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dc.contributor.authorMarkenroth, K.-
dc.contributor.authorAxelsson, L.-
dc.contributor.authorBaxter, S.-
dc.contributor.authorGarcía Borge, María José-
dc.contributor.authorDonzaud, C.-
dc.contributor.authorFayans, S.-
dc.contributor.authorFynbo, H.O.U.-
dc.contributor.authorGoldberg, V. Z.-
dc.contributor.authorGrévy, S.-
dc.contributor.authorGuillemaud-Mueller, D.-
dc.contributor.authorJonson, B.-
dc.contributor.authorKällman, K.-M.-
dc.contributor.authorLeenhardt, S.-
dc.contributor.authorLewitowicz, M.-
dc.contributor.authorLönnroth, T.-
dc.contributor.authorManngard, P.-
dc.contributor.authorMartel, Ismael-
dc.contributor.authorMueller, A. C.-
dc.contributor.authorMukha, I.-
dc.contributor.authorNilsson, T.-
dc.contributor.authorNyman, G.-
dc.contributor.authorOrr, N.A.-
dc.contributor.authorRiisager, K.-
dc.contributor.authorRogachev, G. V.-
dc.contributor.authorSaint-Laurent, M. G.-
dc.contributor.authorSerikov, I. N.-
dc.contributor.authorShul’gina, N. B.-
dc.contributor.authorSorlin, O.-
dc.contributor.authorSteiner, M.-
dc.contributor.authorTengblad, Olof-
dc.contributor.authorThoennessen, M.-
dc.contributor.authorTryggestad, E.-
dc.contributor.authorTrzaska, W. H.-
dc.contributor.authorWenander, F.-
dc.contributor.authorWinfield, J. S.-
dc.contributor.authorWolski, R.-
dc.date.accessioned2008-09-25T13:28:27Z-
dc.date.available2008-09-25T13:28:27Z-
dc.date.issued2000-08-16-
dc.identifier.citationPhysical Review C 62(3): 034308 (2000)-
dc.identifier.issn0556-2813-
dc.identifier.urihttp://hdl.handle.net/10261/7330-
dc.description12 pages, 4 tables, 9 figures.-- PACS nrs.: 21.10.Hw; 21.10.Pc; 25.40.Ny; 27.20.+n.-
dc.description.abstractThe level structure of the unbound nucleus N-11 has been studied by C-10+p elastic resonance scattering in inverse geometry with the LISE3 spectrometer at GANIL, using a C-10 beam with an energy of 9.0 MeV/ nucleon. An additional measurement was done at the A1200 spectrometer at MSU. The excitation function above the C-10+p threshold has been determined up to 5 MeV. A potential-model analysis revealed three resonance states at energies 1.27(-0.05)(+0.18) MeV (Γ = 1.44 ± 0.2 MeV), 2.01(-0.05)(+0.15) MeV (Γ = 0.84 ± 0.2 MeV), and 3.75 ± 0.05 MeV (Γ = 0.60 ± 0.05 MeV) with the spin-parity assignments I(π)=1/2(+),1/2(-),5/2(+), respectively. Hence, N-11 is shown to have a ground state parity inversion completely analogous to its mirror partner Be-11. A narrow resonance in the excitation function at 4.33 ± 0.05 MeV was also observed and assigned spin parity 3/2(-).en_US
dc.description.sponsorshipThe work was partially supported by the National Science Foundation under Grant No. PHY95-28844. The work was also partly supported by a grant from RFBR. S.B. acknowledges the support of the REU program under Grant No. PHY94-24140.en_US
dc.format.extent158860 bytes-
dc.format.mimetypeapplication/pdf-
dc.language.isoengen_US
dc.publisherAmerican Physical Society-
dc.rightsopenAccessen_US
dc.subject[PACS] Spin, parity, and isobaric spinen_US
dc.subject[PACS] Single-particle levels and strength functionsen_US
dc.subject[PACS] Resonance reactionsen_US
dc.subject[PACS] Properties of specific nuclei listed by mass ranges: 6 ≤ A ≤ 19en_US
dc.titleCrossing the dripline to N-11 using elastic resonance scatteringen_US
dc.typeartículoen_US
dc.identifier.doi10.1103/PhysRevC.62.034308-
dc.description.peerreviewedPeer revieweden_US
dc.relation.publisherversionhttp://dx.doi.org/10.1103/PhysRevC.62.034308-
dc.type.coarhttp://purl.org/coar/resource_type/c_6501es_ES
item.openairetypeartículo-
item.cerifentitytypePublications-
item.fulltextWith Fulltext-
item.languageiso639-1en-
item.openairecristypehttp://purl.org/coar/resource_type/c_18cf-
item.grantfulltextopen-
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