Metal ion injection into metals III. Irradiation system and experimental techniques

1973 ◽  
Vol 18 (1-2) ◽  
pp. 73-78 ◽  
Author(s):  
H. J. Smith
2016 ◽  
Vol 87 (2) ◽  
pp. 02A913
Author(s):  
M. J. Segal ◽  
R. A. Bark ◽  
R. Thomae ◽  
E. E. Donets ◽  
E. D. Donets ◽  
...  

2012 ◽  
Vol 83 (2) ◽  
pp. 02A511 ◽  
Author(s):  
A. Thorn ◽  
E. Ritter ◽  
F. Ullmann ◽  
W. Pilz ◽  
L. Bischoff ◽  
...  

2017 ◽  
Vol 8 (11) ◽  
pp. 7862-7872 ◽  
Author(s):  
Zhongling Lang ◽  
Peng Yang ◽  
Zhengguo Lin ◽  
Likai Yan ◽  
Ming-Xing Li ◽  
...  

The close interplay of theoretical and experimental techniques can facilitate the understanding and rational synthesis of novel inorganic clusters, and here an impressive example is shown for the class of cuboid-shaped polyoxo-12-palladates(ii) with a central metal ion guest.


2006 ◽  
Vol 77 (3) ◽  
pp. 03A909 ◽  
Author(s):  
A. Pikin ◽  
J. G. Alessi ◽  
E. N. Beebe ◽  
A. Kponou ◽  
K. Prelec

1994 ◽  
Vol 65 (10) ◽  
pp. 3091-3098 ◽  
Author(s):  
B. H. Wolf ◽  
H. Emig ◽  
D. Rück ◽  
P. Spädtke
Keyword(s):  

Author(s):  
R. Levi-Setti ◽  
J. M. Chabala ◽  
Y. L. Wang

We have shown the feasibility of 20 nm lateral resolution in both topographic and elemental imaging using probes of this size from a liquid metal ion source (LMIS) scanning ion microprobe (SIM). This performance, which approaches the intrinsic resolution limits of secondary ion mass spectrometry (SIMS), was attained by limiting the size of the beam defining aperture (5μm) to subtend a semiangle at the source of 0.16 mr. The ensuing probe current, in our chromatic-aberration limited optical system, was 1.6 pA with Ga+ or In+ sources. Although unique applications of such low current probes have been demonstrated,) the stringent alignment requirements which they imposed made their routine use impractical. For instance, the occasional tendency of the LMIS to shift its emission pattern caused severe misalignment problems.


Author(s):  
R. Levi-Setti ◽  
J.M. Chabala ◽  
Y.L. Wang

Finely focused beams extracted from liquid metal ion sources (LMIS) provide a wealth of secondary signals which can be exploited to create high resolution images by the scanning method. The images of scanning ion microscopy (SIM) encompass a variety of contrast mechanisms which we classify into two broad categories: a) Emission contrast and b) Analytical contrast.Emission contrast refers to those mechanisms inherent to the emission of secondaries by solids under ion bombardment. The contrast-carrying signals consist of ion-induced secondary electrons (ISE) and secondary ions (ISI). Both signals exhibit i) topographic emission contrast due to the existence of differential geometric emission and collection effects, ii) crystallographic emission contrast, due to primary ion channeling phenomena and differential oxidation of crystalline surfaces, iii) chemical emission or Z-contrast, related to the dependence of the secondary emission yields on the Z and surface chemical state of the target.


Author(s):  
J. A. N. Zasadzinski ◽  
R. K. Prud'homme

The rheological and mechanical properties of crosslinked polymer gels arise from the structure of the gel network. In turn, the structure of the gel network results from: thermodynamically determined interactions between the polymer chain segments, the interactions of the crosslinking metal ion with the polymer, and the deformation history of the network. Interpretations of mechanical and rheological measurements on polymer gels invariably begin with a conceptual model of,the microstructure of the gel network derived from polymer kinetic theory. In the present work, we use freeze-etch replication TEM to image the polymer network morphology of titanium crosslinked hydroxypropyl guars in an attempt to directly relate macroscopic phenomena with network structure.


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