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experiment
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Phys. Rev.
jan Horse The
Methodwithradioactiveion
10C2 92, 015805 (2015).
Nishina Center using the CRIB apparatus from the†18α)15 O reaction
atastrophysicalenergies
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Phys.
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pps.
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eredby the AVF
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performed again in Fall 2015. The new experiment isished in3
usedforﬁtting
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above
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5)
posit
References
10pps.
also
reportedin this Accelerator
Report .Horse M
Firstapplicationof Progress
the Trojan
represents the peak positions in 19 Ne excitation energy
6.411)
E. Tribble
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Rep. Prog.
77, 106901 (2014).
TheR.nuclear
crosssection
and Phys.
the astrophysicalfac18
15
F(p,α)
Oreactio
beam:
studyoftheobtained
from
theﬁttingprocedure.
2)
S.
Cherubinietal.,
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used
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RIKEN23) A. S. Adekola
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18
15
repre
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E.
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C83S.052801(2011).
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R.G.
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10 et al., Phys. Rev., C 83, 042801 (2011)4) A.
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the ∗9 A. Coc,
theM.
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T.shows
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105 -106
185)
S.
Cherubini
etthresholdal.: In thisreport.
∗12∗3,∗135)
F+preaction(EpositionoftheforthethKiss,
S. Bishop,=and D.Nalso reported in this Accelerator Progress Report .
6) C.
E. MeV).
BeeretTheal., redPhys.
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C 83,represent
042801 (2011)26.41
dashedGaussians
10-5000500
1000
cal facused for ﬁtting the data. The numbers above the arrows
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Ec.m. (keV)
The resultsof a pioneering experiment
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10represents
the peak 1,2)
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1d in this3) A.
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sectionspectrumas a function
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M. 18
Lairdfromet al.,thePhys.
Rev.inLett.,
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articlePhys.
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iment is5) S.
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∗1 positionort5) .
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INFN-LNS,
Catania,ItalyRev., C 83, 042801 (2011)
300 400 500 600 700 800 900∗5Center1for Nuclear Study, The University of Tokyo
Department of Physics, Tohoku University∗7 Departmentof Physics, Yamagata University
10−1∗8 Rare Isotope Science Project, Institute for Basic Science∗9 Department of Physics, Kyushu University
0100 200 300 400 500 600 700 800 900∗10 Centre de Spectrométrie Nucléaire et de SpectrométrieE (keV)
deMasse, IN2P3∗11 Institut dePhysiqueIN2P3 S-factor from thisα)15Nucléaire,O astrophysicalFig.
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The full dots are THM experimental data with
∗13 work.
TUM+∗14 the3/2Hungfor Dao
the Hospitalresonance atassumption
J π =Tran
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E = 6460 keV, the open ones corresponds to the assumption of J π = 5/2− (the diﬀerence from this lastassumption to the other possible value 1/2− and 3/2−
being negligeable within the errors). The solid and - 60 dashed lines shown in the ﬁgure are calculations presented and discussed in Ref.6) smeared to the present†

Condensed from the article in Phys. Rev. CE (keV)
92, 015805(2015)
experimentwasperformed at the RIKEN∗1 The
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Fig. 2. The
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pps.
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DepartmentofYamagata
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∗14 the30 MeV Cyclotron Center, Tran Hung Dao Hospital

E = 6460 keV, the open ones corresponds to the as-

sumption of J π = 5/2− (the diﬀerence from this last
References−1) R.
E. Tribbletoettheal., otherRep. Prog.
Phys.
77,1/2106901(2014).
and3/2−
assumption
possiblevalue
2) S.
Cherubinietal.,
ApJ
457,855,(1996).
being negligeable within the errors). The solid and3) A.
S. Adekola
et al., Phys.
C83(R) (2011).
dashedlines shownin theRev.,ﬁgure
are052801
calculations
pre6)
4) A.
M.
Laird
etal.,
Phys.
Rev.
Lett.,
110,032502(2013).
sented and discussed in Ref. smeared to the present
5) S. Cherubini et al.: In this report.
experimental resolution.
6) C. E. Beer et al., Phys. Rev., C 83, 042801 (2011)

Fig. 2. Twork
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