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Harwell, 1978). , Mass, charge, and energy distributions in very asymmetric thermal fission of 235U; Nucl. Phys. A 502 (1989) 233c–242c. , Mass, charge and energy distributions in the very asymmetric fission of 249 Cf induced by thermal neutrons, Nucl. Phys. A 571 (1994) 427–446. , Isomerenverhältnisse bei der Spaltung von 249Cf mit thermischen Neutronen in Abhängigkeit von der kinetischen Energie der Spaltfragmente, Dissertation, Univ. Mainz (1996). , Simultaneous investigation of fission fragments and neutrons in 252Cf(sf); Nuclear Phys.
The separation takes place according to the ratio (A/q) of mass to ionic charge state. The charge states of the ions range from about 15 to 30 and result from the dynamic equilibrium that arises when fission fragments with their full kinetic energy (of 50 to 120 MeV) are moving through the target material. The resolution of the separator is sufficiently good to allow in general the isolation of single masses in spite of the multiplicity of the q values. 24 The electric sector field of Lohengrin separates the fission fragments according to the ratio of kinetic energy to ionic charge state (E/q).
Nucl. Part. Sci. 32 (1982) 117–147. , "Ultrafast chemical separations", Nuclear Science Series: Radiochemical Techniques, Rep. NAS-NS-3118, National Academy Press, Washington, DC (1993). , Independent fission yield measurements, Nucl. Sci. Engineering 94 (1986) 337. , Advances of Inorganic Chemistry and Radiochemistry, Vol. 2, Academic Press, New York (1960) 315–362. , Mass spectrometry, Nuclear Science, Mass Spectrometry Reviews, 7 (1988) 71–111. , "Status of fission product yield data", Fission Product Nuclear Data (FPND) — 1977 (Proc.