scholarly journals Investigation of Ion Irradiation Effects in Silicon and Graphite Produced by 23 MeV I Beam

Materials ◽  
2021 ◽  
Vol 14 (8) ◽  
pp. 1904
Author(s):  
Kristina Tomić Luketić ◽  
Marko Karlušić ◽  
Andreja Gajović ◽  
Stjepko Fazinić ◽  
Jacques H. O’Connell ◽  
...  

Both silicon and graphite are radiation hard materials with respect to swift heavy ions like fission fragments and cosmic rays. Recrystallisation is considered to be the main mechanism of prompt damage anneal in these two materials, resulting in negligible amounts of damage produced, even when exposed to high ion fluences. In this work we present evidence that these two materials could be susceptible to swift heavy ion irradiation effects even at low energies. In the case of silicon, ion channeling and electron microscopy measurements reveal significant recovery of pre-existing defects when exposed to a swift heavy ion beam. In the case of graphite, by using ion channeling, Raman spectroscopy and atomic force microscopy, we found that the surface of the material is more prone to irradiation damage than the bulk.

1998 ◽  
Vol 4 (S2) ◽  
pp. 558-559
Author(s):  
K. E. Sickafus

In ion irradiation damage studies on ceramics, damage evolution is often assessed using Rutherford backscattering spectroscopy and ion channeling (RBS/C) techniques. In a typical experiment, a single crystal ceramic sample is irradiated with heavy ions and then the crystal is exposed to He ions along a low-index crystallographic orientation. Simultaneously, the backscattered He ion yield is measured as a function of ion energy loss. For He ions scattered from the heavy ion irradiated volume, the He ion yield increases in proportion to the heavy ion dose. The RBS/C yield rises because the He ion beam is dechanneled by, for instance, interstitial point defects and clusters and their associated strain fields. A quantitative measure of dechanneling is denoted by χmin, defined as the ratio of the He ion yield along a low-index crystal orientation, to the yield obtained in a random (non-channeling) orientation. The damage parameter xmin varies from 0 to 1, where 1 represents the maximum damage level that can be measured by RBS/C.


2012 ◽  
Vol 167 (7) ◽  
pp. 506-511 ◽  
Author(s):  
G. Devaraju ◽  
S. V.S. Nageswara Rao ◽  
N. Srinivasa Rao ◽  
V. Saikiran ◽  
T. K. Chan ◽  
...  

2015 ◽  
Vol 30 (9) ◽  
pp. 1473-1484 ◽  
Author(s):  
Clarissa A. Yablinsky ◽  
Ram Devanathan ◽  
Janne Pakarinen ◽  
Jian Gan ◽  
Daniel Severin ◽  
...  

Abstract


1997 ◽  
Vol T73 ◽  
pp. 337-339
Author(s):  
T Mitamura ◽  
M Terasawa ◽  
X Fan ◽  
T Kohara ◽  
K Ueda ◽  
...  

2002 ◽  
Vol 91 (3) ◽  
pp. 1129-1134 ◽  
Author(s):  
Saskia Kraft ◽  
Beate Schattat ◽  
Wolfgang Bolse ◽  
Siegfried Klaumünzer ◽  
Felix Harbsmeier ◽  
...  

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