Properties of excited 0+ states in C14 and O14

I have computed expected energies and widths of excited ${0}^{+}$ states in $^{14}\mathrm{O}$, using experimental information from $^{14}\mathrm{C}$ and a variety of wave functions. Agreement for the ${0}_{2}$ state is fair, but my calculations do not support a recent suggestion that a previously unknown state unresolved from the second ${2}^{+}$ state might be the ${0}_{3}$ state.

[1]  A. Wuosmaa,et al.  Invariant-mass spectroscopy of O14 excited states , 2019, Physical Review C.

[2]  A. Wuosmaa,et al.  First Observation of Unbound ^{11}O, the Mirror of the Halo Nucleus ^{11}Li. , 2018, Physical review letters.

[3]  H. Fortune Energies and widths of T =1 single-particle states in 14 O and 14 N , 2015 .

[4]  H. Fortune Structure of 11 Li(g.s.) and an excited 3 /2 - state , 2015 .

[5]  H. Fortune,et al.  Potential-model estimate of the mass of 11 O(g.s.) , 2013 .

[6]  H. Fortune Systematic behavior of mirror energy differences for Z=8,10 nuclei and the mass of 15Ne , 2013 .

[7]  H. Fortune,et al.  Low-lying resonances in 14F and 14B , 2011 .

[8]  H. Fortune,et al.  Update on energy and width of {sup 19}Mg(g.s.) , 2011 .

[9]  H. Fortune Coulomb energies in {sup 16}Ne and low-lying levels of {sup 17}Na , 2010 .

[10]  C. Nociforo,et al.  Observation of Two-Proton Radioactivity of Mg-19 by Tracking the Decay Products , 2007 .

[11]  H. Fortune,et al.  Comment on "predicting narrow states in the spectrum of a nucleus beyond the proton drip line". , 2007, Physical review letters.

[12]  H. Fortune,et al.  Two-Proton Decay Energy and Width of 19 Mg(g.s.) , 2007 .

[13]  H. Fortune,et al.  Excited 0 + , T = 2 states in Be 12 , C 12 , and O 12 , 2006 .

[14]  H. Fortune,et al.  Constraints on energy ofB9(1/2+) andC10(02+) , 2006 .

[15]  H. Fortune,et al.  Coulomb energies in {sup 17}Ne and the ground state mass of {sup 18}Na , 2006 .

[16]  H. Fortune,et al.  Proton and alpha spectroscopic factors for states at 6.4–7.5 MeV in Ne 19 , 2006 .

[17]  H. Fortune Constraints on energies of 15 F(g.s.), 15 O(1/2 + , T = 3/2 ), and 16 F(0 + , T = 2) , 2006 .

[18]  H. Fortune,et al.  {sup 18}Na: Mass excess and low-lying states , 2005 .

[19]  H. Fortune,et al.  Energy shifts and configuration mixing in the A=15 quartet , 2005 .

[20]  A. Tamii,et al.  Level widths of O-14 states studied in the high-resolution N-14(He-3,t)O-14 reaction , 2005 .

[21]  H. Fortune,et al.  Low-lying levels of B 9 , 2004 .

[22]  B. A. Brown,et al.  22Mgand the21Na(p,γ)reaction rate , 2003 .

[23]  H. Fortune,et al.  Properties of states at 7–8 MeV in 18 Ne , 2003 .

[24]  H. Fortune,et al.  Structure of 16 Ne ground state , 2002 .

[25]  H. Fortune,et al.  2 p 3 / 2 strength in 4 0 , 4 1 Sc and the 39 Ca ( p , γ ) reaction rate , 2002 .

[26]  H. Fortune,et al.  Energies and widths of T=32 states in A=11 nuclei , 2001 .

[27]  H. Fortune,et al.  Structure of 17Ne ground state , 2001 .

[28]  B. A. Brown,et al.  ω γ for 19 Ne ( p , γ ) 20 Na ( 2.64 MeV ) , 2000 .

[29]  Sherr,et al.  Comment on "Stellar reactions with short-lived nuclei: 17F(p, alpha)14O" , 2000, Physical review letters.

[30]  H. Fortune,et al.  Structure of 12 Be and 12 O ground states , 1999 .

[31]  B. A. Brown,et al.  No Tetra-proton cluster in 20Mg , 1999 .

[32]  H. Fortune,et al.  Coulomb energies in 18 Ne , 1998 .

[33]  D. R. Tilley,et al.  Energy Levels of Light Nuclei A =1 6 , 1993 .

[34]  F. Ajzenberg‐Selove Energy levels of light nuclei A = 13-15 , 1991 .

[35]  R. Peterson,et al.  The 14C(α, α')14C and 13C(d, p)14C reactions , 1984 .

[36]  G. Stephans,et al.  /sup 12/C(t,p) and the ground state of /sup 14/C , 1982 .

[37]  G. E. Moore,et al.  Structure of 14C from 12C(t, p) , 1978 .

[38]  S. Cohen,et al.  Spectroscopic factors for the 1p shell , 1967 .

[39]  W. Pinkston,et al.  SHELL MODEL ASSIGNMENTS FOR THE ENERGY LEVELS OF C$sup 14$ AND N$sup 1$$sup 4$ , 1960 .