scholarly journals Influence of even nucleon numbers and closed shells on mass and charge distribution in low energy fission

1994 ◽  
Vol 181 (1) ◽  
pp. 175-188 ◽  
Author(s):  
Z. Buyukmumcu ◽  
H. N. Erten ◽  
N. K. Aras
Keyword(s):  
Charge Distribution ◽  
Low Energy ◽  
Closed Shells

Angular, energy and charge distribution in the scattering of low-energy helium ions by an amorphous silicon surface

1998 ◽  
Vol 10 (4) ◽  
pp. 741-752 ◽  
Author(s):  
B Arezki ◽  
Y Boudouma ◽  
P Benoit-Cattin ◽  
A C Chami ◽  
C Benazeth ◽  
...  
Keyword(s):  
Amorphous Silicon ◽  
Charge Distribution ◽  
Silicon Surface ◽  
Low Energy ◽  
Helium Ions ◽  
Angular Energy

Charge distribution in low energy fission of actinides

2004 ◽  
Vol 30 (2) ◽  
pp. 107-127 ◽  
Author(s):  
H Naik ◽  
R J Singh ◽  
R H Iyer
Keyword(s):  
Charge Distribution ◽  
Low Energy

Charge distribution mapping by low energy electrons

2004 ◽  
Vol 85 (19) ◽  
pp. 4490 ◽  
Author(s):  
P. S. Dorozhkin ◽  
Z.-C. Dong
Keyword(s):  
Charge Distribution ◽  
Low Energy ◽  
Low Energy Electrons ◽  
Distribution Mapping

scholarly journals Energy loss and effective charge of low-energy oxygen ions in partially ionized plasma

2000 ◽  
Vol 18 (4) ◽  
pp. 639-646
Author(s):  
K. NISHIGORI ◽  
U. NEUNER ◽  
M. TAKIZAWA ◽  
M. KOJIMA ◽  
T. SAGAMI ◽  
...  
Keyword(s):  
Energy Loss ◽  
Charge Distribution ◽  
Effective Charge ◽  
Low Energy ◽  
Stopping Power ◽  
Oxygen Ions ◽  
Power Equation ◽  
Slow Ions ◽  
Partially Ionized ◽  
Peak Value

This article reports on the interaction between slow ions and a partially ionized plasma. Temporal evolutions of energy loss and charge distribution of 2.4 MeV oxygen beams in the laser-induced polyethylene plasma were measured. The charge distribution showed strong stripping ability in the early phase of the plasma. Stopping power deduced from the experimental energy loss was 1.9 times larger than that for the solid. The effective charge of the projectile ion was estimated from the yields of 4+ and 6+ states. The peak value of the effective charge was 1.4 times larger than that of the solid. The stopping power equation given by Sigmund was extended for the partially ionized plasma and it could reproduce the measured energy loss.

Charge Distribution in the Mass Region 128 —134 in Low Energy Fission of Actinides

1993 ◽  
Vol 62 (1-2) ◽  
pp. 1-6 ◽  
Author(s):  
H. Naik ◽  
S. P. Dange ◽  
T. Datta
Keyword(s):  
Charge Distribution ◽  
Mass Region ◽  
Low Energy

Nuclear-Charge Distribution in Low-Energy Fission

1962 ◽  
Vol 126 (3) ◽  
pp. 1112-1127 ◽  
Author(s):  
A. C. Wahl ◽  
R. L. Ferguson ◽  
D. R. Nethaway ◽  
D. E. Troutner ◽  
K. Wolfsberg
Keyword(s):  
Charge Distribution ◽  
Nuclear Charge ◽  
Low Energy ◽  
Nuclear Charge Distribution

A Unified Interpretation of Mass and Charge Distribution and Prompt Neutron Evaporation in Low-Energy Nuclear Fission

1969 ◽  
Vol 24 (12) ◽  
pp. 2000-2003 ◽  
Author(s):  
H. O . Denschlag ◽  
S. M. Qaim
Keyword(s):  
Experimental Data ◽  
Simple Model ◽  
Transition State ◽  
Charge Distribution ◽  
Nuclear Fission ◽  
Low Energy ◽  
Prompt Neutron ◽  
Neutron Evaporation ◽  
State Configuration

AbstractA simple model for a transition state configuration in low-energy fission is given. In its light the latest experimental data on mass and charge distribution and on prompt neutron evaporation are discussed.

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