The disintegration of B10 and F19 by fast neutrons

The disintegration of B10 and F19 by fast neutrons has been studied using a grid-type ionization chamber filled with argon and boron trifluoride enriched in B10. Monoenergetic neutrons for studying the reactions from 0.2 to 8.2 MeV were produced with the Li7 (p, n)Be7, T(p, n)He3 and D(d, n)He3 reactions. Alpha groups from the B10((n, α)Li7 reaction leaving Li7 in its ground and first excited state at 478 keV were studied over the entire energy range. The cross section for the (n, α) reaction decreased rapidly from 1048 mb at 0.2 MeV to 180 mb at 1.2 MeV and then increased to 451±60 mb at the 1,84 MeV resonance. For higher energies broad resonance structure was observed with the cross section generally decreasing and reaching a value of 31 mb at 8.2 MeV. The B10(n, t2α) reaction was observed for neutron energies above 1.3 MeV. The cross section for this reaction increased to 80 mb at 4.5 MeV and was comparable to that for the B10(n, α)Li7 reaction above 5 MeV. The B10 (n, t2α) reaction was found to proceed mainly by three-body breakup or through the 4.63 MeV excited state of Li7. Some reactions may have proceeded through the 2.9 MeV level of Be8 but few, if any, proceeded through the ground state of Be8. The total excitation function for the F19(n, α)N16 reaction leaving N16 in the ground and first three excited states was studied for neutron energies above 2.9 MeV. Ten resonances were observed. The cross section increases to 135±50 mb at 5.80 MeV and then decreases at higher energies.

[1]  F. Ajzenberg‐Selove,et al.  Energy levels of light nuclei. VI , 1959 .

[2]  J. K. Bair,et al.  Elastic Scattering Angular Distributions of Fast Neutrons on Light Nuclei , 1955 .

[3]  D. B. James,et al.  THE PULSE HEIGHT DISTRIBUTION FROM BORON TRIFLUORIDE PROPORTIONAL COUNTERS IRRADIATED WITH 4.87-MEV. NEUTRONS , 1955 .

[4]  R. L. Macklin,et al.  Total Neutron Yields from Light Elements under Proton and Alpha Bombardment , 1959 .

[5]  J. Harvey,et al.  DESIGN OF GRID IONIZATION CHAMBERS , 1949 .

[6]  J. P. Conner,et al.  Preparation of Thin Tritium Targets , 1951 .

[7]  L. Goldberg,et al.  A Connexion Between the Granulation and the Structure of the Low Chromosphere , 1957, Nature.

[8]  M. E. Wyman,et al.  (n,t) CROSS SECTIONS FOR B$sup 10$, B$sup 11$, AND Be$sup 9$ , 1958 .

[9]  G. Frye,et al.  B$sup 10$(n,t2$alpha$) AND B$sup 10$(n,dn'2$alpha$) REACTIONS FOR 6-20 MEV NEUTRONS , 1956 .

[10]  E. Titterton,et al.  Ground-State Transitions in the Reaction 10B(n,t)8Be , 1957, Nature.

[11]  S. A. Korff,et al.  Effect of Gaseous Impurities on BF3 Proportional Counters , 1960 .

[12]  J. Chadwick,et al.  Disintegration by Slow Neutrons , 1935, Nature.

[13]  J. Seagrave,et al.  The Pickup Reactions B 10 (n, d)Be 9 for 14-Mev Neutrons , 1954 .

[14]  H. Barschall,et al.  Total Cross Sections of Light Elements for (α, n) Neutrons , 1956 .

[15]  G. C. Hanna,et al.  THE ENERGY OF ALPHA PARTICLES FROM U234, U238, AND Th232 , 1957 .

[16]  A. O. Hanson,et al.  A Neutron Detector Having Uniform Sensitivity from 10 Kev to 3 Mev , 1947 .

[17]  J. Perkin THE FAST NEUTRON DISINTEGRATION OF C$sup 12$ AND B$sup 1$$sup 0$ , 1951 .

[18]  M. Goldhaber,et al.  Detection of Nuclear Disintegration in a Photographic Emulsion , 1935, Nature.

[19]  D. Miller,et al.  Total Cross Sections of Light Nuclei for p , T -Neutrons , 1951 .

[20]  J. Marion,et al.  NEUTRON-INDUCED REACTIONS IN FLUORINE , 1955 .

[21]  J. E. Brolley,et al.  MONOENERGETIC NEUTRON TECHNIQUES IN THE 10- TO 30-MEV RANGE , 1956 .

[22]  H. Bichsel,et al.  The disintegration of nitrogen by fast neutrons , 1959 .

[23]  D. Miller,et al.  Disintegration of Boron by Fast Neutrons , 1951 .