TheoremBase

Bounds the cube through the Sobolev embedding, proves monotonicity from a pointwise factorisation, and obtains monotonicity relative to the form operator by testing against truncations of the cube map and letting the truncation parameter vanish.

Proof

Each result cited below is universally quantified over the data appearing in its own statement, and is applied here to the data named in the step in question.

Preliminary remarks.

(R1) For y∈Ry\in\mathbb{R} with 0≤y0\le y one has ∣y∣=y|y|=y: by claim 1 of Properties of the Absolute Value in an Ordered Field either ∣y∣=y|y|=y or ∣y∣=−y|y|=-y, and in the second case 0≤∣y∣=−y0\le|y|=-y gives y≤0y\le0 by claim 4 of Elementary Order Arithmetic in an Ordered Field, whence y=0y=0 by antisymmetry of the order and ∣y∣=−0=0=y|y|=-0=0=y by claim 4 of Additive Cancellation and Elementary Additive Identities in a Field.

(R2) For y∈Ry\in\mathbb{R} one has 0≤y20\le y^{2}: by claim 1 of Properties of the Absolute Value in an Ordered Field either ∣y∣=y|y|=y or ∣y∣=−y|y|=-y, so in both cases ∣y∣ ∣y∣=y y=y2|y|\,|y|=y\,y=y^{2}; and 0≤∣y∣0\le|y| by that claim, so claim 5 of Elementary Arithmetic in an Ordered Field with the nonnegative multiplier ∣y∣|y| gives 0=0 ∣y∣≤∣y∣ ∣y∣0=0\,|y|\le|y|\,|y|, the first equality by claim 1 of Zero Products and Elementary Identities in a Field.

(R3) For a,b∈Ra,b\in\mathbb{R} with 0≤a0\le a and a≤ba\le b one has a3≤b3a^{3}\le b^{3}, by claim 5 of Properties of Natural Number Powers in a Field.

Claim 1. Let U∈H1(Tn)U\in H^{1}(\mathbb{T}^{n}) and let uu be a representative of UU. By The Sobolev Embedding of the First Sobolev Space of the Torus into the Sixth Lebesgue Space in Dimensions at Most Three (ii), which applies because n≤3n\le3, we have u∈L6(Tn)u\in\mathcal{L}^{6}(\mathbb{T}^{n}) and ∥u∥6≤5 ∥U∥H1\lVert u\rVert_{6}\le5\,\lVert U\rVert_{H^{1}}. Applying Elementary Properties of the p-Seminorm (vi) with r=3r=3, s=2s=2 and h=uh=u, so that 0<r0<r, 1≤s1\le s and 1≤rs=61\le rs=6, we conclude that ∣u∣3|u|^{3} is measurable, belongs to L2(Tn)\mathcal{L}^{2}(\mathbb{T}^{n}), and satisfies

∥ ∣u∣3 ∥2=(∥u∥6)3.\bigl\lVert\,|u|^{3}\,\bigr\rVert_{2}=\bigl(\lVert u\rVert_{6}\bigr)^{3}.

The pointwise cube u3u^{3} is measurable by claim 3 of Arithmetic of Measurable Real- and [0,∞]-Valued Maps, applied twice, and ∣u3(x)∣=∣u(x)∣3|u^{3}(x)|=|u(x)|^{3} for every x∈Qx\in Q by claim 4 of Properties of the Absolute Value in an Ordered Field, applied twice. Hence Elementary Properties of the p-Seminorm (iii) gives u3∈L2(Tn)u^{3}\in\mathcal{L}^{2}(\mathbb{T}^{n}) with ∥u3∥2≤∥∣u∣3∥2\lVert u^{3}\rVert_{2}\le\bigl\lVert|u|^{3}\bigr\rVert_{2}. Since seminorms are nonnegative by Power-Integrable Functions and the p-Seminorm (iii), (R3) applied to 0≤∥u∥6≤5∥U∥H10\le\lVert u\rVert_{6}\le5\lVert U\rVert_{H^{1}} gives (∥u∥6)3≤(5∥U∥H1)3(\lVert u\rVert_{6})^{3}\le(5\lVert U\rVert_{H^{1}})^{3}, and claim 3 of Properties of Natural Number Powers in a Field together with 53=1255^{3}=125 gives (5∥U∥H1)3=125 (∥U∥H1)3(5\lVert U\rVert_{H^{1}})^{3}=125\,(\lVert U\rVert_{H^{1}})^{3}. Combining,

∥u3∥2≤125 (∥U∥H1)3.\lVert u^{3}\rVert_{2}\le125\,\bigl(\lVert U\rVert_{H^{1}}\bigr)^{3}.

If u~\tilde{u} is a further representative of UU then uu and u~\tilde{u} agree almost everywhere, hence so do u3u^{3} and u~3\tilde{u}^{3}, and [u3]=[u~3][u^{3}]=[\tilde{u}^{3}] by The Lebesgue Space Lᵖ(μ) (i). Since L2(Tn)L^{2}(\mathbb{T}^{n}) is a real vector space by The Riesz–Fischer Theorem (i), the scalar multiple b [u3]b\,[u^{3}] lies in L2(Tn)L^{2}(\mathbb{T}^{n}), so BB is a well-defined map from H1(Tn)H^{1}(\mathbb{T}^{n}) to L2(Tn)L^{2}(\mathbb{T}^{n}).

Claim 2. We first record a pointwise inequality. For s,t∈Rs,t\in\mathbb{R}, expanding the products in the field R\mathbb{R},

(s−t) (s2+st+t2)=s3−t3,4 (s2+st+t2)=(2s+t)2+3 t2,(s-t)\,(s^{2}+st+t^{2})=s^{3}-t^{3},\qquad 4\,(s^{2}+st+t^{2})=(2s+t)^{2}+3\,t^{2},

where 2=1+12=1+1, 3=2+13=2+1 and 4=3+14=3+1. By (R2) both (2s+t)2(2s+t)^{2} and t2t^{2} are nonnegative, hence so is 3t23t^{2} and hence so is their sum, by claim 5 of Elementary Arithmetic in an Ordered Field and clause 2 of Ordered Field. Since 44 is positive, its inverse 4−14^{-1} is positive by claim 7 of Elementary Order Arithmetic in an Ordered Field, so multiplying by 4−14^{-1} gives 0≤s2+st+t20\le s^{2}+st+t^{2}. Consequently, by (R2) and clause 2 of Ordered Field,

0≤(s−t)2 (s2+st+t2)=(s−t) (s−t) (s2+st+t2)=(s3−t3) (s−t).0\le(s-t)^{2}\,(s^{2}+st+t^{2})=(s-t)\,(s-t)\,(s^{2}+st+t^{2})=(s^{3}-t^{3})\,(s-t).

Now let U,W∈H1(Tn)U,W\in H^{1}(\mathbb{T}^{n}) with representatives uu and ww. By the vector space operations of The Lebesgue Space Lᵖ(μ) (ii), u−wu-w is a representative of U−WU-W and b (u3−w3)b\,(u^{3}-w^{3}) is a representative of B(U)−B(W)B(U)-B(W). By claim 1 of L²(μ) Is a Real Hilbert Space (i) the pointwise product of two members of L2(Tn)\mathcal{L}^{2}(\mathbb{T}^{n}) is integrable and

⟨B(U)−B(W),U−W⟩L2=∫Tnb (u3−w3) (u−w) dx.\bigl\langle B(U)-B(W),U-W\bigr\rangle_{L^{2}}=\int_{\mathbb{T}^{n}}b\,\bigl(u^{3}-w^{3}\bigr)\,(u-w)\,dx .

By the pointwise inequality just proved and 0≤b0\le b, the integrand is nonnegative at every point of QQ, by clause 2 of Ordered Field. Comparing it with the zero function, claim 2 of Linearity and Monotonicity of the Lebesgue Integral, and the Integrability Criterion gives that the integral is nonnegative. Thus BB is monotone.

Claim 3. Let RR and UU be as in the claim and let uu be a representative of UU. By The Riesz–Fischer Theorem (i) the norm of L2(Tn)L^{2}(\mathbb{T}^{n}) is absolutely homogeneous and ∥[v]∥L2=∥v∥2\lVert[v]\rVert_{L^{2}}=\lVert v\rVert_{2}, so, using ∣b∣=b|b|=b from (R1),

∥B(U)∥L2=b ∥u3∥2≤b⋅125 (∥U∥H1)3,\lVert B(U)\rVert_{L^{2}}=b\,\lVert u^{3}\rVert_{2}\le b\cdot125\,\bigl(\lVert U\rVert_{H^{1}}\bigr)^{3},

the inequality by claim 1 together with claim 5 of Elementary Arithmetic in an Ordered Field and the nonnegative multiplier bb. Norms are nonnegative by Real Inner Product Spaces (ii), so (R3) applied to 0≤∥U∥H1≤R0\le\lVert U\rVert_{H^{1}}\le R gives (∥U∥H1)3≤R3(\lVert U\rVert_{H^{1}})^{3}\le R^{3}, and multiplying by the nonnegative number 125 b125\,b yields ∥B(U)∥L2≤125 b R3\lVert B(U)\rVert_{L^{2}}\le125\,b\,R^{3}. As RR was an arbitrary positive real number and 125bR3125bR^{3} does not depend on UU, BB is bounded on VV-bounded sets.

Claim 4. Let U∈D(A)U\in D(A). By Hilbert Triples: Standing Notation and Background (iii) we have U∈H1(Tn)U\in H^{1}(\mathbb{T}^{n}), AU∈L2(Tn)AU\in L^{2}(\mathbb{T}^{n}) and

⟨AU,Y⟩L2=⟨U,Y⟩H1for every Y∈H1(Tn).\bigl\langle AU,Y\bigr\rangle_{L^{2}}=\bigl\langle U,Y\bigr\rangle_{H^{1}}\qquad\text{for every }Y\in H^{1}(\mathbb{T}^{n}).

Let uu be a representative of UU, let gjg_{j} be a representative of ∂jU\partial_{j}U for j∈[n]j\in[n], and let zz be a representative of AUAU.

By Existence of a Sequence of Positive Real Numbers with Limit Zero there is a sequence (εm)m∈N(\varepsilon_{m})_{m\in\mathbb{N}} of positive real numbers converging to 00. Fix m∈Nm\in\mathbb{N} and let ϕεm\phi_{\varepsilon_{m}} be the function of A Bounded-Derivative Truncation of the Cube Map on the Real Line (i) for the parameter εm\varepsilon_{m}. By A Bounded-Derivative Truncation of the Cube Map on the Real Line (ii) it is of class C1C^{1} on R1\mathbb{R}^{1} with ∂1ϕεm=ϕεm′\partial_{1}\phi_{\varepsilon_{m}}=\phi_{\varepsilon_{m}}', and by A Bounded-Derivative Truncation of the Cube Map on the Real Line (iii) together with (R1) its derivative satisfies ∣ϕεm′(s)∣≤4 εm−1|\phi_{\varepsilon_{m}}'(s)|\le4\,\varepsilon_{m}^{-1} for every s∈Rs\in\mathbb{R}. Hence The Chain Rule for Weak Derivatives on the Torus applies with ϕ=ϕεm\phi=\phi_{\varepsilon_{m}} and M=4εm−1M=4\varepsilon_{m}^{-1}, which is nonnegative by claim 7 of Elementary Order Arithmetic in an Ordered Field: by The Chain Rule for Weak Derivatives on the Torus (ii) the class ϕεm(U)=[ϕεm∘u]\phi_{\varepsilon_{m}}(U)=[\phi_{\varepsilon_{m}}\circ u] lies in L2(Tn)L^{2}(\mathbb{T}^{n}), and by The Chain Rule for Weak Derivatives on the Torus (iii) it lies in H1(Tn)H^{1}(\mathbb{T}^{n}) with ∂jϕεm(U)=[(ϕεm′∘u) gj]\partial_{j}\phi_{\varepsilon_{m}}(U)=[(\phi_{\varepsilon_{m}}'\circ u)\,g_{j}] for every j∈[n]j\in[n].

Taking Y=ϕεm(U)Y=\phi_{\varepsilon_{m}}(U) in the displayed identity and expanding the Sobolev inner product by The Sobolev Space of Once Weakly Differentiable Square-Integrable Classes on the Torus (ii) and then each L2L^{2} inner product by claim 1 of L²(μ) Is a Real Hilbert Space (i),

⟨AU,ϕεm(U)⟩L2=∫Tnu (ϕεm∘u) dx+∑j=1n∫Tn(ϕεm′∘u) gj gj dx.\bigl\langle AU,\phi_{\varepsilon_{m}}(U)\bigr\rangle_{L^{2}} =\int_{\mathbb{T}^{n}}u\,\bigl(\phi_{\varepsilon_{m}}\circ u\bigr)\,dx +\sum_{j=1}^{n}\int_{\mathbb{T}^{n}}\bigl(\phi_{\varepsilon_{m}}'\circ u\bigr)\,g_{j}\,g_{j}\,dx .

Every integrand here is nonnegative at every point of QQ: the first by A Bounded-Derivative Truncation of the Cube Map on the Real Line (iv), and each of the others because 0≤ϕεm′0\le\phi_{\varepsilon_{m}}' by A Bounded-Derivative Truncation of the Cube Map on the Real Line (iii) and 0≤gj(x)20\le g_{j}(x)^{2} by (R2), so that clause 2 of Ordered Field applies. By claim 2 of Linearity and Monotonicity of the Lebesgue Integral, and the Integrability Criterion each integral is therefore nonnegative, and by Finite Sums of Real Numbers: Nonnegativity, Domination by the Sum, and Limits (i) so is the finite sum. Hence

0≤⟨AU,ϕεm(U)⟩L2=∫Tnz (ϕεm∘u) dx,0\le\bigl\langle AU,\phi_{\varepsilon_{m}}(U)\bigr\rangle_{L^{2}}=\int_{\mathbb{T}^{n}}z\,\bigl(\phi_{\varepsilon_{m}}\circ u\bigr)\,dx ,

the equality again by claim 1 of L²(μ) Is a Real Hilbert Space (i).

We now let mm grow. Let x∈Qx\in Q. By A Bounded-Derivative Truncation of the Cube Map on the Real Line (v),

∣ϕεm(u(x))−u(x)3∣≤εm ∣u(x)∣5,\bigl|\phi_{\varepsilon_{m}}(u(x))-u(x)^{3}\bigr|\le\varepsilon_{m}\,|u(x)|^{5},

and the right-hand side converges to 00 by Arithmetic of Limits of Real Sequences, being the constant ∣u(x)∣5|u(x)|^{5} times a sequence converging to 00; so claim 3 of Order Properties of Limits of Real Sequences shows that (ϕεm(u(x)))m∈N(\phi_{\varepsilon_{m}}(u(x)))_{m\in\mathbb{N}} converges to u(x)3u(x)^{3}, and Arithmetic of Limits of Real Sequences then shows that (z(x) ϕεm(u(x)))m∈N(z(x)\,\phi_{\varepsilon_{m}}(u(x)))_{m\in\mathbb{N}} converges to z(x) u(x)3z(x)\,u(x)^{3}. Moreover, by A Bounded-Derivative Truncation of the Cube Map on the Real Line (iv) and claim 4 of Properties of the Absolute Value in an Ordered Field,

∣z(x) ϕεm(u(x))∣=∣z(x)∣ ∣ϕεm(u(x))∣≤∣z(x)∣ ∣u(x)∣3\bigl|z(x)\,\phi_{\varepsilon_{m}}(u(x))\bigr|=|z(x)|\,\bigl|\phi_{\varepsilon_{m}}(u(x))\bigr|\le|z(x)|\,|u(x)|^{3}

for every mm, using claim 5 of Elementary Arithmetic in an Ordered Field with the nonnegative multiplier ∣z(x)∣|z(x)|. The functions ∣z∣|z| and ∣u∣3|u|^{3} lie in L2(Tn)\mathcal{L}^{2}(\mathbb{T}^{n}), the first by Elementary Properties of the p-Seminorm (iii) and the second by claim 1, so their pointwise product is integrable by claim 1 of L²(μ) Is a Real Hilbert Space (i). Each function z (ϕεm∘u)z\,(\phi_{\varepsilon_{m}}\circ u) is measurable, being a product of measurable functions by claim 3 of Arithmetic of Measurable Real- and [0,∞]-Valued Maps, and so is z u3z\,u^{3}. By Dominated Convergence Theorem,

∫Tnz (ϕεm∘u) dx⟶∫Tnz u3 dx.\int_{\mathbb{T}^{n}}z\,\bigl(\phi_{\varepsilon_{m}}\circ u\bigr)\,dx\longrightarrow\int_{\mathbb{T}^{n}}z\,u^{3}\,dx .

Every term of the left-hand sequence is nonnegative, so comparing with the constant sequence 00 and applying claim 1 of Order Properties of Limits of Real Sequences gives

0≤∫Tnz u3 dx=⟨AU,[u3]⟩L2.0\le\int_{\mathbb{T}^{n}}z\,u^{3}\,dx=\bigl\langle AU,[u^{3}]\bigr\rangle_{L^{2}} .

Finally, by the symmetry and bilinearity of the inner product, Real Inner Product Spaces (i), and 0≤b0\le b,

⟨B(U),AU⟩L2=b ⟨[u3],AU⟩L2=b∫Tnz u3 dx≥0,\bigl\langle B(U),AU\bigr\rangle_{L^{2}}=b\,\bigl\langle[u^{3}],AU\bigr\rangle_{L^{2}}=b\int_{\mathbb{T}^{n}}z\,u^{3}\,dx\ge0 ,

using claim 5 of Elementary Arithmetic in an Ordered Field with the nonnegative multiplier bb. Thus BB is AA-monotone.

Claim 5. By claim 1 the map BB sends V=H1(Tn)V=H^{1}(\mathbb{T}^{n}) into H=L2(Tn)H=L^{2}(\mathbb{T}^{n}); by claims 2, 3 and 4 it is monotone, bounded on VV-bounded sets and AA-monotone. By Monotone, AA-Monotone and Locally Bounded Nonlinearities on a Hilbert Triple (iv), BB is a monotone nonlinearity for (H,V,A)(H,V,A).

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