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10C (79AJ01)(See Energy Level Diagrams for 10C) GENERAL: See also (74AJ01) and Table 10.22 [Table of Energy Levels] (in PDF or PS). Model calculations:(IR74A, IR76C). Special reactions (See also reaction 2 in (74AJ01).):(BA73PP, RI74C, BA75L, BE76DD, BU76G, AR77B). Pion reactions (See also reactions 3 and 9 here.):(GI75B, RE75, WA77A, HO77P, AM78). Astrophysical questions:(PA72L, VI76D, SI77D). Other topics:(IR74A, IR76C, VO76C). Ground state properties:(BE75Q) (Note added in proof: Q0 = -23360.74 ± 0.5 keV (J.A. Nolen, private communication): this leads to an atomic mass excess of 15699.9 ± 0.5 keV for 10C.).
10C decays with a half-life of 19.255 ± 0.053 sec to 10B*(0.7, 1.7): the branching ratios are (98.53 ± 0.02)% and (1.465 ± 0.014)% respectively (RO72C): see reaction 40 in 10B and Table 10.20 (in PDF or PS).
See (CE74E).
At Ep = 185 MeV the π- spectrum shows groups corresponding to 10C*(0, 3.36 ± 0.07, 5.28 ± 0.06, 6.63 ± 0.15). Angular distributions have been obtained for the π- corresponding to these four states. The π+/π- intensity ratio is usually >> 1 for analog states in 10Be and 10C (DA73F). The population of 10Be*(0, 3.35, 5.28) is also reported at Ep = 613 MeV (CO78M). See also (DI74F, RE75, DI76D, NO76F; theor.).
See (MO74F).
Ethresh. = 4880.6 ± 0.6 keV (RO74F); the mean of this measurement and the earlier measurement of (FR66E) leads to Q0 = -4432.84 ± 0.6 keV (RO74F). See also (FR76C). The first excited state of 10C is located at Ex = 3.3527 ± 0.0015 MeV (PA69; from γ-decay). τm for 10C*(3.35) = 155 ± 25 fsec; Γγ = 4.25 ± 0.69 meV (FI68C). Angular distributions have been measured for the n0 and n1 groups and for the neutrons corresponding to 10C*(5.2 ± 0.3) at Ep = 30 and 50 MeV. The excitation of 10C*(6.5 ± 0.3, 8.3 ± 0.3, 8.9 ± 0.3) is also reported (CL70). See also 11C in (80AJ01).
Angular distributions have been measured at E(3He) = 14 MeV (NU70; t0) and 217 MeV (WI76A; t0, t1 and t to 10C*(5.6)). The latter have been compared with microscopic calculations using a central + tensor interaction [Jπ = 0+, 2+, 2+] (WI76A). The previously reported structures at 5.28 ± 0.06 and 6.58 ± 0.06 MeV (MA66H) are best fitted by Ex = 5.22 ± 0.04 [Γ = 225 ± 45 keV], 5.38 ± 0.07 [300 ± 60 keV] and 6.580 ± 0.020 MeV [190 ± 35 keV] (SC75). [It is not clear which of the 5.2 - 5.4 MeV states is the 2+ state studied by (WI76A).] See also (74AJ01) and 13N in (81AJ01).
See (74AJ01).
See (JO77) and 12C in (80AJ01).
At Eπ+ = 49.3 MeV dσ/dΩlab = 0.65 ± 0.25 μb/sr (θ = 30°) for the transitions to 10C*(0 + 3.4) (AM78).
Angular distributions have been reported at Ep = 30.0 to 54.1 MeV [see (74AJ01)] and at 51.9 MeV (YA77; t to 12C*(0, 3.35, 5.28, 6.6)) and 80 MeV (AN77D; t to 12C*(0, 3.35, 5.3)). L = 0, 2 and 2 for 10C*(0, 3.35, 5.28 ± 0.06), and therefore Jπ = 0+, 2+ and 2+: see (BE67S, YA77) but note that the "5.28 MeV" state is probably unresolved [see reaction 6 and 10Be]. At Ep = 51.9 MeV 10C*(0, 3.4) are strongly excited and states at Ex = 5.28, 5.55 and 6.6 MeV [L = 2 --> Jπ = 2+] are weakly populated. The (p, t) angular distributions are compared with those of the (p, 3He) reaction to analog states in 10B (YA77). The excitation energy of 10C*(3.4) is 3350.0 ± 1.0 keV (BE74M). (BE67S) find Ex = 6.61 ± 0.06 MeV, Γc.m. = 300 ± 50 keV. See also (KA74C, BA77Z) (Note added in proof: Q0 = -23360.74 ± 0.5 keV (J.A. Nolen, private communication): this leads to an atomic mass excess of 15699.9 ± 0.5 keV for 10C.)
See 14C in (76AJ04).
At E(3He) = 70.3 MeV the angular distributions of the 6He ions corresponding to the population of 10C*(0, 3.35) have been measured. The group to 10C*(3.35) is much more intense than the ground state group: multi-step processes may be important (KA73C). (DE76H) suggest, on the basis of an FRDWBA analysis, that the process can be interpreted as a direct cluster transfer to both final states. See also (74AJ01).
See (DE71U).
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