Author: I. Nonaka
Publisher:
ISBN:
Category :
Languages : en
Pages : 14
Book Description
Numerical Differential Cross Sections of the ([alpha], P) Reaction: I. C12
Numerical Differential Cross Sections of the ([alpha], P) Reaction: II. B1°, N14, O16 and Ne2°
Numerical Differential Cross Sections of the Scattering of Alpha Particles IV C12 - II
Author: Tōkyō Daigaku. Genshikaku Kenkyūjo
Publisher:
ISBN:
Category :
Languages : en
Pages : 25
Book Description
Publisher:
ISBN:
Category :
Languages : en
Pages : 25
Book Description
Numerical Differential Cross Sections of the Scattering of Alpha Particles III CP12 - I
Numerical Differential Cross Sections of the Scattering of Alpha Particles IV CP12 - II
Differential Cross Sections of Some ([alpha], P) Reactions
Numerical Cross Sections of the Reaction 15N(p,[alpha]) 12C Between 6.70 and 15.16 MeV of Proton Energies
DIFFERENTIAL CROSS SECTIONS FOR THE REACTIONS C12(Li6,p)O17 AND C12(Li6,d)O16 from 3.4 to 4.0 MeV.
Author: J. M. Blair
Publisher:
ISBN:
Category :
Languages : en
Pages : 6
Book Description
Absolute differential cross sections are pre sented for the reactions C12(Li6,p)O17 (ground state and first three excited states) and C12(Li6,d)O16 (ground state), for laboratory energies from 3.4 to 4.0 MeV. Total cross sec tions are about 1 mb at 4.0 MeV. Fluctuations in the angular distributions and total cross sections suggest that the reactions proceed via the compound nucleus F18 which is excited to the region of over-lapping levels. This is in con trast to the predominantly direct character of the previously studied reaction C12(Li6, alpha) N14. (Author).
Publisher:
ISBN:
Category :
Languages : en
Pages : 6
Book Description
Absolute differential cross sections are pre sented for the reactions C12(Li6,p)O17 (ground state and first three excited states) and C12(Li6,d)O16 (ground state), for laboratory energies from 3.4 to 4.0 MeV. Total cross sec tions are about 1 mb at 4.0 MeV. Fluctuations in the angular distributions and total cross sections suggest that the reactions proceed via the compound nucleus F18 which is excited to the region of over-lapping levels. This is in con trast to the predominantly direct character of the previously studied reaction C12(Li6, alpha) N14. (Author).