Digital Data for Volcano Hazards from Mount Rainier, Washington, Revised 1998

2008 ◽  
Author(s):  
S.P. Schilling ◽  
S. Doelger ◽  
R.P. Hoblitt ◽  
J.S. Walder ◽  
C.L. Driedger ◽  
...  
2008 ◽  
Author(s):  
S.P. Schilling ◽  
S. Doelger ◽  
J.S. Walder ◽  
C.A. Gardner ◽  
R.M. Conrey ◽  
...  
Keyword(s):  

2008 ◽  
Author(s):  
S.P. Schilling ◽  
S. Doelger ◽  
W.E. Scott ◽  
T.C. Pierson ◽  
J.E. Costa ◽  
...  

2008 ◽  
Author(s):  
S.P. Schilling ◽  
S. Doelger ◽  
D.R. Sherrod ◽  
L.G. Mastin ◽  
W.E. Scott

Author(s):  
S.P. Schilling ◽  
S. Doelger ◽  
W.E. Scott ◽  
R.M. Iverson

1995 ◽  
Author(s):  
R.P. Hoblitt ◽  
J.S. Walder ◽  
C.L. Driedger ◽  
K.M. Scott ◽  
P.T. Pringle ◽  
...  

2008 ◽  
Author(s):  
S.P. Schilling ◽  
S. Doelger ◽  
C.R. Bacon ◽  
L.G. Mastin ◽  
K.E. Scott ◽  
...  

1998 ◽  
Author(s):  
R.P. Hoblitt ◽  
J.S. Wilder ◽  
C.L. Driedger ◽  
K.M. Scott ◽  
P.T. Pringle ◽  
...  

Author(s):  
D. R. Denley

Scanning tunneling microscopy (STM) has recently been introduced as a promising tool for analyzing surface atomic structure. We have used STM for its extremely high resolution (especially the direction normal to surfaces) and its ability for imaging in ambient atmosphere. We have examined surfaces of metals, semiconductors, and molecules deposited on these materials to achieve atomic resolution in favorable cases.When the high resolution capability is coupled with digital data acquisition, it is simple to get quantitative information on surface texture. This is illustrated for the measurement of surface roughness of evaporated gold films as a function of deposition temperature and annealing time in Figure 1. These results show a clear trend for which the roughness, as well as the experimental deviance of the roughness is found to be minimal for evaporation at 300°C. It is also possible to contrast different measures of roughness.


Author(s):  
Stuart McKernan ◽  
C. Barry Carter

Convergent-beam electron diffraction (CBED) patterns contain an immense amount of information relating to the structure of the material from which they are obtained. The analysis of these patterns has progressed to the point that under appropriate, well specified conditions, the intensity variation within the CBED discs may be understood in a quantitative sense. Rossouw et al for example, have produced numerical simulations of zone-axis CBED patterns which show remarkable agreement with experimental patterns. Spence and co-workers have obtained the structure factor parameters for lowindex reflections using the intensity variation in 2-beam CBED patterns. Both of these examples involve the use of digital data. Perhaps the most frequent use for quantitative CBED analysis is the thickness determination described by Kelly et al. This analysis has been implemented in a variety of different ways; from real-time, in-situ analysis using the microscope controls, to measurements of photographic prints with a ruler, to automated processing of digitally acquired images. The potential advantages of this latter process will be presented.


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