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Energy Levels of Light Nuclei A = 14 - Triangle Universities Nuclear ...

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polynominals and fitted the coefficients at resonances corresponding to <strong>14</strong> N*(13.16, 13.24, 13.67,<br />

13.76) obtaining J π =1 + ,2 − ,2or3 + , and 1, respectively, for these states. However, an R-matrix<br />

analysis by (83CS03) suggests J π =2 − ,3 + ,1 + for <strong>14</strong> N*(13.69, 13.74, 13.77). (75WI04) finds that<br />

a surprising proportion <strong>of</strong> states have a higher cross section for neutron than for proton emission:<br />

the fluctuations <strong>of</strong> σ n /σ p at low E α suggest sizable isospin impurities in the <strong>14</strong> N states.<br />

4. (a) 10 B(α, d) 12 C Q m =1.3401 E b =11.6125<br />

(b) 10 B(α, t) 11 C Q m = −11.1244<br />

Excitation curves have been measured at E α up to 27 MeV [see (70AJ04, 76AJ04, 81AJ01)].<br />

The low energy resonances are exhibited in Table <strong>14</strong>.12. At the higher energies the yield curves<br />

are fairly smooth although broad resonances in the d 1 and d 0 yields corresponding to <strong>14</strong> N*(23.25),<br />

respectively have been reported as has a sharp rise in the 15.1 MeV γ yield ≈ 1MeVabovethe<br />

12 C* (15.1) + p + n threshold, a channel which is not isospin forbidden: see (81AJ01). For cross<br />

sections at E α =29.5 MeV (reaction (a)) and 25.0 and 30.1 MeV (reaction (b)) see (83VA28). See<br />

also 12 Cin(90AJ01) and(89VA07).<br />

5. 10 B(α, α) 10 B E b =11.6125<br />

The yield <strong>of</strong> α-particles [and <strong>of</strong> 0.7 MeV γ-rays for E α =2.1 to 3 MeV] has been measured for<br />

E α to 50.6 MeV: see (81AJ01). Observed resonances are displayed in Table <strong>14</strong>.12. In addition to<br />

two strong resonances in the α 0 yields at E α =2.21 and 4.26 MeV ( <strong>14</strong> N*(13.19, <strong>14</strong>.66)), two other<br />

states ( <strong>14</strong> N*(13.72, <strong>14</strong>.25)) are required to fit the data: an R-matrix calculation leads to J π =3 + ,<br />

1 + [see, however, (75WI04)], 3 + and 2 − for <strong>14</strong> N*(13.19, 13.72, <strong>14</strong>.25, <strong>14</strong>.66): see (81AJ01).<br />

6. 10 B( 6 Li, d) <strong>14</strong> N Q m =10.1374<br />

States with E x > 10 MeV studied in this reaction at E( 6 Li) = 34 MeV are displayed in Table<br />

<strong>14</strong>.13 (84CL08). In addition most <strong>of</strong> the lower-lying T = 0 states have been populated: see (70AJ04,<br />

81AJ01).<br />

7. 10 B( 7 Li, t) <strong>14</strong> N Q m =9.<strong>14</strong>46<br />

At E( 7 Li) = 24 MeV angular distributions <strong>of</strong> the tritons to <strong>14</strong> N*(3.95, 5.83, 6.45, 8.96, 9.13,<br />

10.06, 10.81, 12.79 + 12.81, 13.03, 15.26) have been studied. <strong>14</strong> N*(4.91, 5.11, 5.69, 6.20, 7.03, 7.97,<br />

8.49, 8.98, 9.39, 11.05, 11.51, 12.42) are also populated: see (81AJ01).<br />

8. 10 B( 9 Be, αn) <strong>14</strong> N Q m =10.0390<br />

For cross sections see (86CU02).<br />

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