A=13N (1981AJ01)

The weighted mean of the three measurements of τ_1/2 = 9.965 ± 0.005 min (1960JA12), 9.963 ± 0.009 min (1968RI15) and 9.965 ± 0.010 min (1977AZ01) is 9.965 ± 0.004 min. See also Table 13.22 (in PDF or PS) of (1970AJ04). The decay is entirely to ¹³C_g.s.: log ft = 3.667 ± 0.001 from the tables of (1971GO40). The positrons are completely polarized: see (1970AJ04). See also (1978MA1P), (1976AJ04, 1977BA48, 1978RA2A), (1979DA1D; astrophys.) and (1977AZ02, 1977RI08, 1977YO1E, 1979DE15; theor.).

2. ¹⁰B(³He, γ)¹³N Q_m = 21.637

The 90° cross sections for γ₀ and γ₂₊₃ have been measured for E(³He) = 4.8 to 14 MeV: no pronounced structures are observed (1972BE05). See also (1976AJ04) and (1974LO1B).

3. ¹⁰B(³He, n)¹²N Q_m = 1.574 E_b = 21.637

Activation cross sections have been reported for E(³He) = 1 to 30.6 MeV: there is some evidence of broad structures. See (1976AJ04), (1974LO1B) and ¹²N in (1980AJ01).

4. ¹⁰B(³He, p)¹²C Q_m = 19.6940 E_b = 21.637

Observed resonances in the yields of proton groups and of 12.7 and 15.1 MeV γ-rays are displayed in Table 13.19 (in PDF or PS). For polarization measurements see (1970AJ04) and (1976LA1F). See also (1974LO1B) and ¹²C in (1980AJ01).

5. ¹⁰B(³He, d)¹¹C Q_m = 3.197 E_b = 21.637

Activation cross sections (1976GA27) and excitation functions have been measured for E(³He) = 1 to 19 MeV: for resonances see Table 13.19 (in PDF or PS). See also (1974LO1B) and ¹¹C in (1980AJ01).

6. (a) ¹⁰B(³He, t)¹⁰C Q_m = -3.670 E_b = 21.637
(b) ¹⁰B(³He, ³He)¹⁰B

See (1976AJ04) and ¹⁰B and ¹⁰C in (1979AJ01).

7. ¹⁰B(³He, α)⁹B Q_m = 12.142 E_b = 21.637

Excitation functions for α₀ and α₁ have been measured for E(³He) = 2 to 19 MeV. Observed resonances are displayed in Table 13.19 (in PDF or PS). See also (1974LO1B) and ⁹B in (1979AJ01).

8. ¹⁰B(α, n)¹³N Q_m = 1.060

Angular distributions have been measured for E_α = 1.5 to 4.6 MeV (n₀) and ≈ 4.6 MeV (n₁, n₂₊₃) (1973VA25), and at 18.0, 19.0 and 20.2 MeV (1976DU08; n₀, n₁). See also ¹⁴N and (1976EP1A; astrophys.).

9. ¹⁰B(⁶Li, t)¹³N Q_m = 5.843

At E(⁶Li) = 18 MeV the known states of ¹³N with 6.3 < E_x < 11.7 MeV are observed, with the exception of ¹³N*(7.9, 8.92). In addition, evidence is presented for a ¹³N state at E_x = 9.00 MeV with Γ_cm = 280 ± 30 keV: it is very strongly excited and its angular distribution is similar to that for ¹³C*(9.50) in the mirror reaction (⁶Li, ³He) suggesting that these two states are analogs. Other analog assignments made on the basis of corresponding intensities in the mirror reaction are given in reaction 14 of ¹³C. The widths of ¹³N*(6.89, 7.38) are, respectively, 120 ± 30 and 70 ± 30 keV (1974HO06). See also (1970AJ04).

10. ¹⁰B(¹⁴N, ¹¹B)¹³N Q_m = 0.902

At E(¹⁰B) = 100 MeV, angular distributions are reported for the transitions to ¹³N*(0, 3.5, 7.4, 11.9) (1975NA15). See also (1976NA09, 1977MO1A) and (1976AJ04).

11. ¹¹B(³He, n)¹³N Q_m = 10.182

Neutron groups have been observed to a number of states of ¹³N: see Table 13.20 (in PDF or PS). The parameters of the first T = 3/2 state at E_x = 15.06 MeV are displayed in Table 13.7 (in PDF or PS) where they are compared with the corresponding quantities for ¹³C*(15.11) (1973AD02, 1975MA21, 1977MA16, 1979AD01). Angular distributions for n₀ have recently been reported at E(³He) = 1.70 and 1.90 MeV (1979OS10) and 5.2 to 12 MeV (1977DA18). See also ¹⁴N and (1977OS08; theor.).

12. ¹¹B(¹¹B, ⁹Li)¹³N Q_m = -12.965

See (1974AN36).

13. (a) ¹²C(p, γ)¹³N Q_m = 1.9434
(b) ¹²C(p, γp')¹²C
Q₀ = 1943.31 ± 0.32 keV (1977FR20);
Q₀ = 1944.01 ± 0.22 keV (1977HE26).

Resonances for capture radiation are displayed in Table 13.21 (in PDF or PS). No resonance is observed at E_p = 1.73 MeV [¹³N*(3.55)]: ωΓ_γ < 0.006 eV (1963YO06).

Excitation functions have been measured for E_p = 150 to 2500 keV. In addition to the first two resonances, direct radiative capture is observed. In reaction (b), studied for E_p = 610 to 2700 keV the capture γ-ray yield is dominated by a direct capture process to ¹³N*(2.36). The cascade decay ¹³N*(3.51 → 2.36) has an intensity of 8 ± 1% (1974RO29). Extrapolating the cross section to E_cm = 25 keV yields a cross section factor S = 1.45 ± 0.20 keV · b (1974RO29). A reanalysis of the data by (1980BA54) suggests S = 1.54^+0.15_-0.10 keV · b. For other discussions of astrophysical questions see (1976AJ04) and (1975ZI1A, 1976BR1H, 1976RO1Q).

At E_p = 14.2 MeV, capture radiation from the first T = 3/2 state, ¹²N*(15.06), is reported: see Table 13.7 (in PDF or PS) for the parameters and the decay modes of this state (1968DI04, 1975MA21, 1977MA16). The angular distributions of the γ-rays determine J = 3/2 for ¹³N*(15.06) (1968DI04).

Excitation functions for γ-rays have also been measured at E_p = 8.7 to 24.4 MeV (γ₀) and 19.9 to 24.4 MeV (γ₁, γ₂₊₃) (1976BE28) and at 16 to 37 MeV (γ₀) and 23 to 37 MeV (γ₂₊₃) (1976FE1C). Angular distributions of γ₀ are reported for 16.5 < E_p < 27.0 MeV by (1980WO1A; prelim.). At E_p = 40 to 100 MeV most of the γ strength is due to transitions to ¹³N*(3.5), probably to ¹³N*(3.55) [J^π = 5/2⁺] because of its single particle character. Transitions to higher states may also be indicated (1979KO05, 1979AR1G). Differential cross sections for the transitions to the ground state have been measured for E_p-bar = 10 to 17 MeV. The total E2 capture cross section are ≈ 0.2 μb and no resonance effects are observed. The E2 energy-weighted sum rule depleted over this energy range is (8.5 ± 3.3)% (1980HE04). The interference between the M1(E2) T = 3/2 resonance (¹³N*(15.06)) and the E1 GDR has been studied by (1980SN01): the E1 capture is found to be predominantly d-wave (1980SN01). At E_p-bar = 28.5 MeV, the capture is dominated by γ₂₊₃ but γ₀ and a transition to ¹³N*(8.1) are also observed (1980BL1B).

See also reaction 14, (1976AJ04), (1976TSZZ, 1977TS1A, 1979BL1F), (1974LO1B, 1979SN1A), (1977YO1F, 1978GO1F, 1979RO12; applications) and (1977AL18, 1977BA29, 1979JOZP; theor.).

14. (a) ¹²C(p, p)¹²C E_b = 1.9434
(b) ¹²C(p, 2p)¹¹B Q_m = -15.9569
(c) ¹²C(p, pα)⁸Be Q_m = -7.3667
(d) ¹²C(p, 3p)¹⁰Be Q_m = -27.1857
(e) ¹²C(p, π⁺)¹³C Q_m = -135.403

Yield curves for elastic protons, protons inelastically scattered to ¹²C*(4.4, 7.7, 9.6, 12.7, 15.1) and for γ-rays from ¹²C*(4.4, 12.7, 15.1) have been studied at many energies: see Table 13.22 (in PDF or PS) for a display of the characteristics of the observed structure. Recent yield measurements include those of (1976ME22; E_p = 0.3 to 2.0 MeV), (1976BE28; 13.8 → 24.4 MeV (12.7 MeV γ), 16.4 → 24.4 MeV (15.1 MeV γ)), (1976FE1C; 16 → 37 (4.4 MeV γ), 16 → 31 (12.7 MeV γ), 17 → 37 MeV (15.1 MeV γ)) and 22 to 27 MeV (1980HO07; (12.7 and 15.1 MeV γ)).

A phase shift analysis of the elastic scattering analyzing power for E_p-bar = 11.5 to 18.1 MeV shows four T = 1/2 states with E_x = 14.06, 16.00, 18.16 and 18.18 MeV, with J^π = 3/2⁺, 7/2⁺, 3/2⁺, 1/2^-: see Table 13.22 (in PDF or PS) (1976ME18). At E_p-bar = 19.15 to 23.34 MeV, measurements of the elastic group and the protons to ¹²C*(4.4, 12.7) locate 1/2⁺ (E1), 5/2^- (E2) and 7/2⁺ (E3) resonances below 21 MeV, 3/2⁺ (E1) and 5/2^- resonances with 21 < E_x < 22 MeV and 1/2⁺ and 3/2⁺ resonances above 22 MeV: see Table 13.22 (in PDF or PS) (1979GA13). Elastic polarization measurements are also reported at E_p-bar = 0.45 to 0.60 MeV (1979KR18; study of Mott-Schwinger interaction), E_p = 7.16 to 7.43 MeV (1977ME06), E_p-bar ≈ 14.2 MeV (1980WIZW), 36.2 MeV (1978BE49), 39.9 to 75.0 MeV (1980KA02), 52.3 to 68.2 MeV (1977EG1A), E_p = 185 MeV (1979IN01; ¹²C*(0, 4.4, 7.7, 9.6), E_p-bar = 800 MeV (1978HO05, 1978RA17) and E_p = 1 GeV (1977AL25, 1980AL09). Polarization measurements involving ¹²C*(4.4, 12.71, 15.11, 15.4, 16.1) are reported by (1978HO11) at E_p-bar = 50 and 65 MeV: a marked difference in the analyzing powers for the groups to the 1⁺ states ¹²C*(12.71, 15.11) is observed. At E_p-bar = 800 MeV analyzing powers have been measured for ¹²C*(12.7, 15.1, 18.3, 19.4): those to ¹²C*(12.7, 18.3) are negative. The values of A_y appear to be charateristic of the isospin transfer (1980MO06). For other polarization measurements see (1979KA1N; E_p-bar = 65 MeV; p₀, p₂), (1979FU1H; E_p-bar = 24.1, 26.2, 28.0 MeV; p₁; measured spin flip probability), (1979BE44; E_p-bar = 299, 380, 483 and 561 MeV), (1979LI03; ¹²C*(4.4); E_p-bar = 800 MeV), (1977NA16, 1977NA29, 1978NA18:(p, 2p); E_p-bar = 635 MeV) and the older measurements [E_p = 0.5 MeV to 3.6 GeV] listed in Tables 13.26 (in PDF or PS) in (1970AJ04) and 13.28 (in PDF or PS) in (1976AJ04). See also (1978SE01).

For total cross section measurements see (1976AJ04) and (1979SC07; E_p = 191 to 550 MeV) and (1978JA16; E_p = 0.87 GeV/c and 2.10 GeV/c). See also (1979DE31). For reaction (b) see ¹¹B in (1980AJ01) and (1979KO21). For reaction (c) see ⁸Be in (1979AJ01). For reaction (d) see (1979KO36).

Bremsstrahlung measurements are reported by (1978TR05) near the E_p = 1.7 MeV resonance and by (1976MA06, 1976MA55, 1977MU1C, 1979LE1G, 1979LE1H). See also (1979JA17, 1980LI01; theor.).

Inclusive cross sections have been measured by (1978FR12, 1979FR12, 1979KO21). For polarization measurements at E_p-bar = 316 and 516 MeV see (1978KA08). Studies of hadron multiple production are reported by (1977AV01, 1978AR1J, 1978AZ02). Spallation measurements have been carried out by (1976RO12, 1977FO04, 1978WE1D, 1979RA20). See also (1979VD02). The production of π⁺ with E_p-bar = 200 MeV (reaction (e)) is reported by (1978AU07).

15. (a) ¹²C(p, n)¹²N Q_m = -18.120 E_b = 1.9434
(b) ¹²C(p, pn)¹¹C Q_m = -18.721

The cross section for reaction (a) has been measured from threshold to E_p = 50 MeV. Resonant structure is observed corresponding to E_x = 21, 24 and , possibly ≈ 27 MeV (1968RI01). See also (1976RO10) and ¹²N in (1980AJ01).

Cross sections for reaction (b) have been measured to 300 GeV: see (1976AJ04). At E_p = 800 MeV, σ = 32.0 ± 1.0 mb (1976HO19). See also (1976BE1K).

16. (a) ¹²C(p, d)¹¹C Q_m = -16.497 E_b = 1.9434
(b) ¹²C(p, t)¹⁰C Q_m = -23.364
(c) ¹²C(p, ³He)¹⁰B Q_m = -19.6940

For polarization measurements [reaction (a)] see (1970AJ04) and (1977HA1N; E_p-bar = 27.4 MeV; d₀, d₁) and (1979HO1H; E_p-bar = 65 MeV; d₀, d₁). See also ¹¹C in (1980AJ01).

Polarization measurements involving the t₀ and t₁ groups have been carried out at E_p = 49.5 MeV (1970NE17). See also ¹⁰B and ¹⁰C in (1979AJ01).

17. ¹²C(p, α)⁹B Q_m = -7.552 E_b = 1.9434

Yield curves for α₀ have been measured over the 14.2 MeV resonance, corresponding to the first T = 3/2 state at E_x = 15.06 MeV, and from E_p = 17 to 20 MeV. The yield for the α₁ group has been determined for E_p = 17 to 21.5 MeV. Parameters of observed resonances are displayed in Table 13.22 (in PDF or PS) (1969LE18). Excitation functions for α₀ have also been measured for E_p = 18.5 to 44 MeV at a number of angles: they exhibit structures which are typically 1 MeV broad (1971GU23). See also ⁹B in (1979AJ01).

18. ¹²C(p, ⁶Li)⁷Be Q_m = -22.568 E_b = 1.9434

Excitation functions have been measured for E_p = 36 to 43 MeV: no structure is apparent (1971HO25). See also (1979RA20) and ⁶Li and ⁷Be in (1979AJ01).

19. (a) ¹²C(d, n)¹³N Q_m = -0.2812
(b) ¹²C(d, pn)¹²C Q_m = -2.2246

Measurements of angular distributions of neutrons are tabulated in Table 13.27 (in PDF or PS) of (1970AJ04) and in (1976AJ04). Recent measurements have been reported at E_d-bar = 5.74 to 9.70 MeV (1976TE03; n₀, n₁) and E_d = 13.9 and 15.25 MeV (1975AZ02; n₀, n₁, n₂₊₃).

Reaction (b) is dominated at E_d = 5.0 to 6.5 MeV and at 9.20 and 9.85 MeV by sequential decay via ¹³N*(3.51 + 3.55). At the lower energies ¹³N*(2.36) participates also: see (1976AJ04) and (1976GE20). See also ¹⁴N, (1977BA1L, 1979SI07), (1974LO1B), (1976LO1B; applications) and (1977TR09, 1978BA21; theor.).

20. (a) ¹²C(³He, d)¹³N Q_m = -3.5501
(b) ¹²C(³He, pd)¹²C Q_m = -5.4936

Angular distributions have been studied to the first eight states of ¹³N with E(³He) up to 40 MeV: see (1970AJ04, 1976AJ04). Recent measurements are reported at E(³He) = 25.4 MeV (1979SE07; d₀, d₁, d₂₊₃), E(pol. ³He) = 33.3 MeV (1976KA23; d₀, d₂₊₃) and E(³He) = 43.6 MeV (1980PE13; d₀, d₁, d₂₊₃ and d to ¹³N*(6.36, 6.89, 7.16, 7.38, 8.0, 9.0, 10.78)) and 81.4 MeV (1976KO36; d to ¹³N*(0, 2.36, 3.51 + 3.55, 7.16 + 7.38, 7.9, 10.36, 11.1, 12.08)). See also (1976RO1L). The spectroscopic factors derived by (1980PE13) are S = 0.48, 0.14, 0.53, 0.007, 0.015, < 0.009, 0.024, 0.13 and 0.064 for ¹³N*(0, 2.37, 3.55, 6.36, 6.89, 7.16, 7.38, 8.0, 10.78); S < 0.005 for ¹³N*(9.0) and evidence is presented for its 9/2⁺ character. For other values of S see (1976KA23, 1976KO36, 1979SE07). The energies and widths of the first three excited states are E_x = 2368.2 ± 2.8, 3507.8 ± 7.6 and 3549.2 ± 5.0 keV, with Γ_cm = 36.1 ± 2.8, 54.8 ± 11.5 and 46.5 ± 7.1 keV, respectively (1974BL06). Spectra obtained at E(³He) = 36 MeV at forward angles show the broad d_3/2 state at E_x = 7.9 MeV. Interfering with it is the 120 keV 3/2⁺ state at 6.89 MeV. The line shape of the 5/2⁺ state at 6.36 MeV is said to show a pronounced interference pattern (1979FU03). For reaction (b) see (1978MA42; E(³He) = 70 and 80 MeV). See also (1977BO30, 1977SA1L, 1978BA21; theor.) and ¹⁵O.

21. ¹²C(α, t)¹³N Q_m = -17.8706

Angular distributions of the t₀ groups have been measured at E_α = 56 MeV (1969GA11) and 104 MeV (1972HA08).

22. ¹²C(⁷Li, ⁶He)¹³N Q_m = -8.031

Angular distributions have been obtained at E(⁷Li) = 36 MeV for the ⁶He ions to ¹³N*(0, 3.51+3.55) (1973SC26). The spectroscopic factor for ¹³N_g.s. is 0.72 (1979ZE01).

23. ¹²C(¹⁰B, ⁹Be)¹³N Q_m = -4.642

See (1976AJ04).

24. ¹²C(¹¹B, ¹⁰Be)¹³N Q_m = -9.285

See (1974AN36). See also (1976AJ04).

25. ¹²C(¹²C, ¹¹B)¹³N Q_m = -14.014

At E(¹²C) = 93.8 MeV angular distributions involving ¹³N*(0, 3.51 + 3.55) and various ¹¹B states have been measured by (1979FU04). See also (1979HEZX) and (1976AJ04).

26. ¹²C(¹⁴N, ¹³C)¹³N Q_m = -5.607

Angular distributions involving ¹³N_g.s. and various ¹³C states [see reaction 43 in ¹³C] have been studied at E(¹⁴N) = 28 to 155 MeV: see (1976AJ04) and (1976BA16, 1976NA09). See also (1978MA1F) and (1977WE1H, 1978DZ1A, 1978NA15, 1978WE1F, 1979DO13; theor.).

27. ¹²C(¹⁶O, ¹⁵N)¹³N Q_m = -10.184

At E(¹⁶O) = 128 MeV angular distributions are reported to ¹³N*(0, 2.36, 3.55) (1979PR07; also see for reduced widths).

28. ¹²C(²⁰Ne, ¹⁹F)¹³N Q_m = -10.901

See (1979OR01; E(²⁰Ne) = 150 to 294 MeV).

29. ¹³C(π⁺, π⁰)¹³N Q_m = 2.384

See (1979MO1N) and the "GENERAL" section here.

30. (a) ¹³C(p, n)¹³N Q_m = -3.0030
(b) ¹³C(p, pn)¹²C Q_m = -4.9464

Angular distributions of n₀, n₁, n₂₊₃ have been measured for E_p = 3.1 to 50 MeV: see (1970AJ04, 1976AJ04). See also (1978WA1D). The 0° differential cross section for the n₀ group has been measured to be 4.5 ± 0.7 mb/sr at E_p = 120 MeV (1980GO07). In reaction (b) at E_p = 7.9 to 12 MeV one or both of the ¹³N states at E_x = 3.5 MeV appear to be involved (1971OT02). See also (1980BA11; theor.).

31. ¹³C(³He, t)¹³N Q_m = -2.2392

At E(³He) = 39.6 MeV, angular distributions have been obtained for the tritons corresponding to the ground state of ¹³N and to the excited states at 2.36, 3.53 ± 0.03 (unresolved), 6.36, 7.16, 7.38, 8.92 ± 0.04, 11.85 + 0.04 and 15.06 MeV. States at E_x = 9.5, 10.78 ± 0.04 and 15.98 + 0.05 MeV were also populated, the first of these weakly. The transitions to ¹³N*(7.38, 8.92, 11.85, 15.06) are L = 2 [J^π = 5/2^-, 1/2^-, 3/2^-, 3/2^-, respectively] (1969BA06). Angular distributions have also been reported at E(³He) = 14 MeV (1970NU02; t₀, t₁). For a comparison of the angular distribution to ¹³N*(8.918) and ¹³C*(9.498) at E(³He) = 43.6 MeV, see reaction 57 in ¹³C (1980PE1E).

32. ¹³C(⁶Li, ⁶He)¹³N Q_m = -5.727

Angular distributions have been measured at E(⁶Li) = 31.8 MeV (1970CH19; ¹³N*(0, 3.51 + 3.55)). See also (1979ZE01) and (1976AJ04).

33. ¹³C(¹⁴N, ¹⁴C)¹³N Q_m = -2.377

See (1976AJ04) and (1978OS06; theor.).

34. ¹³O(β⁺)¹³N Q_m = 17.762

See ¹³O.

35. ¹⁴N(γ, n)¹³N Q_m = -10.554

See ¹⁴N.

36. ¹⁴N(n, 2n)¹³N Q_m = -10.554

See (1978RY02), (1977LE1J; applications) and ¹⁵N.

37. ¹⁴N(p, d)¹³N Q_m = -8.3290

Angular distributions have been measured for deuteron groups to ¹³N*(0, 2.36, 3.51 + 3.55, 7.38, 8.92, 11.88) at many energies up to E_p = 155.6 MeV: see (1976AJ04) and by (1977GU14; E_p = 16.2 and 17.7 MeV; p₀) and (1979AO02; E_p-bar = 21 MeV; p₀). See also (1976WA15, 1978MA34; theor.).

38. ¹⁴N(d, t)¹³N Q_m = -4.2963

Angular distributions of the tritons to ¹³N*(0, 3.51, 7.38, 8.92 + (9.00) + 9.48, 11.8) have been obtained at E_d = 52 MeV and analyzed by DWBA. The spectroscopic factors for the ¹³N states [and the mirror states reached in the ¹⁴N(d, ³He)¹³C reaction] are in good agreement with theory and are additional evidence for the J^π assignments of 1/2^-, 3/2^-, 5/2^-, 1/2^-, 3/2^- and 3/2^- to these states (1968HI01). For comparisons of (d, t) and (d, ³He) angular distributions see reaction 80 in ¹³C. See also ¹⁶O in (1982AJ01).

39. (a) ¹⁴N(³He, α)¹³N Q_m = 10.024
(b) ¹⁴N(³He, pα)¹²C Q_m = 8.0808

Alpha particle groups have been observed to the first seven excited states of ¹³N, including two at E_x = 7.166 and 7.388 MeV (1962CL12; ± 8 keV). Angular distributions have been studied at many energies up to E(³He) = 45 MeV: see (1976AJ04) and (1971GU22; 4 to 10.25 MeV; α₀, α₁). Reaction (b), studied at E(³He) = 8 MeV, appears to involve some states of ¹³N, possibly ¹³N*(7.93, 8.92, 11.87) (1969HO13). See also ¹⁷F in (1982AJ01).

40. ¹⁴N(⁶Li, ⁷Li)¹³N Q_m = -3.303

An angular distribution has been measured at E(⁶Li) = 32 MeV for the transition to ¹³N_g.s. and ⁷Li*(0, 0.48). ¹³N*(2.36) was also populated (1971GR44). See also (1976AJ04) and reaction 83 in ¹³C.

41. ¹⁴N(⁹Be, ¹⁰Be)¹³N Q_m = -3.741

See (1976AJ04).

42. ¹⁴N(¹⁰B, ¹¹B)¹³N Q_m = 0.902

See (1976NA09).

43. ¹⁴N(¹⁴N, ¹⁵N)¹³N Q_m = 0.280

See (1976SW02). See also (1976AJ04).

44. ¹⁵N(p, t)¹³N Q_m = -12.9050

At E_p = 43.7 MeV, angular distributions have been obtained for the tritons corresponding to the ground state of ¹³N and the excited states at 3.51 (3/2^-), 6.38 ± 0.03 (5/2⁺), 7.38 (5/2^-), 8.93 ± 0.05 (1/2^-), 10.78 ± 0.06 (1/2^-), 11.88 ± 0.04 (3/2^-) and 15.06 (3/2^-; T = 3/2) MeV [J^π values in parentheses, as determined by DWBA analyses using intermediate-coupling wave functions to obtain the two-nucleon structure factors] (1968FL03). Detailed comparisons have been made with the (p, ³He) reaction to the mirror states in ¹³C (1968FL02, 1968FL03, 1974MA12): see reaction 87 in ¹³C. Angular distributions have also been measured for the triton groups to ¹³N*(0, 3.51 + 3.55, 7.38) at several energies in the range E_p = 24.0 to 43.5 MeV (1974PI05, 1975MI01). See also ¹⁶O in (1982AJ01).

45. ¹⁶O(γ, t)¹³N Q_m = -25.033

See ¹⁶O in (1982AJ01).

46. (a) ¹⁶O(p, α)¹³N Q_m = -5.2185
(b) ¹⁶O(p, pα)¹²C Q_m = -7.1620

Angular distributions of the α₀, α₁ and α₂ groups have been measured for E_p to 54.1 MeV: see (1970AJ04, 1976AJ04). In addition, (1972MA21) have measured the distribution of the α group to a state with E_x = 12.13 ± 0.06 MeV, Γ_cm ≈ 300 keV [J^π = 7/2^-] at E_p = 54.1 MeV. See also (1976AJ04) and ¹⁷F in (1982AJ01).

47. ¹⁶O(³He, ⁶Li)¹³N Q_m = -9.239

Angular distributions have been studied at E(³He) = 30 and 40.7 MeV for the ⁶Li ions corresponding to ¹³N_g.s. (1972OH01).

48. ¹⁶O(α, ⁷Li)¹³N Q_m = -22.566

The angular distribution for the transition to ¹³N_g.s. + ⁷Li_g.s. + 0.48 has been measured at E_α = 42 MeV (1972RU03).

49. ¹⁶O(¹⁴N, ¹⁷O)¹³N Q_m = -6.409

This reaction has been studied at E(¹⁴N) = 79 MeV (1976MO03) and 155 MeV (1975NA15, 1976NA09).

50. ¹⁸O(d, ⁷Li)¹³N Q_m = -7.901

See (1970AJ04).

51. ²⁴Mg(¹²C, ²³Na)¹³N Q_m = -9.747

See (1978NO02).