CERN Accelerating science

002243944 001__ 2243944
002243944 003__ SzGeCERN
002243944 005__ 20170731221635.0
002243944 0247_ $$2DOI$$9Elsevier$$a10.1016/j.nuclphysa.2005.05.159
002243944 0248_ $$aoai:inspirehep.net:1464565$$pcerncds:CERN$$qINSPIRE:HEP$$qForCDS
002243944 035__ $$9http://inspirehep.net/oai2d$$aoai:inspirehep.net:1464565$$d2017-02-02T08:44:07Z$$h2017-02-03T05:00:09Z$$mmarcxml
002243944 035__ $$9Inspire$$a1464565
002243944 041__ $$aeng
002243944 084__ $$2PACS$$a23.40.-s
002243944 084__ $$2PACS$$a26.20.+f
002243944 084__ $$2PACS$$a27.20.+n
002243944 100__ $$aDiget, C Aa$$uAarhus U.
002243944 245__ $$aProperties of the 12 C 10 MeV state determined through β -decay
002243944 260__ $$c2005
002243944 300__ $$a16 p
002243944 520__ $$9Elsevier$$aThe β -delayed triple- α particle decay of 12 B has been measured with a setup that favours coincidence detection. A broad state in 12 C, previously reported around 10 MeV, has been seen and its properties determined through R-matrix analysis of the excitation spectrum. The spin and parity are 0 + . Interference between this state and the Hoyle state at 7.654 MeV has a marked influence on the spectrum. The coupling between the two states makes it difficult to determine the resonance energy.
002243944 542__ $$fElsevier B.V.
002243944 65017 $$2SzGeCERN$$aNuclear Physics - Experiment
002243944 6531_ $$9author$$aRadioactivity
002243944 6531_ $$9author$$a12 Be( β − ) 12 B( β − 3 α ) [produced in Ta( p , X )]
002243944 6531_ $$9author$$ameasured
002243944 6531_ $$9author$$aα -particle coincidences
002243944 6531_ $$9author$$aR-matrix analysis
002243944 6531_ $$9author$$adeduced
002243944 6531_ $$9author$$aspin and parity of levels in 12 C
002243944 6531_ $$9author$$adouble-sided Si strip detector
002243944 6531_ $$9author$$a12Be( [formula omitted]) 12B( [formula omitted]) [produced in Ta( [formula omitted])]
002243944 6531_ $$9author$$aα-particle coincidences
002243944 6531_ $$9author$$aspin and parity of levels in 12C
002243944 690C_ $$aCERN
002243944 700__ $$aBarker, F C$$uAustralian Natl. U., Canberra
002243944 700__ $$aBorge, M J G$$uMadrid, Inst. Estructura Materia
002243944 700__ $$aCederkäll, J$$uCERN
002243944 700__ $$aFedosseev, V N$$uCERN
002243944 700__ $$aFraile, L M$$uCERN
002243944 700__ $$aFulton, B R$$uYork U., England
002243944 700__ $$aFynbo, H O [email protected]$$uAarhus U.
002243944 700__ $$aJeppesen, H B$$uAarhus U.
002243944 700__ $$aJonson, B$$uGoteborg, ITP
002243944 700__ $$aKöster, U$$uCERN
002243944 700__ $$aMeister, M$$uGoteborg, ITP
002243944 700__ $$aNilsson, T$$uCERN
002243944 700__ $$aNyman, G$$uGoteborg, ITP
002243944 700__ $$aPrezado, Y$$uMadrid, Inst. Estructura Materia
002243944 700__ $$aRiisager, K$$uAarhus U.
002243944 700__ $$aRinta-Antila, S$$uJyvaskyla U.
002243944 700__ $$aTengblad, O$$uMadrid, Inst. Estructura Materia
002243944 700__ $$aTurrion, M$$uMadrid, Inst. Estructura Materia
002243944 700__ $$aWilhelmsen, K$$uGoteborg, ITP
002243944 700__ $$aÄystö, J$$uJyvaskyla U.$$uHelsinki U. Observ.$$vHelsinki Institute of Physics, University of Helsinki, FIN-00014 Helsinki, Finland
002243944 773__ $$c3-18$$pNucl. Phys. A$$v760$$y2005
002243944 960__ $$a13
002243944 980__ $$aARTICLE