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Low-lying level structure of $^{56}$Cu and its implications on the rp process

Authors :
Ong, W-J.
Langer, C.
Montes, F.
Aprahamian, A.
Bardayan, D. W.
Bazin, D.
Brown, B. A.
Browne, J.
Crawford, H.
Cyburt, R.
Deleeuw, E. B.
Domingo-Pardo, C.
Gade, A.
George, S.
Hosmer, P.
Keek, L.
Kontos, A.
Lee, I-Y.
Lemasson, A.
Lunderberg, E.
Maeda, Y.
Matos, M.
Meisel, Z.
Noji, S.
Nunes, F. M.
Nystrom, A.
Perdikakis, G.
Pereira, J.
Quinn, S. J.
Recchia, F.
Schatz, H.
Scott, M.
Siegl, K.
Simon, A.
Smith, M.
Spyrou, A.
Stevens, J.
Stroberg, S. R.
Weisshaar, D.
Wheeler, J.
Wimmer, K.
Zegers, R. G. T.
Publication Year :
2017

Abstract

The low-lying energy levels of proton-rich $^{56}$Cu have been extracted using in-beam $\gamma$-ray spectroscopy with the state-of-the-art $\gamma$-ray tracking array GRETINA in conjunction with the S800 spectrograph at the National Superconducting Cyclotron Laboratory at Michigan State University. Excited states in $^{56}$Cu serve as resonances in the $^{55}$Ni(p,$\gamma$)$^{56}$Cu reaction, which is a part of the rp-process in type I x-ray bursts. To resolve existing ambiguities in the reaction Q-value, a more localized IMME mass fit is used resulting in $Q=639\pm82$~keV. We derive the first experimentally-constrained thermonuclear reaction rate for $^{55}$Ni(p,$\gamma$)$^{56}$Cu. We find that, with this new rate, the rp-process may bypass the $^{56}$Ni waiting point via the $^{55}$Ni(p,$\gamma$) reaction for typical x-ray burst conditions with a branching of up to $\sim$40$\%$. We also identify additional nuclear physics uncertainties that need to be addressed before drawing final conclusions about the rp-process reaction flow in the $^{56}$Ni region.<br />Comment: 8 pages, accepted for Phys. Rev. C

Details

Database :
arXiv
Publication Type :
Report
Accession number :
edsarx.1704.07941
Document Type :
Working Paper
Full Text :
https://doi.org/10.1103/PhysRevC.95.055806