Single-Proton Removal Reaction Study of $^{16}$B
J.L. Lecouey
(1)
,
N.A. Orr
(1)
,
F.M. Marqués
(1)
,
N.L. Achouri
(1)
,
J.C. Angélique
(1)
,
B.A. Brown
(2)
,
F. Carstoiu
(1, 3)
,
W.N. Catford
(4)
,
N.M. Clarke
(5)
,
M. Freer
(5)
,
B.R. Fulton
(6)
,
S. Grévy
(1)
,
F. Hanappe
(7)
,
K.L. Jones
(4)
,
M. Labiche
(1)
,
R.C. Lemmon
(4)
,
A. Ninane
(8)
,
E. Sauvan
(1)
,
K.M. Spohr
(9)
,
L. Stuttge
(10)
1
LPCC -
Laboratoire de physique corpusculaire de Caen
2 National Superconducting Cyclotron Laboratory
3 NIPNE - Horia Hulubei National Institute of Physics and Nuclear Engineering
4 Department of Physics
5 Institute for Neuromuscular Research
6 Department of Physics
7 PNTPM
8 Slashdey Integrated Systems Solutions
9 School of Engineering and Science
10 IPHC - Institut Pluridisciplinaire Hubert Curien
2 National Superconducting Cyclotron Laboratory
3 NIPNE - Horia Hulubei National Institute of Physics and Nuclear Engineering
4 Department of Physics
5 Institute for Neuromuscular Research
6 Department of Physics
7 PNTPM
8 Slashdey Integrated Systems Solutions
9 School of Engineering and Science
10 IPHC - Institut Pluridisciplinaire Hubert Curien
N.A. Orr
- Fonction : Auteur
- PersonId : 940479
- ORCID : 0000-0002-8499-8693
F.M. Marqués
- Fonction : Auteur
- PersonId : 941129
- ORCID : 0000-0002-9456-6448
N.L. Achouri
- Fonction : Auteur
- PersonId : 940560
- ORCID : 0000-0003-4411-6796
- IdRef : 069739773
J.C. Angélique
- Fonction : Auteur
- PersonId : 829693
- ORCID : 0000-0003-0032-2870
- IdRef : 123532566
Résumé
The low-lying level structure of the unbound system $^{16}$B has been investigated via single-proton removal from a 35 MeV/nucleon $^{17}$C beam. The coincident detection of the beam velocity $^{15}$B fragment and neutron allowed the relative energy of the in-flight decay of $^{16}$B to be reconstructed. The resulting spectrum exhibited a narrow peak some 85 keV above threshold. It is argued that this feature corresponds to a very narrow (GAMMA ≪100 keV) resonance, or an unresolved multiplet, with a dominant PI(p3/2)$^{−1=$ ⊗ V(d$^{3}$$_{5/2}$)J=3/2+ PI(p3/2)$^{−1}$ ⊗ V (d$^{2}$$_{5/2, s1/2}$)J=3/2+ configuration which decays by d-wave neutron emission.