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Existence of minimizers for the SDRI model in 2d: Wetting and dewetting regime with mismatch strain

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Published/Copyright: August 25, 2023

Abstract

The model introduced in [45] in the framework of the theory on stress-driven rearrangement instabilities (SDRI) [3, 43] for the morphology of crystalline materials under stress is considered. As in [45] and in agreement with the models in [50, 55], a mismatch strain, rather than a Dirichlet condition as in [19], is included into the analysis to represent the lattice mismatch between the crystal and possible adjacent (supporting) materials. The existence of solutions is established in dimension two in the absence of graph-like assumptions and of the restriction to a finite number m of connected components for the free boundary of the region occupied by the crystalline material, thus extending previous results for epitaxially strained thin films and material cavities [6, 35, 34, 45]. Due to the lack of compactness and lower semicontinuity for the sequences of m-minimizers, i.e., minimizers among configurations with at most m connected boundary components, a minimizing candidate is directly constructed, and then shown to be a minimizer by means of uniform density estimates and the convergence of m-minimizers’ energies to the energy infimum as m . Finally, regularity properties for the morphology satisfied by every minimizer are established.

MSC 2020: 49J45; 35R35; 74G65

Communicated by Verena Bögelein


Funding source: Austrian Science Fund

Award Identifier / Grant number: M 2571

Award Identifier / Grant number: P 33716

Award Identifier / Grant number: P 29681

Award Identifier / Grant number: TAI 293

Award Identifier / Grant number: MA16-005

Award Identifier / Grant number: HR 08/2020

Award Identifier / Grant number: CUP: E55F22000270001

Funding statement: Sh. Kholmatov acknowledges support from the Austrian Science Fund (FWF) projects M 2571 and P 33716. P. Piovano acknowledges the support from the Austrian Science Fund (FWF) projects P 29681 and TAI 293, from the Vienna Science and Technology Fund (WWTF) together with the City of Vienna and Berndorf Privatstiftung through Project MA16-005, and from BMBWF through the OeAD-WTZ project HR 08/2020. Furthermore, P. Piovano acknowledges the support obtained by the Italian Ministry of University and Research (MUR) through the PRIN Project “Partial differential equations and related geometric-functional inequalities”, is member of the Italian “Gruppo Nazionale per l’Analisi Matematica, la Probabilità e le loro Applicazioni” (GNAMPA-INdAM) and has received funding from the GNAMPA 2022 project CUP: E55F22000270001. Finally, P. Piovano is grateful for the support received from the Okinawa Institute of Science and Technology (OIST), Japan, as Visiting Professor and Excellence Chair and through the Theoretical Science Visiting Program (TSVP).

A Appendix

We include in this section auxiliary results used in the paper for the convenience of the reader. We begin with a property satisfied by the free-crystal regions in 𝒜 and 𝒜 ~ .

Proposition A.1.

Let A R 2 be a bounded L 2 -measurable set with H 1 ( A ) < + . Then A is a set of finite perimeter in R 2 .

Proof.

Since A Δ Int ( A ¯ ) A ¯ Int ( A ) = A , we have | A Δ Int ( A ¯ ) | | A | = 0 . Hence, it suffices to prove that the open set E := Int ( A ¯ ) has finite perimeter in 2 . Note that, by construction,

E A and 1 ( E ) 1 ( A ) < + .

We divide the proof of E BV ( 2 , { 0 , 1 } ) into three steps.

Step 1. We claim that if E is simply connected, then E BV ( 2 ; { 0 , 1 } ) . Indeed, in this case E is a connected compact set with 1 ( E ) 1 ( A ) < + and, by [33, Lemma 3.12], it contains a closed curve Γ enclosing E ¯ . Since 1 ( Γ ) < + , it is rectifiable in the sense of [33, Section 3.2]: its length 1 ( Γ ) is well-approximated by the length of closed polygonal curves π k whose vertices lie on Γ, i.e., 1 ( π k ) 1 ( Γ ) . Let E k be the set enclosed by π k and observe that

π k 𝐾 Γ .

Since E k are Lipschitz sets, they are sets of finite perimeter and

P ( E k ) = 1 ( π k ) 1 ( Γ ) + 1

for large k. Since E is open, for every x E there exists a ball B r ( x ) E and by the Kuratowski convergence of π k to Γ. It follows that B r ( x ) E k for large k, and hence χ E k ( x ) = χ E ( x ) = 1 . Similarly, χ E k ( x ) = χ E ( x ) = 0 for every x 2 E ¯ provided k is large enough. Therefore, χ E k χ E a.e. in 2 , and hence E k E in L 1 ( 2 ) . Now, by the L 1 -lower semicontinuity of perimeter (see [52, Proposition 12.15]), E is a set of finite perimeter.

Step 2. We claim that if E is connected, then E BV ( 2 ; { 0 , 1 } ) . Indeed, let E be the smallest simply connected open set containing E (basically, E is constructed by filling all “holes” in E), and let

F := E E ¯

be the union of all holes. Since

E E and 1 ( E ) 1 ( A ) < + ,

by step 1, we have E BV ( 2 ; { 0 , 1 } ) . Observing E = E F ¯ , to conclude this step it is enough to prove that F has finite perimeter. Since every open set in 2 is a union of at most countably many connected components[2], we have F = j F j , where the { F j } are open, connected and F i F j = for i j . Since E is connected, each F j is simply connected. Hence, by step 1, F j BV ( 2 ; { 0 , 1 } ) . Moreover, the set F i F j , i j , can have at most one point. Indeed, otherwise, by the definition of F and the connectedness of E, we could find a curve γ F i F j E with 1 ( γ ) > 0 , which contradicts the equality E = Int ( E ¯ ) . Therefore, observing F = F j E , we obtain

j P ( F j ) j 1 ( F j ) = 1 ( j F j ) = 1 ( F ) 1 ( E ) < + .

Thus, F = j F j has finite perimeter in 2 .

Step 3. Now, we prove that E BV ( 2 ; { 0 , 1 } ) (without assuming any extra connectedness assumption). Let { E j } be the family of connected components of E. Since

1 ( E j ) 1 ( E ) < + ,

by step 2, we have E j BV ( 2 ; { 0 , 1 } ) . Therefore, since E = j E j , we obtain that

j P ( E j ) j 1 ( E j ) 1 ( j E j ) + i < j 1 ( E i E j ) 2 1 ( j E j ) = 2 1 ( E ) .

Hence, by the finiteness of 1 ( E ) , the set E = j E j has finite perimeter in 2 . ∎

The following proposition, which is based on [52, Proposition 2.16], is used throughout the paper.

Proposition A.2.

Let K R 2 be such that H 1 ( K ) < + and let { E t } t Υ be a family of sets parametrized by t Υ such that

(A.1) 1 ( K E t E s ) = 0

and H 1 ( K E t ) > 0 . Then Υ is at most countable.

Proof.

The proof runs along the lines of the proof of [52, Proposition 2.16]. For j , let Υ j Υ be the set of all t Υ such that 1 ( K E t ) > 1 j . Then, by (A.1), Υ j cannot contain more than j 1 ( K ) elements. Since Υ = j Υ j , the set Υ is at most countable. ∎

We finally state a regularity property of GSBD functions with d - 1 -negligible jump.

Proposition A.3.

Let U R d be a connected bounded open set and let u GSBD 2 ( U ) be such that H d - 1 ( J u ) = 0 . Then u H loc 1 ( U ) .

Proof.

Indeed, for r > 0 let Q := x 0 + ( - r , r ) d U be any cube centered at x U and let 0 < θ ′′ < θ < 1 . For shortness, write

Q := x 0 + ( - θ r , θ r ) d and Q ′′ := x 0 + ( - θ ′′ r , θ ′′ r ) d .

By [11, Proposition 3.1 (1)] (see also [10, Theorem 1.1]), there exists an 2 -measurable set ω Q and a rigid displacement a : d d such that | ω | c * r d - 1 ( J u ) = 0 and

Q | u - a | 2 d d - 1 𝑑 x = Q ω | u - a | 2 d d - 1 𝑑 x c * r 2 ( Q | e ( u ) | 2 ) d d - 1 ,

where c * depends only on d. Hence, u L loc 2 d / ( d - 1 ) ( Q ) . Next, fix any mollifier ρ 1 C ( B r ( 0 ) ) with

ρ ϵ C c ( B ( θ - θ ′′ ) ϵ ) ,

where ρ ϵ ( x ) := ρ 1 ( x / ϵ ) , ϵ ( 0 , r ) . By [11, Proposition 3.1], there exists p ¯ > 0 depending on n and ϵ such that

Q ′′ | e ( u * ρ ϵ ) - e ( u ) * ρ ϵ | 2 𝑑 x c ( d - 1 ( J u ) r d - 1 ) p ¯ Q | e ( u ) | 2 𝑑 x = 0 ,

where c depends on n, ρ 1 and ϵ. Hence,

(A.2) e ( u * ρ ϵ ) = e ( u ) * ρ ϵ a.e. in  Q ′′ .

Recall that u * ρ ϵ C ( Q ′′ ) . Since e ( u ) L 2 ( Q ) , we have

e ( u ) * ρ ϵ C ( Q ′′ ) L 2 ( Q ′′ ) ;

in particular,

e ( u * ρ ϵ ) C ( Q ′′ ) L 2 ( Q ′′ ) .

By the Poincaré–Korn inequality, u * ρ ϵ H 1 ( Q ′′ ) . Since e ( u ) * ρ ϵ e ( u ) in L 2 ( Q ′′ ) as ϵ 0 , in view of (A.2), there exists ϵ 0 > 0 such that

e ( u * ρ ϵ ) L 2 ( Q ′′ ) e ( u ) L 2 ( Q ′′ ) + 1 for all  ϵ ( 0 , ϵ 0 ) .

Moreover, by the Poincaré–Korn inequality, for any ϵ ( 0 , ϵ 0 ) there exists a rigid displacement a ϵ such that

u * ρ ϵ - a ϵ H 1 ( Q ′′ ) C e ( u * ρ ϵ ) L 2 ( Q ′′ ) C ( e ( u ) L 2 ( Q ′′ ) + 1 ) ,

where C is the Poincaré–Korn constant for a cube. Thus, the family { u * ρ ϵ } ϵ is uniformly bounded in H 1 ( Q ′′ ) . Since u * ρ ϵ u in L 2 ( Q ′′ ) , there exists a rigid displacement a such that a ϵ a in L 2 ( Q ′′ ) . Then u * ρ ϵ - a ϵ weakly converges to u - a in H 1 ( Q ′′ ) , i.e., u - a H 1 ( Q ′′ ) . Since a is linear and θ ′′ is arbitrary, u H loc 1 ( Q ) . Now, covering U with finitely many cubes of edgelength 2 r , we get u H loc 1 ( U ) . ∎

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Received: 2022-07-06
Accepted: 2023-06-19
Published Online: 2023-08-25
Published in Print: 2024-07-01

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