S. Fan, A. Wagner, E. Grosse In order to examine the feasibility of studying neutron rich nuclei close to the astrophysical r-process path at ELBE we investigated the production cross sections of fission fragments from photo-induced fission. The isotopic fragment distribution from bremsstrahlung-induced fission of 238U using bremsstrahlung from incident electron energies Ee can be written as
where the bremsstrahlung spectrum N(E(Ee)) was calculated using EGS4 [1], the photofission cross section sF was taken from Ref. [2]. Zp denotes the most probable charge in a Gaussian distribution and was calculated using the Zp model [3]. The width parameter sZ of the charge distribution from photofission of 238U was found to be 0.34 [4], and Ni denotes the normalization parameter. The correction factor Fp(E(Ee)) for the proton odd-even effect is defined [4] as
where dmonop(E) was deduced from experimental data[4]. Fig. 1 shows the postneutron mass distribution for the 238U(g,f) reaction with bremsstrahlung from 12 MeV electrons [5]. Fig.2 depicts the elemental mass distribution and Fig.3 shows the isotopic distribution of postneutron fission fragments (colored), nuclei with known half-lifes are shown as open boxes, stable nuclei are shown as filled boxes. Also drawn is the limit of nuclei with mean lifetimes against b-decay of more than 43 ms from theoretical predictions by Moeller [6].
References
[1] W.R. Nelson et al., SLAC-Report-265 (1985).
[2] B.L. Berman et al., Phys. Rev. C 21 (1980) 1215.
[3] R.K. Gupta et al., Phys. Rev. C 30 (1984) 395.
[4] K. Persyn et al., Nucl. Phys. A 620 (1997) 171.
[5] E. Jacobs et al., Phys. Rev. C 21 (1980) 237.
[6] P. Moeller et al., Atomic Data Nucl. Data Tables 66 (1997) 131-343.
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