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

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For possible resonant structure in (a) see (76AJ04). For reaction (b) see (81AJ01, 86AJ01).<br />

See also (90HA46).<br />

6. 11 B(α, p) <strong>14</strong> C Q m =0.7842<br />

Angular distributions <strong>of</strong> p 0 have been measured at E α = 1.43 to 31.2 MeV: see (76AJ04,<br />

81AJ01, 86AJ01). At E α = 118.1 MeV angular distributions have been studied [DWBA analysis]<br />

to <strong>14</strong> C*(6.09, 6.59, 6.73, 7.01, 8.32, 9.80, 10.43[u], 10.74, 11.38[u], 11.7[u], <strong>14</strong>.67, <strong>14</strong>.87, 15.20, 16.43,<br />

16.72, 17.30, 21.40 [u]). It is suggested that one <strong>of</strong> the states at 11.7 MeV has J π =4 − and the<br />

other J π =(1, 2, 3) − , and that the state at 16.43 has J π =6 − (87AN04). At E α =48MeVan<br />

angular distribution is reported to a state at E x =23.288 ± 0.015 MeV with Γ lab =70± 3keV.<br />

The sharpness <strong>of</strong> the state suggests that J is large, and that perhaps it is a 7 − state (88BR26,<br />

and J.D. Brown, private communication). A search has been made for an 8 − state up to 26 MeV<br />

(at 20 ◦ ): the upper limit for its strength is 0.2 that for the 23.29 MeV state (J.D. Brown, private<br />

communication). See also 15 N, (89BR1J) and(88CA26; astrophys.).<br />

7. (a) 11 B( 6 Li, 3 He) <strong>14</strong> C Q m =4.8027<br />

(b) 11 B( 7 Li, α) <strong>14</strong> C Q m =18.1304<br />

Below E x =10.4 MeV, <strong>14</strong> C*(6.09, 6.73, 6.90 + 7.01, 7.34, 8.32, 9.78) are observed in both<br />

reactions at E(Li) = 34 MeV (84CL08): the states observed at higher excitation energies are<br />

displayedinTable<strong>14</strong>.5. The intensities <strong>of</strong> the 3 He and α groups in the two reactions are significantly<br />

different. Comparison <strong>of</strong> the angular distributions in reaction (a) and in the analog reaction 11 B( 6 Li,<br />

t) <strong>14</strong> N, as well as other data, leads to the assignment <strong>of</strong> analog pairs: see reaction 11 in <strong>14</strong> N. It<br />

is suggested that <strong>14</strong> C*(11.73) and not <strong>14</strong> C*(11.67) is populated in the inelastic pion scattering<br />

(84CL08). For the earlier work on reaction (b), see (76AJ04).<br />

8. 12 C(t, p) <strong>14</strong> C Q m =4.6410<br />

Observed proton groups are displayed in Table <strong>14</strong>.6. Angular distributions have been measured<br />

at E t =5.5 to23MeV[see(81AJ01)] and at 33 MeV (86CO1T; prelim.; to <strong>14</strong> C*(6.09, 6.6[u], 7.01,<br />

8.31, 10.5[u], <strong>14</strong>.87, 16.43). For other results see (86AJ01). See also 15 N.<br />

9. 12 C(α, 2p) <strong>14</strong> C Q m = −15.1731<br />

At E α = 65 MeV angular distributions have been measured to <strong>14</strong> C*(0, 6.73 ± 0.02, 8.40 ± 0.<strong>14</strong>,<br />

10.69 ± 0.05, 11.69 ± 0.06[u], <strong>14</strong>.84 ± 0.4). The two most strongly populated states (or groups <strong>of</strong><br />

states) are <strong>14</strong> C*(6.73, 10.69). J π =1 − and (6 + ,5 − ) are favored for <strong>14</strong> C*(11.69, <strong>14</strong>.84). For the<br />

latter 4 + is considered to be very unlikely: see (86AJ01). See also (81AJ01) for the earlier work.<br />

15

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