Proton and deuteron radiative capture to A = 13 nuclei

[1]  M. Anghinolfi,et al.  Proton and deuteron radiative capture in light nuclei , 1988 .

[2]  Stephens,et al.  Gamma decay of isovector giant resonances built on highly excited states in 111Sn. , 1986, Physical review letters.

[3]  Matts Roos,et al.  MINUIT-a system for function minimization and analysis of the parameter errors and correlations , 1984 .

[4]  M. Anghinolfi,et al.  Anticoincidence scintillator spectrometer for photon energies up to 100 MeV , 1983 .

[5]  C. D. Atti,et al.  Antisymmetry and orthogonality effects in single-particle models of (γ, p) reactions , 1983 .

[6]  M. Anghinolfi,et al.  Computed response functions of large NaI spectrometers at photon energies above 20 MeV , 1983 .

[7]  M. Anghinolfi,et al.  Proton capture by 11B above the giant resonance , 1983 .

[8]  D. Dowell,et al.  Excited-State Giant Dipole Resonances in (p, γ): A New Probe of Single-Particle Strengths , 1983 .

[9]  J. M. Lafferty,et al.  Examination of direct radiative capture formalism , 1982 .

[10]  M. Anghinolfi,et al.  The response function of large NaI detectors to high energy photons , 1981 .

[11]  J. Bussoletti,et al.  Investigation of the electric quadrupole strength in 13N using the 12C(p, γ0)13N reaction , 1980 .

[12]  G. Ricco,et al.  An energy-independent nonlocal potential model. II. The asymmetry term , 1980 .

[13]  P. Ottaviani,et al.  Photoreactions in 13C in the 2p-1h continuum shell model , 1977 .

[14]  G. Ricco,et al.  An Energy-independent Nonlocal Potential Model for Bound and Scattering States* , 1976 .

[15]  R. Helmer,et al.  High-energy levels in 13N (II) , 1976 .

[16]  D. Johnson,et al.  High-Energy Levels in 13N , 1973 .

[17]  G. E. Brown.  Direct and semi-direct (p, γ) and (n, γ) reactions , 1964 .

[18]  F. A. Nikolaev,et al.  The 12C(p, γ) reaction from 10 to 50 MeV , 1963 .