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13B (1991AJ01)
(See Energy Level Diagrams for 13B)
GENERAL: See also (1986AJ01) and 
13.1 [Table of Energy
Levels] (in PDF or PS) here.
Model calculations: (1988WO04, 1989PO1K, 1989WO1E).
Complex reactions involving 13B: (1985BO1A, 1986AV1B, 1986BI1A, 1986UT01, 1987AN1A, 1987BA38, 1987SA25, 1987VI02, 1988CA06, 1988RU01, 1988SA19, 1989KI13, 1989SA10, 1989YO02, 1990HA46).
Muon and neutrino capture and reactions: (1985KO39).
Pion capture and reactions (See also reactions 5 and 6): (1985SA06, 1988HA12, 1989JE02).
Hypernuclei: (1986FE1A, 1986ME1F, 1986WU1D, 1988MA1G, 1989BA92).
Antinucleon interactions: (1988MA48).
Other topics: (1985AN28, 1986AN07).
Ground-state properties of 13B: (1985AN28, 1988VA03, 1988WO04, 1989SA10, 1989WO1E, 1990LO10).
μ = +3.17778(51) nm (1978LEZA).
Interaction cross sections at 790 MeV/A for 13B ions with Be, C, and Al are reported by (1988TA10). The interaction radius and the r.m.s. radius for the nucleon distribution in 13B have also been derived (1988TA10).
| 1. 13B(β-)13C | Qm = 13.437 |
The half-life of 13B is 17.36 ± 0.16 ms: see (1981AJ01). See also (1988SA04). The branching
ratios to various 13C states are shown in 
13.2 (in PDF or PS): they indicate Jπ =
1/2- or 3/2- for 13Bg.s.. See also (1989PO1K, 1989SA1P, 1989WO1E; theor.).
| 2. 7Li(7Li, p)13B | Qm = 5.962 |
Observed proton and γ-ray groups are shown in 
13.3 (in PDF or PS). See also 14C.
| 3. 11B(t, p)13B | Qm = -0.233 |
Observed proton groups are displayed in 13.3 (in PDF or PS).
| 4. 12C(13C, 12N)13B | Qm = -30.776 |
See (1986VO02, 1988VO06) and 12N in (1990AJ01).
| 5. 13C(γ, π+)13B | Qm = -153.006 |
At Ee = 195 MeV the 13B Ex region to 12 MeV has been
studied by (1983MI06):
they find that the photopion reaction predominantly excites M2 states at low q and M4
states at high q. Fits to the data are obtained by assuming the excitation of
13Bg.s. and 13B*(3.5, 6.4, 9.0) [the latter are clearly
due to unresolved groupings of levels]. Comparisons are made with the 13C(e,
e') work in the analog region in 13C (1983MI06). [For T = 3/2
states see 
13.6 (in PDF or PS).] For other work on this reaction see (1986AJ01). See also reaction 40 in 13C, the
"General" section and (1986SI07; theor.).
| 6. 13C(π-, γ)13B | Qm = 126.131 |
Gamma rays have been observed which are associated with the 13B ground state; an unresolved doublet at Ex ≈ 3.5 - 3.7 MeV; sharp states at Ex ≈ 6.5 and 7.6 MeV; a broad level (or unresolved levels) at ≈ 10.2 MeV (1983MA16; see for radiative capture branching ratios). The analogs of the peaks at Ex = 6.5, 7.6 and 10.2 MeV, calculated to be at 13C*(21.6, 22.7, 25.3), are attributed to a ΔL = 1, ΔS = 1, ΔT = 1 spin-isospin giant dipole resonance of 13C (1983MA16). See also the "General" section.
| 7. 13C(n, p)13B | Qm = -12.655 |
The 0° ground-state differential cross section has been measured at En = 198 MeV (1988JA01). At En = 65 MeV, 13B*(0, 3.5) and the region from 6 - 10 MeV have been studied (1986WAZU; prelim.). See also (1986FO1E, 1987BR32, 1989SOZY, 1989SOZW) and (1986ALZJ).
| 8. 13C(d, 2p)13B | Qm = -14.880 |
At Ed = 70 MeV the angular distribution to 13Bg.s. has been reported. Structures at Ex = 3.8, 5.2, 6.6 MeV are also observed. For VAP measurements see 15N (1986MO27).
| 9. 13C(7Li, 7Be)13B | Qm = -14.299 |
At E(7Li) = 21 MeV/A, forward angular distributions are reported to 13Bg.s. and to unresolved structures at 3.5, 4.0, 5.1, 6.3, 7.0 and 7.6 MeV, and to a broad (Γ ≈ 2.3 MeV) structure at 9.5 MeV. The latter is suggested to be due to the GDR (1990NA03) [see for possible Jπ assignments].
| 10. 14C(γ, p)13B | Qm = -20.832 |
See (1987GO09; theor.).
| 11. 14C(t, α)13B | Qm = -1.017 |
See (1986AJ01).