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  4. Thalamic nuclei clustering on High Angular Resolution Diffusion Images
 
conference paper

Thalamic nuclei clustering on High Angular Resolution Diffusion Images

Grassi, A
•
Cammoun, L  
•
Pollo, C
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2008
Proceedings of the 16th Scientific meeting of International Society for Magnetic Resonance in Medicine (ISMRM) Toronto- Canada Mai 2008
International Society for Magnetic Resonance in Medicine

Thalamic nuclei can be distinguished by their characteristic fiber orientations, which influence the diffusion. Fiber orientations are relatively aligned within a nucleus due to the fact that the cerebrocortical striations within a nucleus all target the same region of cortex. The number of thalamic nuclei reported with histological methods varies with the method employed, although most cyto/myeloarchitec stains identify 14 major nuclei. We present a new approach for thalamic nuclei segmentation on High Angular Diffusion Resolution Images (HARDI), performed with a constrained k-means clustering. As described by John D.Carew[1], it is possible to classify HARDI data based on the shape of the diffusion, thanks to the complex information coming from them. Mette R. Wiegell [2] proposed a thalamic nuclei clustering with k- means on diffusion tensor images, using a combination of a voxel distance and a diffusion tensor distance. In the same way, we use the k-mean algorithm with a weighted sum of two distances to cluster the thalamic nuclei on HARDI data.

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Type
conference paper
Author(s)
Grassi, A
Cammoun, L  
Pollo, C
Hagmann, P  
Meuli, R
Thiran, J P  
Date Issued

2008

Published in
Proceedings of the 16th Scientific meeting of International Society for Magnetic Resonance in Medicine (ISMRM) Toronto- Canada Mai 2008
Subjects

lts5

Editorial or Peer reviewed

REVIEWED

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EPFL

EPFL units
LTS5  
Event nameEvent placeEvent date
International Society for Magnetic Resonance in Medicine

Toronto

Mai 3-9, 2008

Available on Infoscience
June 9, 2008
Use this identifier to reference this record
https://infoscience.epfl.ch/handle/20.500.14299/26187
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