Inference on fission timescale from neutron multiplicity measurement in18O+184W

Author(s):  
Niraj Kumar Rai ◽  
Aman Gandhi ◽  
M T Senthil Kannan ◽  
Sujan Kumar Roy ◽  
Saneesh Nedumbally ◽  
...  

Abstract The pre-scission and post-scission neutron multiplicities are measured for the 18O + 184W reaction in the excitation energy range of 67.23−76.37 MeV. Langevin dynamical calculations are performed to infer the energy dependence of fission decay time in compliance with the measured neutron multiplicities. Different models for nuclear dissipation are employed for this purpose. Fission process is usually expected to be faster at a higher beam energy. However, we found an enhancement in the average fission time as the incident beam energy increases. It happens because a higher excitation energy helps more neutrons to evaporate that eventually stabilizes the system against fission. The competition between fission and neutron evaporation delicately depends on the available excitation energy and it is explained here with the help of the partial fission yields contributed by the different isotopes of the primary compound nucleus.

1997 ◽  
Vol 3 (S2) ◽  
pp. 881-882 ◽  
Author(s):  
Dale E. Newbury

Throughout the history of electron-beam X-ray microanalysis, analysts have made good use of the strong dependence of electron range on incident energy (R ≈ E1,7) to optimize the analytical volume when attacking certain types of problems, such as inclusions in a matrix or layered specimens. The “conventional” energy range for quantitative electron beam X-ray microanalysis can be thought of as beginning at 10 keV and extending to the upper limit of the accelerating potential, typically 30 - 50 keV depending on the instrument. The lower limit of 10 keV is selected because this is the lowest incident beam energy for which there is a satisfactory analytical X-ray peak excited from the K-, L-, or M- shells (in a few cases, two shells are simultaneously excited, e.g., Fe-K and Fe-L) for every element in the Periodic Table that is accessible to X-ray spectrometry, beginning with Be (Ek =116 eV) and extending to the transuranic elements. This criterion is based upon establishing a minimum overvoltage U = E0/Ec > 1.25, which is the practical minimum for useful excitation.


1975 ◽  
Vol 53 (2) ◽  
pp. 117-122 ◽  
Author(s):  
J. P. Labrie ◽  
E. E. Habib ◽  
Z. Preibisz

Excited levels of 70Ge and proton holes in 69Ga have been investigated by means of the 69Ga (3He, d)70Ge reaction at an incident beam energy of 22.5 MeV. Angular distributions were measured and are compared with the prediction of the distorted-wave-Born-approximation (DWBA) theory in order to obtain the spectroscopic strengths of each level.The number of proton holes in 69Ga was obtained from the sum rule of the spectroscopic strengths. The vacancy probability UJ2 and the center of gravity energy EJ for the 2p3/2, 1f5/2, and 2p1/2 subshells are[Formula: see text]These are compared with the pairing model calculations.


2005 ◽  
Vol 20 (02n03) ◽  
pp. 690-692 ◽  
Author(s):  
◽  
MARTIN KOTULLA

We have measured the reaction γp→η′p from threshold up to 2.6 GeV incident beam energy using the Crystal Barrel and TAPS detectors at the ELSA accelerator. At present the knowledge about the resonance contribution to this process is very limited. Our measurement is a significant improvement of the data basis. We will present preliminary results.


1990 ◽  
Vol 202 ◽  
Author(s):  
J. J. Cuomo ◽  
J. Bruley ◽  
J. P. Doyle ◽  
D. L. Pappas ◽  
K. L. Saenger ◽  
...  

ABSTRACTWe report on a study of hard amorphous carbon thin films prepared by condensing streams of energetic carbon species, onto a range of substrates maintained at different temperatures. The carbon vapor is generated either by ion sputtering, laser ablation or e-beam evaporation. Spatially resolved electron-energy-loss spectra reveal variations in the films′ microstructure brought about by altering the deposition conditions. We estimate that the density of the different films varies between 2.0 and 3.26 g/cm3. We observe an evolution towards denser films upon increasing incident beam energy, reducing substrate temperature, and increasing substrate thermal conductivity. Low density films contain a predominance of trigonally bonded sp2-hybridized carbon (i.e graphitic carbon) and the highest density films contain a high fraction (∽ 80%) of tetr-ahedral sp3-bonded carbon (i.e. diamond-like).


1995 ◽  
Vol 78 (4) ◽  
pp. 2311-2322 ◽  
Author(s):  
Stephan Kirchner ◽  
Jin Wang ◽  
Zhijian Yin ◽  
Martin Caffrey

2006 ◽  
Vol 632 (4) ◽  
pp. 480-484 ◽  
Author(s):  
M. Mahjour-Shafiei ◽  
H.R. Amir-Ahmadi ◽  
J.C.S. Bacelar ◽  
R. Castelijns ◽  
K. Ermisch ◽  
...  

1994 ◽  
Vol 01 (04) ◽  
pp. 581-583
Author(s):  
T.L. BUSH ◽  
T.S. JONES ◽  
D.O. HAYWARD

The interaction of O 2 and N 2 molecular beams with a Na-covered Si(100)-(2×1) surface has been studied as a function of incident beam energy and sodium coverage. Exposure to O 2 at 300 K results in the immediate dissociation of the molecules on impact with the surface leading to the direct formation of silicon oxide. In contrast, significant nitridation requires a further step involving desorption of the sodium. The rate of formation of the oxide or nitride increases uniformly with sodium coverage. In addition, the reaction probability for both processes is significantly enhanced by increasing the translational energy of the incident O 2 or N 2 molecules. These observations indicate that both reactions proceed via a direct collisional activation process in which local electrostatic forces in the vicinity of the Na atoms are responsible for the promotional effect.


2014 ◽  
Vol 53 (7S) ◽  
pp. 07KC10 ◽  
Author(s):  
Tomoyuki Sawada ◽  
Tomohisa Norisuye ◽  
Mariko Kohyama ◽  
Kazuki Sugita ◽  
Hideyuki Nakanishi ◽  
...  

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