By Yasumasa Nishiura, Motoko Kotani

This quantity includes 8 papers brought on the RIMS overseas convention "Mathematical demanding situations in a brand new section of fabrics Science", Kyoto, August 4–8, 2014. The contributions deal with matters in disorder dynamics, negatively curved carbon crystal, topological research of di-block copolymers, endurance modules, and fracture dynamics. those papers spotlight the robust interplay among arithmetic and fabrics technology and likewise replicate the task of WPI-AIMR at Tohoku collage, within which collaborations among mathematicians and experimentalists are actively ongoing.

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**Additional resources for Mathematical Challenges in a New Phase of Materials Science: Kyoto, Japan, August 2014**

**Example text**

T/ D 0. , to components which do not touch the boundary of the domain. This clearly opens up the possibility of distinguishing between interior 34 T. 5 2 10-3 Fig. 3 Averaged evolution curves for the number of boundary components of the patterns which were used to generate Fig. 2. The left and right images are for the positive and negative nodal domains, respectively. , only the interior or bulk behavior allows one to distinguish the noise amplitude in the model (3) and boundary components of the microstructure, and allows one to separate bulk behavior from boundary behavior.

6 Inherent scalings of the delineating curves from Fig. 5. By incorporating the wave number k into the scaling formula for these curves, one can see that they approach a single universal scaling law as k becomes large, see also (10). More precisely, if the curves from Fig. 5 are plotted in a =k2 - =k2 -coordinate system, where k is the wave number from the legend in Fig. 5, one obtains the colored curves in the above image. In addition, the black line denotes the scaled version of the parameter combinations at which the k-branch equilibrium becomes globally stable, as given by (11).

For example, in the right-most upper image of Fig. t/ D 401 pieces. t/ D 71. t/ D 41. The independence of the Betti numbers from the specific shape can be either a strength or a weakness of this approach, but in cases without a priori knowledge of the specific geometry of the patterns it frequently is the former. The Betti numbers for p 1 measure holes in dimension p. t/, though the correspondence is slightly more complicated. In two-dimensional domains, such as the ones depicted in Fig. 1, tunnels are reduced to loops which cannot be contracted to a point within the set.