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A. Kenik, and K. F. Russell, in High Temperature Alloys: Processing for Properties, G. E. Fuchs and J. B. , to be published in Met. , 2004. 6. S. Ukai, M. Fujiwara, J. Nucl. Mater. 307-311 (2002) 749. 7. R. E. Stoller, P. J. Maziasz, A. F. Rowcliffe and M. P. Tanaka, J. Nucl. Mater. 155-157 (1988) 1328-1334. 8. E. A. Kenik and E. H. Lee, in Phase Stability Under Irradiation, J. R. Holland, L. K. Mansur, and D. I. , AIME, New York, 1981, pp. 493-503. 9. J. D. Hunn, E. H. Lee, T. S. Byun, and L. K.

B. , to be published in Met. , 2004. 6. S. Ukai, M. Fujiwara, J. Nucl. Mater. 307-311 (2002) 749. 7. R. E. Stoller, P. J. Maziasz, A. F. Rowcliffe and M. P. Tanaka, J. Nucl. Mater. 155-157 (1988) 1328-1334. 8. E. A. Kenik and E. H. Lee, in Phase Stability Under Irradiation, J. R. Holland, L. K. Mansur, and D. I. , AIME, New York, 1981, pp. 493-503. 9. J. D. Hunn, E. H. Lee, T. S. Byun, and L. K. Mansur, J. Nucl. Mater. 282 (2000) 131-136. 10. J. D. Hunn, M. B. Lewis, and E. H. Lee, in Proceedings of the Second International Topical Meeting on Nuclear Applications of Accelerator Technology, American Nuclear Society, La Grange Park, 1998, pp.

4) The size of atomistic simulations is very small, and cannot deal with complex dislocation structures. Methods for reducing the degrees of freedom are needed. (5) The boundary conditions used in MD simulations are either periodic, fixed, or represented by elastic Green’s functions. General methods for embedding MD simulations into the continuum are in an early stage of development. (6) DD codes are limited to small size crystals. To improve their speed and range of applicability, new methods of designing these codes on massively parallel computers are needed.

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