Full text: Proceedings, XXth congress (Part 3)

  
International Archives of the Photogrammetry, Remote Sensing and Spatial Information Sciences, Vol XXXV, Part B3. Istanbul 2004 
o- intensity deviation of the same neighbouring region 
as the above defined. 
g(x,y,z) = the intensity value of the target voxel 
x,y,z = the coordinates of the target voxel 
h = a parameter which corresponds to control the 
easiness of growing, 
The results obtained by the vessel segmentation using the above 
condition were not satisfactory ones in which many parts of 
shortages were found. The main reason of this seems to be that 
the intensity value changes widely in the vicinity of the branch 
bifurcation. 
We carried out a branch-based region growing as a trial to 
check the actual intensity transition within blood vessels. The 
voxels with more than 70 intensity level (max=255) are set as 
the target voxels. Figure 6 shows the linkages between branches 
and branch attributes (length, thickness and intensity value). 
Each rectangle corresponds to each branch unit, i.e., region 
between bifurcations. The brightness inside rectangles indicates 
the intensity value of the corresponding branch unit, and its 
length and width indicate the length and thickness of the branch 
unit respectively. 
This figure shows that the average values of the intensity and 
the thickness of the vessel widely change in the vicinity of the 
branch. The relation between the intensity and the thickness of 
each branch is shown in Figure 7. The horizontal axis indicates 
vessel thickness obtained by counting the number of voxels in 
the cross section area and the vertical axis indicates the average 
intensity of each branch unit. 
We can see a close relation between the thickness and the 
intensity on this figure. Especially, in the range of section area 
(thickness) less than 30, this relation seems almost linear. On 
the other hand, there exist several dots which don't fit to the 
relation. They seem to correspond to the leak region. By getting 
rid of these dots on branch units, we can get more proper results. 
The following equation is proposed for this purpose: 
C min + kd, (d, < d. ) (2) 
Hm (d, 2 d,) 
C nin s kd, 
MW, = average intensity of i-th extracted branch 
d; = average thickness of i-th extracted branch 
Cmin = lower limits of the intensity of ROI 
k = exclusive rate (if k=0, all branches are accepted) 
d; = upper limits of the thickness range that the linear 
relation between thickness and intensity is formed. 
where 
cos o thickness. 
  
    
right IC 
    
E intensity T 
  
    
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Figure 6. Attributes and linkages of extracted branches. 
  
  
  
  
  
  
   
  
    
  
  
  
  
  
  
    
  
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Figure 7. Relation between the thickness and the intensity of 
each branch unit. 
2.5 Connection search over a gap 
In the case of a narrow and long region like a blood vessel, a 
break of growing often occurs because of missing voxels on the 
way. This problem can be solved by extending the searching 
area for vessels. But it increases over-extraction errors and 
needs a lot of processing time. 
In fact, the break occurs at the edge of the vessel, and it is 
enough to search for vessels at that point only. In the branch- 
based region growing, the growing stops at the each edge of the 
vessel, and then starts seeking vessels over a gap. If a vessel to 
be connected is found, the extracting process starts again, 
otherwise, the process enters into the next branch extraction. 
Figure 8 shows results of segmentation. The start point of the 
region growing was set at a point inside the carotid artery. In 
the case of this data, as the intensity of a posterior 
communicating artery is partially low, the following vertebral 
artery and some subsequent vessels are not extracted by the 
conventional method shown in the left image. By using our 
method presented above, those vessels are extracted and 
moreover narrow vessels of parietal region are also detected as 
shown in the right image.
	        
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