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71.
Rainer W Hasse 《Pramana》1978,11(4):441-455
The polarization of the fragments from binary fission or of scattering or fusioning heavy nuclei is investigated in the liquid
drop model. Due to the mutual Coulomb repulsion near contact the fragments may be polarized with respect to their charges
(electric dipole moments from inhomogeneous charge distributions) as well as with respect to their shapes (quadrupole and
octupole deformations). The lowering of the minimum energy near contact due to charge polarization is in the order of 1 MeV
if one takes into account the energy from the giant dipole restoring force derived from the volume symmetry energy in addition
to the liquid drop energies. The question whether one obtains prolate or oblate shapes is entirely due to the restriction
in deformation space (fixed distance between centers-of mass or between the tips of the fragments). 相似文献
72.
V.L. Kuznetsov L.E. Lazareva V.G. Nedorezov N.V. Nikitina N.M. Parovic 《Nuclear Physics A》1979,324(1):29-38
The ratio of delayed to prompt fission yields has been measured for 241Am and 243Am samples irradiated by a bremsstrahlung photon pulsed beam over the energy range Eγmax = 10–80 MeV. The relative probabilities of 240mfAm and 242mfAm isomer production and the cross sections of the 241Am(γ, n)240mfAm and 243Am(γ, n)242mfAm reactions were deduced from the yields measured in the E1 giant resonance region. 相似文献
73.
A measurement of symmetric and asymmetric photofission yields of238U in the energy region from 4.5 MeV to 6.5 MeV has been performed. As γ-source the bremsstrahlung from a microtron has been used. The fission yields are obtained from β-counting of chemically separated isotopes 111Ag, 115Cd and 117Cd for symmetric fission and 139Ba for asymmetric fission. Some structures in the yield curves at about 5.3 MeV and a pronounced maximum at about 6.0 MeV in the valley-to-peak ratio in the fission fragment yield distribution are observed. It is suggested that these effects are connected with the double-hump fission barrier concept and indicate differences between fission barriers for symmetric and asymmetric fission. 相似文献
74.
Ternary and quaternary fission produced in silver and bromine nuclei have been studied withK5 nuclear emulsion exposed to 1.8 GeV/cK
− beams. The frequency of the ternary events is found to be ∼0.08 of that of the binary events produced in the same volume
of the emulsion. The range ratio and range distribution of the fission fragments are studied and the angles between each pair
of the fragments are determined. Ranges are found to vary from 5 to 40μ with a maximum number lying between 5 and 10μ. The angles between the fission fragments are found to form a broad distribution extending from 40° to 180°. A few of the
events have also been analysed to give them a possible identity. A possible case of quaternary fission has also been reported.
This paper was presented at the Symposium on 3rd High Energy Physics held at Bhubaneswar during November 1976. 相似文献
75.
Several characteristics of fission accompanied by long range alpha particles (LRA) have been studied in the thermal neutron
induced fission of235U. The kinetic energies of fission fragments and the LRA were measured with a back-to-back ionization chamber and semiconductor
detectors respectively. The kinetic energies of the two fragments and the LRA in LRA fission, along with the energies of pair
fragments in the normal binary fissions, were recorded event by event on a magnetic tape by means of a four-parameter data
acquisition system. The data were analysed to study the dependence of different quantities in LRA fission on the fragment
mass ratio, LRA energy and the total kinetic energy of the fission fragments. It is seen that the most probable energy of
LRA increases significantly for near symmetric mass divisions. The total kinetic energy for all mass ratios in LRA fission
is found to be (2.6±0.7) MeV larger than that in binary fission. The difference in the total kinetic energies in LRA and binary
fissions is seen to be dependent on mass ratio. This result may suggest that the scission configuration in LRA fission is
different for different mass ratios. Correlations between the fission fragment and LRA energies have been studied for several
mass ratios. It is seen that the most probable fragment kinetic energyĒ
k varies nearly linearly with the LRA energyE
a for various mass divisions but the variation of the most probable LRA energyĒ
a with fragment kinetic energyE
k is found to deviate from linearity for several mass ratios. From a least square fit to the variation ofĒ
k withE
a it is found that the slope (dĒ
k/dEa) increases with the increase in mass ratio. The present results are discussed to arrive at a better understanding of the
scission configuration in the fission accompanied by LRA emission. 相似文献
76.
Angular distributions of light charged particles from 252Cf fission in the ranges 0–46° and 134–180°
A.J. Kordyasz E. Piasecki L. Nowicki P. Koczoń J. Sobolewski M. Kisieliński W. Czarnackif 《Nuclear Physics A》1985,439(1):28-44
Alpha particles, tritons, deuterons and protons accompanying 252Cf fission were registered in coincidence with both fission fragments by means of a system containing two-dimensional position-sensitive silicon detectors. Angular distributions, kinetic energy spectra of light charged particles as well as mass distributions of fission fragments in coincidence with light charged particles were measured. The experimental results are compared with some theoretical models. 相似文献
77.
Hadi Eslamizadeh 《中国物理 C》2010,34(11):1714-1716
A dynamical statistical model is used to analyze the experimental shape isomer yields data in the reaction d+240Pu at E=20–29 MeV.The possibility of determining the nuclear dissipation is discussed.Comparison of the experimental data with the calculations leads to a value of the reduced dissipation coeffcient β=0.45×1021 s-1 for the Am isotopes. 相似文献
78.
The present work represents the results of angular distribution measurements performed for promt gamma-rays in the range of 1.1 … 1.2. MeV due to the 233U(n, f) and 239Pu(n,f) reactions. The measurements yielded anisotropy values found to be consistent with values previously measured and using the same technique at different gamma energy bands. Such consistency, also found to exist between anisotropy values previously measured for the 235U(n,f) reaction, is a strong evidence about the energy independence of the anisotropy and indicates that the gamma spectra (at 180° and 90° to the fission direction) are essentially the same. The average values of the fragment angular momentum were calculated according to Strutinsky and Nix-Swiatecki theories. It was found that the values of the average angular momentum calculated for 234U, 236U and 240Pu according to Strutinsky,s formula (at different gamma energy bands) are consistent and yield average values which are in good agreement with those obtained from direct measurements. 相似文献
79.
G. Dersch R. Beckmann G. Feige T. Lund P. Vater R. Brandt 《Isotopes in environmental and health studies》2013,49(6):303-304
A recent article interpreted the experiment by Dersch et al. on the formation of 24Na in 40Ar + Cu interactions in a very simple manner. The results from emulsion experiments performed with 3.6 AGeV 22Ne were adapted for the interpretation of the experiments with 1.8 AGeV 40Ar. The model used the same mean value for the energy of minimum ionizing protons and pions at all angles. It is argued that a more complex approach is needed for a satisfactory interpretation. 相似文献
80.
Iodine and tellurium isotopes produced in the fission of 232Th with 30.5 MeV alpha particles were separated using a method of sublimation in an air stream and the independent yields of 130I, 131I, 132m,gI, 133I 134I, 134m,gTe, 133mTe and 134Te (cumulative) were determined by means of high resolution Ge(Li) γ-ray spectrometry. A Gaussian fit to the experimental data was used to obtain the width parameter σz and the most probable charge Zp of the nuclear charge distribution in the isobaric chains 130 – 131. The most probable masses for fission fragments with Z = 52 and Z = 53 were also deduced from the measured fission yields. 相似文献