resonating group method (RGM). Comparison with experimental cross section data. Relevance to formation of nuclei in primordial and stellar nucleosynthesis. NUCLEAR STRUCTURE 7,8Li, 9Be; calculated levels, J, π. 2H; calculated ground-state and pseudostate energies. No-core shell model (NCS) approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.93.054606
2016RO27 Phys.Rev.Lett. 117, 222501 (2016) C.Romero-Redondo, S.Quaglioni, P.Navratil, G.Hupin How Many-Body Correlations and α Clustering Shape 6He NUCLEAR STRUCTURE 6He; analyzed available data; calculated g.s. energies, charge and matter radii, two-neutron separation energies.
doi: 10.1103/PhysRevLett.117.222501
2015HU04 Phys.Rev.Lett. 114, 212502 (2015) G.Hupin, S.Quaglioni, P.Navratil Unified Description of 6Li Structure and Deuterium-4He Dynamics with Chiral Two- and Three-Nucleon Forces NUCLEAR STRUCTURE 6Li; calculated energy levels, J, π, ground-state properties. No core shell model calculations. NUCLEAR REACTIONS 2H(α, d), 4He(d, d), E < 10 MeV; calculated σ(θ). Comparison with experimental data, a unified ab initio description.
doi: 10.1103/PhysRevLett.114.212502
2015LA04 Phys.Rev. C 91, 021301 (2015) J.Langhammer, P.Navratil, S.Quaglioni, G.Hupin, A.Calci, R.Roth Continuum and three-nucleon force effects on 9Be energy levels NUCLEAR STRUCTURE 9Be; calculated n-8Be phase shifts and eigenphase shifts for negative parity, levels, J, π relative to the n-8Be threshold. Calculations based on ab initio no-core shell model with continuum to include three-nucleon (3N) interactions.
doi: 10.1103/PhysRevC.91.021301
2015SC12 Phys.Rev. C 92, 014320 (2015) M.D.Schuster, S.Quaglioni, C.W.Johnson, E.D.Jurgenson, P.Navratil Operator evolution for ab initio electric dipole transitions of 4He NUCLEAR REACTIONS 4He(γ, X), E>26 MeV; calculated total photoabsorption cross section, total dipole strength through renormalized matrix elements obtained in the framework of similarity renormalization (SRG) group method with NN+3N interactions. Comparison with experimental data. NUCLEAR STRUCTURE 4He; calculated ground-state energy, point-proton root-mean-square radius, total dipole strength, and electric dipole polarizability using NN+3N Hamiltonians. The ab initio no-core shell-model calculations. Comparison with experimental results.
doi: 10.1103/PhysRevC.92.014320
2015SM03 Phys.Rev. C 92, 064314 (2015) D.Smalley, H.Iwasaki, P.Navratil, R.Roth, J.Langhammer, V.M.Bader, D.Bazin, J.S.Berryman, C.M.Campbell, J.Dohet-Eraly, P.Fallon, A.Gade, C.Langer, A.Lemasson, C.Loelius, A.O.Macchiavelli, C.Morse, J.Parker, S.Quaglioni, F.Recchia, S.R.Stroberg, D.Weisshaar, K.Whitmore, K.Wimmer Lifetime measurements of 17C excited states and three-body and continuum effects NUCLEAR REACTIONS 9Be(18C, 17C), E=74.2 MeV/nucleon, [secondary 18C beam from 9Be(22Ne, X), E=120 MeV/nucleon primary reaction using A1900 fragment separator at NSCL-MSU]; measured one-neutron knockout reaction products, Eγ, Iγ, (particle)γ-coin using GRETINA array for γ rays, and S800 spectrograph for particles, level half-lives using RDM method and a plunger device. 17C; deduced levels, J, π, B(M1). Comparison with importance-truncated no-core shell model (IT-NCSM), and importance-truncated no-core shell model with continuum (IT-NCSMC) calculations.
doi: 10.1103/PhysRevC.92.064314
2014HU17 Few-Body Systems 55, 1013 (2014) G.Hupin, S.Quaglioni, J.Langhammer, P.Navratil, A.Calci, R.Roth Progress on Light-Ion Fusion Reactions with Three-Nucleon Forces NUCLEAR REACTIONS 4He(n, n), E<16 MeV; calculated σ(θ), phase shifts. Comparison with available data.
doi: 10.1007/s00601-013-0800-4
2014HU21 Phys.Rev. C 90, 061601 (2014) G.Hupin, S.Quaglioni, P.Navratil Predictive theory for elastic scattering and recoil of protons from 4He NUCLEAR REACTIONS 4He(p, p), E<12 MeV; calculated p-4He phase shifts; σ(θ, E), centroids and widths of 3/2- and 1/2- resonances in 5Li. Comparison with several experimental results. Method involved solving the Schrodinger equation for five nucleons interacting through two and three-nucleon forces within the framework of chiral effective field theory. Relevance to ion-beam analysis of surface layers of solids, thin films, and fusion-reactor materials.
doi: 10.1103/PhysRevC.90.061601
2014KW03 Phys.Lett. B 732, 210 (2014) E.Kwan, C.Y.Wu, N.C.Summers, G.Hackman, T.E.Drake, C.Andreoiu, R.Ashley, G.C.Ball, P.C.Bender, A.J.Boston, H.C.Boston, A.Chester, A.Close, D.Cline, D.S.Cross, R.Dunlop, A.Finlay, A.B.Garnsworthy, A.B.Hayes, A.T.Laffoley, T.Nano, P.Navratil, C.J.Pearson, J.Pore, S.Quaglioni, C.E.Svensson, K.Starosta, I.J.Thompson, P.Voss, S.J.Williams, Z.M.Wang Precision measurement of the electromagnetic dipole strengths in 11Be NUCLEAR REACTIONS 196Pt(11Be, 11Be'), E=1.73, 2.09 MeV/nucleon;measured reaction products, Eγ, Iγ. 11Be; deduced yields, B(E1). Comparison with FRESCO code calculations.
doi: 10.1016/j.physletb.2014.03.049
2014RO11 Phys.Rev.Lett. 113, 032503 (2014) C.Romero-Redondo, S.Quaglioni, P.Navratil, G.Hupin 4He+n+n Continuum within an Ab initio Framework NUCLEAR STRUCTURE 6He; calculated energy levels, J, π, widths, eigenphase shifts. Ab initio theory, three-cluster Schrodinger equation.
doi: 10.1103/PhysRevLett.113.032503
2014RO23 Few-Body Systems 55, 927 (2014) C.Romero-Redondo, P.Navratil, S.Quaglioni, G.Hupin Ab Initio NCSM/RGM for Three-Body Cluster Systems and Application to 4He+n+n NUCLEAR STRUCTURE 6,4He; calculated ground state energies, diagonal phase shifts for different J, π channels. Comparison with available data.
doi: 10.1007/s00601-014-0876-5
2014SC08 Phys.Rev. C 90, 011301 (2014) M.D.Schuster, S.Quaglioni, C.W.Johnson, E.D.Jurgenson, P.Navratil Operator evolution for ab initio theory of light nuclei NUCLEAR STRUCTURE 3H; calculated rms radius as a function of SRG evolution parameter. 4He; calculated ground-state energy, rms radius, and total strength of dipole transition, renormalization percent as a function of range of Gaussian operator. The ab initio calculations using similarity renormalization group (SRG). SRG-evolved operators in the two- and three-body spaces. Importance of three-body contribution at long range.
doi: 10.1103/PhysRevC.90.011301
2013BA01 Phys.Rev.Lett. 110, 022505 (2013) S.Baroni, P.Navratil, S.Quaglioni Ab Initio Description of the Exotic Unbound 7He Nucleus NUCLEAR STRUCTURE 4,6,7He; calculated energy levels, J, π, spectroscopic factors, phase shifts. Ab Initio calculations, comparison with Green's function Monte Carlo and NCSM calculations.
doi: 10.1103/PhysRevLett.110.022505
2013BA11 Phys.Rev. C 87, 034326 (2013) S.Baroni, P.Navratil, S.Quaglioni Unified ab initio approach to bound and unbound states: No-core shell model with continuum and its application to 7He NUCLEAR STRUCTURE 4,6,7He; calculated ground-state energies, levels, J, π, spectroscopic factors, resonance centroids, widths of bound and unbound states. No-core shell model with continuum (NCSMC) with resonating group method (RGM). Comparison with previous studies and experimental data.
doi: 10.1103/PhysRevC.87.034326
2013BO19 Comput.Phys.Commun. 184, 085101 (2013) S.Bogner, A.Bulgac, J.Carlson, J.Engel, G.Fann, R.J.Furnstahl, S.Gandolfi, G.Hagen, M.Horoi, C.Johnson, M.Kortelainen, E.Lusk, P.Maris, H.Nam, P.Navratil, W.Nazarewicz, E.Ng, G.P.A.Nobre, E.Ormand, T.Papenbrock, J.Pei, S.C.Pieper, S.Quaglioni, K.J.Roche, J.Sarich, N.Schunck, M.Sosonkina, J.Terasaki, I.Thompson, J.P.Vary, S.M.Wild Computational nuclear quantum many-body problem: The UNEDF project NUCLEAR REACTIONS 3He(d, p), 7Be(p, γ), E<1MeV; 172Yb, 188Os, 238U(γ, X), E<24 MeV; calculated σ. Comparison with experimental data. NUCLEAR STRUCTURE 100Zr; calculated quadrupole deformation parameter, radii, neutron separation energy.
doi: 10.1016/j.cpc.2013.05.020
2013HU10 Phys.Rev. C 88, 054622 (2013) G.Hupin, J.Langhammer, P.Navratil, S.Quaglioni, A.Calci, R.Roth Ab initio many-body calculations of nucleon-4He scattering with three-nucleon forces NUCLEAR REACTIONS 4He(n, n), E=11, 15 MeV; 4He(p, p), E=5.95, 9.89, 7.89, 11.99 MeV; calculated scattering differential σ(E, θ), and analyzing powers. No-core shell model combined with resonating-group method (NCSM/RGM) including three-nucleon (3N) interactions. Algebraic expressions for 3N-force integration kernels. Comparison with experimental data.
doi: 10.1103/PhysRevC.88.054622
2013QU02 Phys.Rev. C 88, 034320 (2013); Erratum Phys.Rev. C 94, 019902 (2016) S.Quaglioni, C.Romero-Redondo, P.Navratil Three-cluster dynamics within an ab initio framework NUCLEAR STRUCTURE 6He; calculated ground-state energy within the 4He +n + n cluster basis for Borromean nucleus. Three-cluster dynamics within the ab initio framework of no-core shell model/resonating-group (NCSM/RGM) method.
doi: 10.1103/PhysRevC.88.034320
2012NA03 Phys.Rev.Lett. 108, 042503 (2012) Ab Initio Many-Body Calculations of the 3H(d, n)4He and 3He(d, p)4He Fusion Reactions NUCLEAR REACTIONS 3H(d, n), 3He(d, p), E<2 MeV; calculated phase shifts, S-factors. Ab-initio no-core shell model. NUCLEAR STRUCTURE 2,3H, 3,4He; calculated ground state energies, point-proton rms radii. SRG-N3LO NN potential, NCSM calculations.
doi: 10.1103/PhysRevLett.108.042503
2012NA21 Prog.Theor.Phys.(Kyoto), Suppl. 196, 117 (2012) P.Navratil, S.Quaglioni, R.Roth, W.Horiuchi Ab Initio Calculations of Light-Ion Reactions NUCLEAR REACTIONS 7Be(p, γ), E<2.5 MeV; 3H(d, n), 3He(d, p), E<1 MeV; calculated S-factors, scattering phase shifts.
doi: 10.1143/PTPS.196.117
2011FO01 Few-Body Systems 49, 11 (2011) C.Forssen, P.Navratil, S.Quaglioni The ab initio No-Core Shell Model and Light Nuclei NUCLEAR STRUCTURE 3H, 4He, 6,7,8,9,11Li; calculated ground-state energies, quadrupole and magnetic dipole moments, charge radii. Ab initio no-core shell model (NCSM), comparison with experimental results.
doi: 10.1007/s00601-010-0106-8
2011FR11 Phys.Rev.Lett. 107, 122502 (2011) J.A.Frenje, C.K.Li, F.H.Seguin, D.T.Casey, R.D.Petrasso, D.P.McNabb, P.Navratil, S.Quaglioni, T.C.Sangster, V.Yu.Glebov, D.D.Meyerhofer Measurements of the Differential Cross Sections for the Elastic n-3H and n-2H Scattering at 14.1 MeV by Using an Inertial Confinement Fusion Facility NUCLEAR REACTIONS 2,3H(n, n), E=14.1 MeV; measured reaction products En, In; deduced σ(θ). An internal confinement fusion facility.
doi: 10.1103/PhysRevLett.107.122502
2011GR08 Phys.Rev.Lett. 106, 162502 (2011) G.F.Grinyer, D.Bazin, A.Gade, J.A.Tostevin, P.Adrich, M.D.Bowen, B.A.Brown, C.M.Campbell, J.M.Cook, T.Glasmacher, S.McDaniel, P.Navratil, A.Obertelli, S.Quaglioni, K.Siwek, J.R.Terry, D.Weisshaar, R.B.Wiringa Knockout Reactions from p-Shell Nuclei: Tests of Ab Initio Structure Models NUCLEAR REACTIONS Be(10Be, n)9Be, Be(10C, n)9C, C(10C, n)9C, E=80, 120 MeV/nucleon; measured reaction products. 10Be, 10C; deduced σ, three-body forces. Variational Monte Carlo, no core shell model ab initio calculations.
doi: 10.1103/PhysRevLett.106.162502
2011NA13 Phys.Rev. C 83, 044609 (2011) Ab initio many-body calculations of deuteron-4He scattering and 6Li states NUCLEAR REACTIONS 4He(d, X), E=2.935, 6.965, 8.971, 12 MeV; calculated σ(E, θ) using no-core shell model/resonating-group method (NCSM/RGM). 6Li; deduced bound and unbound states. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.044609
2011NA30 Phys.Lett. B 704, 379 (2011) P.Navratil, R.Roth, S.Quaglioni Ab initio many-body calculation of the 7Be(p, γ)8B radiative capture NUCLEAR REACTIONS 7Be(p, γ), (p, p'), E < 7 MeV; calculated σ, σ(θ), S-factors, scattering lengths. Ab initio no-core shell model/resonating group method (NCSM/RGM). NUCLEAR STRUCTURE 7Be; calculated charge radius, quadrupole and magnetic moments, B(M1). NCSM framework.
doi: 10.1016/j.physletb.2011.09.079
2011NA39 J.Phys.:Conf.Ser. 312, 082002 (2011) P.Navratil, S.Quaglioni, R.Roth Ab Initio Theory of Light-ion Reactions NUCLEAR REACTIONS 4He(p, p), E=12, 14.32, 17 MeV; calculated σ(θ), analyzing power. 3H(n, n), E=14 MeV;3He(p, p), E=13.6 MeV; calculated phase shift, σ(θ). 7Be(p, p), E(cm)=0-6 MeV;8He(n, n), E(cm)=0-5 MeV; calculated phase shifts. 7Be(p, p'), E(cm)=0-6 MeV; calculated σ. 3He(d, p), E(cm)=8-2000 keV; calculated S-factor. Ab initio NCSM (no-core shell model) with RGM (resonating-group method); compared with available data.
doi: 10.1088/1742-6596/312/4/082002
2010NA18 Phys.Rev. C 82, 034609 (2010) P.Navratil, R.Roth, S.Quaglioni Ab initio many-body calculations of nucleon scattering on 4He, 7Li, 7Be, 12C, and 16O NUCLEAR REACTIONS 4He, 7Li, 7Be, 12C, 16O(n, n), (p, p), E not given; calculated σ, σ(θ), analyzing powers, phase shifts. No-core shell model, resonating-group method (NCSM/RGM). Comparison with experimental data. Predicted resonances for 8Li and 8B.
doi: 10.1103/PhysRevC.82.034609
2009GA23 Phys.Rev.Lett. 103, 102502 (2009); Erratum Phys.Rev.Lett. 122, 029901 (2019) D.Gazit, S.Quaglioni, P.Navratil Three-Nucleon Low-Energy Constants from the Consistency of Interactions and Currents in Chiral Effective Field Theory NUCLEAR STRUCTURE 3H, 3He; calculated binding energies, T1/2 for 3H; deduced weak dependence on the short-range correlations.
doi: 10.1103/PhysRevLett.103.102502
2009NA13 J.Phys.(London) G36, 083101 (2009) P.Navratil, S.Quaglioni, I.Stetcu, B.R.Barrett Recent developments in no-core shell-model calculations NUCLEAR STRUCTURE 3H, 4,6,8He, 6,7,8,9,10,11Li, 11Be, 7,8,9,10,11B, 12,13C, 16O;calculated rms radii, level energies, J, π, B(E1), quadrupole and magnetic moments. NUCLEAR REACTIONS 7Be(p, γ), 3He, 3H(α, γ), E ≤ 1.5, 2.5 MeV; calculated S-factor, NCSM overlap functions.
doi: 10.1088/0954-3899/36/8/083101
2009QU02 Phys.Rev. C 79, 044606 (2009) Ab initio many-body calculations of nucleon-nucleus scattering NUCLEAR REACTIONS 3H, 4He, 10Be(n, n'), E not given; 3,4He(p, p'), E not given; calculated ground state energies, σ, phase shifts. Ab-initio no-core shell model, resonating-group method using realistic interactions, coupled-channel calculations. 10,11Be; calculated level energies by NCSM calculations.
doi: 10.1103/PhysRevC.79.044606
2009ST11 Phys.Rev. C 79, 064001 (2009) I.Stetcu, S.Quaglioni, J.L.Friar, A.C.Hayes, P.Navratil Electric dipole polarizabilities of hydrogen and helium isotopes NUCLEAR STRUCTURE 3H, He, 4He; calculated electric dipole polarizability using the Schrodinger equation. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.064001
2008QU03 Phys.Rev.Lett. 101, 092501 (2008) Ab Initio Many-Body Calculations of n-3H, n-4He, p-3, 4He, and n-10Be Scattering NUCLEAR REACTIONS 3H, 4He, 10Be(n, n'), E not given; 3,4He(p, p'), E not given; calculated ground state energies, phase shifts, total σ; many body approach based on Resonating Group method and no-core shell model. NUCLEAR STRUCTURE 10,11Be; calculated energies of ground and excited states; CD-Bonn NN potential; comparison with earlier calculations; parity inversion in 11Be ground state.
doi: 10.1103/PhysRevLett.101.092501
2007QU02 Nucl.Phys. A790, 372c (2007) S.Quaglioni, I.Stetcu, S.Bacca, B.R.Barrett, C.W.Johnson, P.Navratil, N.Barnea, W.Leidemann, G.Orlandini Benchmark calculation of inclusive responses in the four-body nuclear system NUCLEAR STRUCTURE 4He; calculated quadrupole response function. No-core shell model, effective interaction hyperspherical harmonic approach.
doi: 10.1016/j.nuclphysa.2007.03.068
2007QU03 Phys.Lett. B 652, 370 (2007) The 4He total photo-absorption cross section with two- plus three-nucleon interactions from chiral effective field theory NUCLEAR STRUCTURE 4He; calculated ground-state energy, radius, dipole response functions. No-core shell model. NUCLEAR REACTIONS 4He(γ, p), (γ, n), E=20-120 MeV; calculated σ, three body interaction effects. Comparison with data.
doi: 10.1016/j.physletb.2007.06.082
2007ST05 Nucl.Phys. A785, 307 (2007) I.Stetcu, S.Quaglioni, S.Bacca, B.R.Barrett, C.W.Johnson, P.Navratil, N.Barnea, W.Leidemann, G.Orlandini Benchmark calculation of inclusive electromagnetic responses in the four-body nuclear system NUCLEAR STRUCTURE 4He; calculated ground-state energy, quadrupole and dipole response functions. No-core shell model, effective interaction hyperspherical harmonic approaches.
doi: 10.1016/j.nuclphysa.2006.12.047
2005QU04 Phys.Rev. C 72, 064002 (2005) S.Quaglioni, V.D.Efros, W.Leidemann, G.Orlandini 4He(e, e'p)3H reaction with full final-state interactions NUCLEAR REACTIONS 4He(e, e'p), E=high; calculated longitudinal response. Comparison with data.
doi: 10.1103/PhysRevC.72.064002
2004QU02 Phys.Rev. C 69, 044002 (2004) S.Quaglioni, W.Leidemann, G.Orlandini, N.Barnea, V.D.Efros Two-body photodisintegration of 4He with full final state interaction NUCLEAR REACTIONS 4He(γ, p), (γ, n), E=20-120 MeV; calculated σ, final state interaction effects. Comparison with data.
doi: 10.1103/PhysRevC.69.044002
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