Structure of 
<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mi mathvariant="normal">Be</mml:mi><mml:mprescripts/><mml:none/><mml:mn>13</mml:mn></mml:mmultiscripts></mml:math>
 studied in proton knockout from 
<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mi mathvariant="normal">B</mml:mi><mml:mprescripts/><mml:none/><mml:mn>14</mml:mn></mml:mmultiscripts></mml:math>

Ribeiro, G.; Nácher, E.; Tengblad, O.; Fernández, P.; Aksyutina, Y.; Álvarez‐Pol, H.; Atar, L.; Aumann, T.; Avdeichikov, V.V.; Beceiro-Novo, S.; Bemmerer, D.; Benlliure, J.; Bertulani, C. A.; Boillos, J. M.; Boretzky, K.; Borge, María José García; Caamaño, M.; Caesar, C.; Casarejos, E.; Catford, W. N.; Cederkäll, J.; Chartier, M.; Chulkov, L. V.; Cortina-Gil, D.; Cravo, E.; Crespo, R.; Pramanik, U. Datta; Dillmann, I.; Elekes, Z.; Enders, J.; Ershova, O.; Estradé, A.; Farinon, F.; Fraile, L. M.; Freer, M.; Fynbo, H. O. U.; Galaviz, D.; Geißel, H.; Gernhäuser, R.; Golubev, P.; Göbel, K.; Hagdahl, J.; Heftrich, T.; Heil, M.; Heine, M.; Heinz, A.; Henriques, A.; Holl, M.; Hufnagel, Alexander G.; Ignatov, A.; Johansson, H.; Jonson, B.; Kalantar‐Nayestanaki, N.; Kanungo, R.; Kelić-Heil, A.; Kurz, N.; Kröll, T.; Labiche, M.; Langer, C.; Bleis, T. Le; Lemmon, R. C.; Lindberg, Simon; Machado, J.; Marganiec, J.; Movsesyan, A.; Nilsson, T.; Nociforo, C.; Panin, V.; Paschalis, S.; Perea, Á.; Petri, M.; Piétri, S.; Plag, R.; Reifarth, R.; Rigollet, C.; Riisager, K.; Rossi, D.; Röder, M.; Savran, D.; Scheit, H.; Simon, H.; Sorlin, O.; Syndikus, I.; Taylor, J. T.; Thies, R.; Velho, P.; Wagner, A.; Wamers, F.; Vandebrouck, M.; Weick, H.; Wheldon, C.; Wilson, G. L.; Wimmer, Christian; Winfield, J. S.; Woods, P. J.; Zhukov, M. V.; Zilges, A.; Zuber, Κ.

doi:10.1103/physrevc.98.024603

Cited by 11 publications

(49 citation statements)

References 59 publications

(188 reference statements)

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“…We note that the same gamma transitions were observed in Ref. [15], though with very limited statistics, while [13] observed only the 2.1 MeV transition. As can be better seen in the inset of Fig.…”

Section: Methodssupporting

confidence: 80%

“…As can be better seen in the inset of Fig. 3 (left), the 2.1 MeV one is observed in coincidence with a structure peaking at ∼0 and ∼3 MeV in the relative energy spectrum, as in [13]. The 2.7 MeV one is observed in coincidence with a structure at ∼3 MeV.…”

Section: Methodssupporting

confidence: 58%

“…Only the levels that can be clearly deduced from the present data are shown. The 2.3 MeV peak observed in the relative energy spectrum likely corresponds to the wellaccepted 5/2 + state in 13 Be, whose tail may be responsible for the ∼0 MeV transition in coincidence with the 2 + state in 12 Be (as discussed, for instance, in Ref. [17]).…”

Section: Methodsmentioning

confidence: 82%

“…This potential, although simpler than the more sophisticated AV18 [46], CD-Bonn [47] or Reid93 [48] interactions, reproduces NN observables up to 300 MeV, so it is suitable for three-body structure calculations. In order to get a realistic description of 14 Be, the 12 Be-n interactions needs to reproduce the properties of the unbound binary subsystem 13 Be. From previous fragmentation and knockout experiments, it is mostly accepted that 13 Be exhibits a low-lying s-wave state and a d-wave resonance around 2 MeV relative energy [10,11,14].…”

Section: Three-body Calculationsmentioning

confidence: 99%

“…In order to get a realistic description of 14 Be, the 12 Be-n interactions needs to reproduce the properties of the unbound binary subsystem 13 Be. From previous fragmentation and knockout experiments, it is mostly accepted that 13 Be exhibits a low-lying s-wave state and a d-wave resonance around 2 MeV relative energy [10,11,14]. There are, however, large discrepancies in the interpretation of the 13 Be spectrum from different experimental works [13,17], many of which are associated with the long-debated existence of a low-lying p-wave resonance and the contribution from excited 12 Be components [15].…”

Section: Three-body Calculationsmentioning

confidence: 99%

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Structure of 13Be probed via quasi-free scattering

et al. 2019

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We present an investigation of the structure of 13 Be obtained via a kinematically complete measurement of the (p, pn) reaction in inverse kinematics at 265 MeV/nucleon. The relative energy spectrum of 13 Be is compared to Transfer-to-the-Continuum calculations which use as structure inputs the overlaps of the 14 Be ground-state wave function, computed in a three-body model, with the unbound states of the 13 Be residual nucleus. The key role of neutron p-wave orbital in the interpretation of the low-relative-energy part of the spectrum is discussed.

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Section: Methodssupporting

confidence: 80%

Section: Methodssupporting

confidence: 58%