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Variable-coefficient parabolic residual and boundary stability

Statement

Let U⊂Rd be nonempty, bounded, and open, T>0, and P[w]=−wt+∑i,j=1daij(x,t)DiDjw+∑j=1db~j(x,t)Djw+c~(x,t)w on Q=U×(0,T). Suppose a(x,t) is symmetric, ξTa(x,t)ξ≥λ0∣ξ∣2 with λ0>0, b~,c~ are bounded and continuous, and c~≤0. There is CP<∞, depending only on U,T,λ0 and the coefficient bounds, such that every w∈C2,1(Q)∩C0(Uˉ×[0,T]) with P[w]∈C0(Q) satisfies ∥w∥C0(Q)≤CP(∥P[w]∥C0(Q)+∥w∥C0(ΓT)), where ΓT=(Uˉ×{0})∪(∂U×[0,T]) excludes the final-time face.

Facts & Assumptions

Given: The bounded cylinder, uniformly elliptic coefficient matrix, bounded drift and zero-order coefficients with c~≤0, and the regularity and data of w in the Statement.

[F1]

The parabolic operator has the sign convention P=−∂t+Lt and its prescribed boundary is initial plus lateral data (Shin's parabolic operator, data, and initial-lateral boundary).

[F2]

On the final-time face the time derivative is the left derivative; at a final-time maximum it is nonnegative (Parabolic cylinder and parabolic boundary).

Proof

Proof strategy: use a spatial exponential barrier and the weak parabolic maximum principle.

1.1givenF1algebrachoose

Choose a1<b1 with a1≤x1≤b1 on Uˉ. Let B=∥b~1∥∞, C0=∥c~∥∞, and choose κ>0 so that κ2λ0−κB−C0≥1. For ψ(x,t)=eκx1, [F1] gives P[ψ]=eκx1(κ2a11+κb~1+c~)≥η:=eκa1>0. Choose M>eκb1 and put Φ=M−ψ. Then Φ>0 and P[Φ]=Mc~−P[ψ]≤−η.

2.1givenstep 1.1algebra

Let R=∥P[w]∥∞, Q0=∥w∥C0(ΓT), and z=w−Q0−(R/η)Φ. On ΓT, z≤0, and in Q, P[z]=P[w]−Q0c~−(R/η)P[Φ]≥−R+R=0.

3.1step 1.1step 2.1F2contradiction

Fix any 0<τ<T and work on Uˉ×[0,τ], where the time derivatives at spatial interior points at t=τ exist because τ<T. Suppose z>0 somewhere on this stopped cylinder. Since z≤0 on ΓT, a positive maximum occurs at a spatial interior point and at a time in (0,τ]. For sufficiently small δ>0, z+δψ still has a positive maximum away from ΓT. At this maximum, the spatial gradient is zero and the spatial Hessian is negative semidefinite; the time derivative is zero for t<τ and nonnegative from the left if t=τ. Thus [F2] and c~≤0 imply P[z+δψ]≤0, while step 2.1 and step 1.1 give P[z+δψ]>0. This contradiction shows z≤0 on every stopped cylinder; let τ↑T and use continuity at the final face. Hence w≤Q0+(R/η)∥Φ∥∞.

4.1step 3.1algebra∎

Apply the same argument to −w, for which P[−w]=−P[w] and the boundary norm is still Q0. Combining the upper and lower bounds gives the asserted estimate with CP=max⁡{1,∥Φ∥∞/η}.

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