Non-electric-dipole photofission of 235U

The electrofission cross section for 235U has been measured from 5.8 to 22 meV. From a combined analysis of this and the photofission cross section measured previously, using the virtual-photon formalism, the photofission cross section for excitations other than E1 has been determined.

[1]  J. Arruda-Neto.  Observation of E2-fission decay for232Th from electro- and photoinduced reactions , 1984 .

[2]  J. Arruda-Neto.  Splitting of isoscalar giant resonances in actinide nuclei , 1984 .

[3]  J. Arruda-Neto.  Coincident-inclusive electrofission angular correlations , 1984 .

[4]  E. Hayward,et al.  Experimental test of virtual photon theory , 1983 .

[5]  A. Richter.  Inelastic Electron Scattering, Fine Structure of M1 Giant Resonances and Gamow-Teller States , 1983 .

[6]  H. Machner,et al.  Fission decay of isoscalar giant resonances excited in 172 MeV α scattering from 238U , 1982 .

[7]  B. Berman,et al.  Electrofission of 234U, 236U and 238U: Angular distributions and E2 strength functions , 1982 .

[8]  A. Vannucci,et al.  Concentration of E2 strength near the fission barrier of /sup 232/Th , 1982 .

[9]  H. Maier,et al.  Investigation of the Fission Decay of the Isoscalar Giant Quadrupole Resonance inU238by Electron- and Positron-Induced Fission , 1981 .

[10]  B. Berman,et al.  Fission decay of the giant quadrupole resonance for /sup 234/U , 1981 .

[11]  S. S. Hanna.  Coincidence experiments in inelastic electron scattering from highly excited states , 1981 .

[12]  D. Horen,et al.  Measurement of the fission decay of the giant quadrupole resonance in 238U , 1981 .

[13]  B. Herman,et al.  Study of electrofission and hadron-induced fission decay of the giant quadrupole resonance of 238U , 1980 .

[14]  B. Berman,et al.  E2 giant resonances and an M1 component in the photofission of /sup 236/U , 1980 .

[15]  B. Berman,et al.  Test of E2 virtual-photon spectra calculated in the distorted-wave Born approximation , 1980 .

[16]  Peter Meyer,et al.  Giant resonance for the actinide nuclei: Photoneutron and photofission cross sections for U-235, U-236, U-238, and Th-232 , 1980 .

[17]  S. Herdade,et al.  Formalism and applications of electrofission and photofission fragment angular distributions , 1980 .

[18]  R. Pitthan,et al.  Giant multipole resonances in the deformed fissionable nucleusU238 , 1980 .

[19]  R. Haag,et al.  Electrofission of238U and232Th , 1979 .

[20]  D. K. Scott,et al.  Observation of isoscalar giant-resonance structure in the fission of /sup 238/U following inelastic scattering of /sup 6/Li , 1979 .

[21]  A. Woude,et al.  Inhibition of the Fission Decay Channel of the Isoscalar Giant Quadrupole Resonance in the Actinide Region , 1979 .

[22]  S. Herdade,et al.  Electric quadrupole giant resonance in the photofission of /sup 238/U , 1978 .

[23]  L. E. Wright,et al.  A new technique for calculating virtual photon spectra , 1977 .

[24]  B. C. Cook.  Least structure solution of photonuclear yield functions , 1963 .