AbstractWe analyze generic sequences for which the geometrically linear energy $$\begin{aligned} E_\eta (u,\chi )\,{:}{=} \,\eta ^{-\frac{2}{3}}\int _{B_{1}\left( 0\right) } \left| e(u)- \sum _{i=1}^3 \chi _ie_i\right| ^2 \, \mathrm {d}x+\eta ^\frac{1}{3} \sum _{i=1}^3 |D\chi _i|({B_{1}\left( 0\right) }) \end{aligned}$$
E
η
(
u
,
χ
)
:
=
η
-
2
3
∫
B
1
0
e
(
u
)
-
∑
i
=
1
3
χ
i
e
i
2
d
x
+
η
1
3
∑
i
=
1
3
|
D
χ
i
|
(
B
1
0
)
remains bounded in the limit $$\eta \rightarrow 0$$
η
→
0
. Here $$ e(u) \,{:}{=}\,1/2(Du + Du^T)$$
e
(
u
)
:
=
1
/
2
(
D
u
+
D
u
T
)
is the (linearized) strain of the displacement u, the strains $$e_i$$
e
i
correspond to the martensite strains of a shape memory alloy undergoing cubic-to-tetragonal transformations and the partition into phases is given by $$\chi _i:{B_{1}\left( 0\right) } \rightarrow \{0,1\}$$
χ
i
:
B
1
0
→
{
0
,
1
}
. In this regime it is known that in addition to simple laminates, branched structures are also possible, which if austenite was present would enable the alloy to form habit planes. In an ansatz-free manner we prove that the alignment of macroscopic interfaces between martensite twins is as predicted by well-known rank-one conditions. Our proof proceeds via the non-convex, non-discrete-valued differential inclusion $$\begin{aligned} e(u) \in \bigcup _{1\le i\ne j\le 3} {\text {conv}} \{e_i,e_j\}, \end{aligned}$$
e
(
u
)
∈
⋃
1
≤
i
≠
j
≤
3
conv
{
e
i
,
e
j
}
,
satisfied by the weak limits of bounded energy sequences and of which we classify all solutions. In particular, there exist no convex integration solutions of the inclusion with complicated geometric structures.
Scaling Limits for the Gibbs States on Distance-Regular Graphs with Classical Parameters
