
In this paper, we introduce the Laguerre bounded variation space and the Laguerre perimeter, thereby investigating their properties. Moreover, we prove the isoperimetric inequality and the Sobolev inequality in the Laguerre setting. As applications, we derive the mean curvature for the Laguerre perimeter.
Citation: He Wang, Yu Liu. Laguerre BV spaces, Laguerre perimeter and their applications[J]. Communications in Analysis and Mechanics, 2023, 15(2): 189-213. doi: 10.3934/cam.2023011
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In this paper, we introduce the Laguerre bounded variation space and the Laguerre perimeter, thereby investigating their properties. Moreover, we prove the isoperimetric inequality and the Sobolev inequality in the Laguerre setting. As applications, we derive the mean curvature for the Laguerre perimeter.
The spaces BV of functions of bounded variation in Euclidean spaces have been a class of function space which can be used in the geometric measure theory. For example, when working with minimization problems, reflexivity or the weak compactness property involving the function space W1,p(Rd) for p>1, in such cases, the space BV usually plays a crucial role. However, for the case of the space W1,1(Rd), one possible approach to address its lack of reflexivity is to consider the space BV(Rd). The importance of generalizing the classical notion of variation has been pointed out in several occasions by E. De. Giorgi in [1]. Recently, Huang, Li and Liu in [2] investigate the capacity and perimeters derived from α-Hermite bounded variation. In a general framework of strictly local Dirichlet spaces with doubling measure, Alonso-Ruiz, Baudoin and Chen et al. in [3] introduce the class of bounded variation functions and proved the Sobolev inequality under the Bakry-ˊEmery curvature type condition. For further information on this topic, we refer the reader to [4,5,6] and the references therein.
One of the aims of this paper is intended to explore and analyze a number of fundamental inquiries in geometric measure theory that are associated with the Laguerre operator in Laguerre BV spaces. To begin with, we will provide a brief introduction to the Laguerre operator.
Given a multiindex α=(α1,⋯,αd), α∈(−1,∞)d, the Laguerre differential operator is defined by:
Lα=−d∑i=1[xi∂2∂xi2+(αi+1−xi)∂∂xi]. |
Let the probabilistic gamma measure μα in Rd+=(0,∞)d be defined as
dμα(x)=d∏i=1xiαie−xiΓ(αi+1)dx:=ω(x)dx. |
As we know that Lα is positive and symmetric in L2(Rd+,dμα), and it has a closure which is selfadjoint in L2(Rd+,dμα) and will be denoted by Lα. The i-th partial derivative associated with Lα is defined as
δi=√xi∂∂xi, |
see [7] or [8]. The operator Lα has the following decomposition:
Lα=d∑i=1δ∗iδi, |
where
δ∗i=−√xi(∂xi+αi+12−xixi) |
is the formal adjoint of δi in L2(Rd+,dμα). Throughout this paper, suppose that Ω⊂Rd+ be an open set. For u∈C1(Rd+) and φ=(φ1,φ2,…,φd)∈C1(Rd+,Rd), define the Lα-gradient and Lα-divergence operators that are associated with Lα:
{∇Lαu:=(δ1u,…,δdu),divLαφ:=δ∗1φ1+δ∗2φ2+⋯+δ∗dφd, |
which also gives
Lαu=divLα(∇Lαu)=−d∑i=1[xi∂2∂xi2+(αi+1−xi)∂∂xi]. |
Naturally, we denote by BVLα(Ω) the set of all functions possessing Laguerre bounded variation (Lα-BV in short) on Ω. Based on the results of [2], we investigate some related topics for the Laguerre setting, and the plan of the notes is given as follows. Section 2.1 collects some basic facts and notations used later, the lower semicontinuity (Lemma 2.1), the completeness (Lemma 2.2), the structure theorem (Theorem 2.3) and approximation via C∞c-functions (Theorem 2.4). Unlike Theorem 2 in [9, Section 5.2.2], we must utilize the mean value theorem for multivariate functions and the intrinsic nature of the Laguerre variation. Section 2.2 is focused on the perimeter PLα(⋅,Ω) induced by BVLα(Ω), as shown in equation (2.6) below.
Remember that the classical perimeter of E⊆Rd is defined as
P(E)=supφ∈F(Rd){∫Edivφ(x)dx}, |
here let F(Rd) be the set that contains all functions
φ=(φ1,⋯,φd)∈C1c(Rd,Rd) |
satisfying
‖φ‖∞=supx∈E{(|φ1(x)|2+⋯+|φd(x)|2)12}≤1. |
As we all know that
P(E)=P(Ec), ∀E⊂Rd | (1.1) |
is an inherent property of P(E) at the elementary level.
In Lemma 2.10, we proved that (1.1) is valid for the Laguerre perimeter PLα(⋅). In Section 2.3, a coarea formula for Lα-BV functions is derived. In Theorem 2.12, we conclude that the isoperimetric inequality
‖f‖Ldd−1(Ω1,dμα)≲|∇Lαf|(Ω1) | (1.2) |
shares equivalence with the Sobolev type inequality
μα(E)d−1d≲PLα(E,Ω1) |
as an application. We point out that, in the proof of (1.2), the inequality |∇f(x)|≲|∇Lαf(x)| on Ω1 holds true. With this in mind, we consider the subset
Ω1=Ω∖{x∈Rd+:∃i∈1,⋯,d such that √xi<1} | (1.3) |
of Ω which is a reasonable substitute of Ω and whose figure is given as follows:
Our motivation comes not only from the fact that these objects are interesting on their own, but also from the possibility of their potential applications in further research concerning the Laguerre operator. Consequently, our aim in Section 3 is to examine the Laguerre mean curvature of a set that has a finite Laguerre perimeter. It is interesting to note that the sets of finite perimeter introduced by E. De Giorgi for the Laplace operator Δ have found applications in classical problems of the calculus of variations, such as the Plateau problem and the isoperimetric problem, see [10,11,12]. Barozzi, Gonzalez, and Tamanini [13] demonstrated that for any finite classical perimeter set E within Rd, its mean curvature is included in L1(Rd). One might naturally wonder whether PLα(E,Ω), α∈(−1,∞)d holds similarly as [13]. Note that it is necessary to use identity (1.1) in the proof of the main theorem of [13]. In Theorem 3.1, we generalize the result of [13] to PLα(⋅,Ω1) and show that if a set E is a subset of Ω1 such that PLα(E,Ω1)<∞, then the mean curvature of E is in L1(Ω1,dμα).
Throughout this paper by C we always denote a positive constant that may vary at each occurrence; A≈B means that 1CA≤B≤CA and the notation X≲Y is used to indicate that X≤CY with a positive constant C independent of significant quantities. Similarly, one writes X≳Y for X≥CY.
This section presents the Lα-BV space, which is defined as the set of all functions that exhibit Laguerre bounded variation and investigates its properties. The Laguerre variation (Lα-variation in short) of f∈L1(Ω,dμα) is defined by
|∇Lαf|(Ω)=supφ∈F(Ω){∫Ωf(x)divLαφ(x)dμα(x)}, |
where F(Ω) denotes the class of all functions
φ=(φ1,φ2,…,φd)∈C1c(Ω,Rd) |
satisfying
‖φ‖L∞=supx∈Ω{(|φ1(x)|2+…+|φd(x)|2)12}≤1. |
We say that an function f∈L1(Ω,dμα) has the Lα-bounded variation on Ω if
|∇Lαf|(Ω)<∞, |
and denote by BVLα(Ω) the class of all such functions, and it is a Banach space with the norm
‖f‖BVLα(Ω)=‖f‖L1(Ω,dμα)+|∇Lαf|(Ω). |
Definition 2.1. Suppose Ω is an open set in Rd+. Let 1≤p≤∞. The Sobolev space Wk,pLα(Ω) associated with Lα is defined as the set of all functions f∈Lp(Ω,dμα) such that
δj1…δjmf∈Lp(Ω,dμα), 1≤j1,…,jm≤d, 1≤m≤k. |
The norm of f∈Wk,pLα(Ω) is given by
‖f‖Wk,pLα:=∑1≤j1…jm≤d, 1≤m≤k‖δj1…δjmf‖Lp(Ω,dμα)+‖f‖Lp(Ω,dμα). |
The upcoming results will gather certain properties of the space BVLα(Ω). We omit the details of their proofs, since we can use the similar arguments as [2] to prove them.
Lemma 2.1. (i) Suppose f∈W1,1Lα(Ω), then
|∇Lαf|(Ω)=∫Ω|∇Lαf(x)|dμα(x), |
which implies W1,1Lα(Ω)⊆BVLα(Ω).
(ii) (Lower semicontinuity). Suppose fk∈BVLα(Ω), k∈N and fk→f in L1loc(Ω,dμα), then
|∇Lαf|(Ω)≤liminfk→∞|∇Lαfk|(Ω). |
Lemma 2.2. The space (BVLα(Ω),‖⋅‖BVLα(Ω)) is a Banach space.
The Hahn-Banach theorem and the Riesz representation theorem can be used to prove the structure theorem for Lα-BV functions, as presented in the following lemma.
Lemma 2.3. (Structure theorem for BVLα functions). Let f∈BVLα(Ω). Then there exists a Radon measure μLα on Ω such that
∫Ωf(x)divLαφ(x)dμα(x)=∫Ωφ(x)⋅dμLα(x) |
for every φ∈C∞c(Ω,Rd) and
|∇Lαf|(Ω)=|μLα|(Ω), |
where |μLα| represents the total variation of the measure μLα.
We can obtain an approximation result for the Lα-variation in the following theorem.
Theorem 2.4. Let Ω1 be an open set defined in (1.3). Assume that u∈BVLα(Ω1), then there exists a sequence {uh}h∈N∈BVLα(Ω1)∩C∞(Ω1) such that
limh→∞‖uh−u‖L1(Ω1,dμα)=0 |
and
limh→∞∫Ω1|∇Lαuh(x)|dμα(x)=|∇Lαu|(Ω1). |
Proof. The approach we take differs from the proof presented in [9, Section 5.2.2, Theorem 2] as we utilize the mean value theorem of multivariate functions and the intrinsic nature of the Lα-variation. Via the lower semicontinuity of Lα-BV functions, it suffices to demonstrate that for ε>0 there exists a function uε∈C∞(Ω1) such that
∫Ω1|uε(x)−u(x)|dμα(x)<ε |
and
|∇Lαuε|(Ω1)≤|∇Lαu|(Ω1)+ε. |
Fix ε>0. If m is a given positive integer, then construct a series of open sets,
Ω1,j:={x∈Ω1:dist(x,∂Ω1)>1m+j}∩B(0,m+j), j∈N, |
where dist(x,∂Ω1)=inf{|x−y|:y∈∂Ω1}. Note that Ω1,j⊂Ω1,j+1⊂Ω1, j∈N and ∞∪j=0Ω1,j=Ω1. Since |∇Lαu|(⋅) is a measure, then choose a value m∈N to be sufficiently large such that
|∇Lαu|(Ω1∖Ω1,0)<ε. | (2.1) |
Set U0:=Ω1,0 and Uj:=Ω1,j+1∖¯Ω1,j−1 for j≥1. Based on the standard outcomes from [9, Section 5.2.2, Theorem 2], our inference is that there exists a partition of unity connected to the covering {Uj}j∈N. Namely, there exist functions {fj}j∈N∈C∞c(Uj) such that 0≤fj≤1, j≥0 and ∞∑j=0fj=1 on Ω1. Thus we have the fact that
∞∑j=0∇Lαfj=(√x1∂∂x1(∞∑j=0fj),√x2∂∂x2(∞∑j=0fj),⋯,√xd∂∂xd(∞∑j=0fj))=0 | (2.2) |
on Ω1. Given ε>0 and u∈L1(Ω1,R), extended to zero out of Ω1, the regularization can be defined as
uε(x):=1εd∫B(x,ε)η(x−yε)u(y)dμα(y), |
where η∈C∞c(Rd+) is a nonnegative radial function satisfying
1ϵdj∫Rd+η(x−yϵj)dμα(x)=1, ∀ j∈N, |
and supp η⊂B(0,1)∩Rd+. Then for each j, there exists 0<εj<ε so small such that
{supp((fju)εj)⊆Uj,∫Ω1|(fju)εj(x)−fju(x)|dμα(x)<ε2−(j+1),∫Ω1|(u∇Lαfj)εj(x)−u∇Lαfj(x)|dμα(x)<ε2−(j+1). | (2.3) |
Construct
vε(x):=∞∑j=0(ufj)εj(x). |
In some neighborhood of each point x∈Ω1, there are only finitely many nonzero terms in this sum, hence vε∈C∞(Ω1) and u=∞∑j=0ufj. Therefore, by a simple computation, we obtain
‖vε−u‖L1(Ω1,dμα)≤∞∑j=0∫Ω1|(fju)εj(x)−fj(x)u(x)|dμα(x)<ε. |
Consequently,
vε→u in L1(Ω1,dμα) as ε→0. |
Now, assume φ∈C1c(Ω1,Rd) and |φ|≤1. We decompose the integral as follows:
∫Ω1vε(x)divLαφ(x)dμα(x)=∫Ω1(∞∑j=0(ufj)εj(x))divLαφ(x)dμα(x)=∞∑j=0∫Ω1(ufj)εj(x)(δ∗1φ1(x)+δ∗2φ2(x)+⋯+δ∗dφd(x))dμα(x):=I+II, |
where
{I:=−∞∑j=0∫Ω1(ufj)εj(x)(√x1∂∂x1φ1(x)+⋯+√xd∂∂xdφd(x))dμα(x),II:=−∞∑j=0∫Ω1(ufj)εj(x)(α1+12−x1√x1φ1(x)+⋯+αd+12−xd√xdφd(x))dμα(x). |
For the sake of research, let
~divLαφ=δ1φ1+δ2φ2+⋯+δdφd. | (2.4) |
As for I, we obtain
I=−∞∑j=0∫Ω1(ufj)εj(x)~divLαφ(x)dμα(x)=−∞∑j=0∫Ω1(ufj)(y)~divLα(ηεj∗φ(y))dμα(y)=−∞∑j=0∫Ω1u(y)~divLα(fj(ηεj∗φ))(y)dμα(y)+∞∑j=0∫Ω1u(y)∇Lαfj⋅(ηεj∗φ)(y)dμα(y)=−∞∑j=0∫Ω1u(y)~divLα(fj(ηεj∗φ))(y)dμα(y)−∞∑j=0∫Ω1φ(y)(ηεj∗(u∇Lαfj)(y)−u∇Lαfj(y))dμα(y):=I1+I2, |
where in the last equality we have used the fact (2.2). In fact, when ‖φ‖L∞≤1, then |fj(ηεj∗φ)(x)|≤1, j∈N, and each point in Ω is contained in at most three of the sets {Uj}∞j=0. Furthemore, (2.3) implies that |I2|<ε.
On the other hand, we modify the integration order to obtain
II=−∞∑j=0∫Ω1(ufj)εj(x)(α1+12−x1√x1φ1(x)+⋯+αd+12−xd√xdφd(x))dμα(x)=−∞∑j=0∫Ω1∫Ω11εdjη(x−yεj)u(y)fj(y)(d∑k=1αk+12−yk√ykφk(x))dμα(y)dμα(x)−∞∑j=0∫Ω1∫Ω11εdjη(x−yεj)u(y)fj(y)×(d∑k=1(αk+12−xk√xk−αk+12−yk√yk)φk(x))dμα(y)dμα(x)=−∞∑j=0∫Ω1u(y)fj(y)((d∑k=1αk+12−yk√ykφk)∗ηεj(y))dμα(y)−∞∑j=0∫Ω1∫Ω11εdjη(x−yεj)u(y)fj(y)×(d∑k=1(αk+12−xk√xk−αk+12−yk√yk)φk(x))dμα(y)dμα(x). |
Therefore, the estimation presented for term I2 above indicates that
|∫Ω1vε(x)divLαφ(x)dμα(x)|=|I1+I2+II|≤J1+J2+ε, |
where
J1:=|−∞∑j=0∫Ω1u(y)~div(fj(ηεj∗φ))(y)dμα(y)−∞∑j=0∫Ω1u(y)fj(y)(d∑k=1αk+12−yk√yk(φk∗ηεj(y)))dμα(y)| |
and
J2:=|−∞∑j=0∫Ω1∫Ω11εdjη(x−yεj)u(y)fj(y)×(d∑k=1(αk+12−xk√xk−αk+12−yk√yk)φk(x))dμα(y)dμα(x)|. |
Furthermore,
J1=|−∞∑j=0∫Ω1u(y)~divLα(fj(ηεj∗φ))(y)dμα(y)−∞∑j=0∫Ω1u(y)fj(y)(d∑k=1αk+12−yk√ykφk∗ηεj(y))dμα(y)|≤|−∫Ω1u(y)~divLα(f0(ηε0∗φ))(y)dμα(y)−∫Ω1u(y)f0(y)(d∑k=1αk+12−yk√ykφk∗ηε0(y))dμα(y)|+|−∞∑j=1∫Ω1u(y)~divLα(fj(ηεj∗φ))(y)dμα(y)−∞∑j=1∫Ω1u(y)fj(y)(d∑k=1αk+12−yk√ykφk∗ηεj(y))dμα(y)|≤|∇Lαu|(Ω1)+∞∑j=1|∇Lαu|(Uj)≤|∇Lαu|(Ω1)+|∇Lαu|(Ω1∖Ω1,0)≤|∇Lαu|(Ω1)+3ε, |
where we applied the fact (2.1) in the final inequality. Note that ψ(xk)=αk+12−xk√xk, ‖φ‖L∞≤1 and supp η⊆B(0,1)∩Rd+. Assuming |xk−yk|<εj<|yk|/2, the mean value theorem of multivariate functions guarantees the existence of θ∈(0,1) such that
|ψ(xk)−ψ(yk)|=|αk+122(yk+θ(xk−yk))−32+12(yk+θ(xk−yk))−12||xk−yk|≤(|αk+12|2|yk+θ(xk−yk)|−32+12|yk+θ(xk−yk)|−12)|xk−yk|. |
Consequently, we obtain
J2=|∞∑j=0∫Ω1∫Ω11εdjη(x−yεj)u(y)fj(y)(d∑k=1(αk+12−xk√xk−αk+12−yk√yk)φk(x))×dμα(y)dμα(x)|≤εj2∞∑j=0∫Ω1∫Ω1|1εdjη(x−yεj)u(y)fj(y)|d∑k=1|αk+12||yk+θ(x−yk)|−32×|φk(x)|dμα(y)dμα(x)+εj2∞∑j=0∫Ω1∫Ω1|1εdjη(x−yεj)u(y)fj(y)|d∑k=1|yk+θ(xk−yk)|−12×|φk(x)|dμα(y)dμα(x)≤Cεj∞∑j=0∫Ω1∫Ω1|1εdjη(x−yεj)u(y)fj(y)|d∑k=1|αk+12||yk|−32dμα(y)dμα(x)+Cεj∞∑j=0∫Ω1∫Ω1|1εdjη(x−yεj)u(y)fj(y)|d∑k=1|yk|−12dμα(y)dμα(x)≤Cεj∞∑j=0∫Ω1∫Ω1|1εdjη(x−yεj)|dμα(x)d∑k=1|αk+12||u(y)||fj(y)||yk|−32dμα(y)+Cεj∞∑j=0∫Ω1∫Ω1|1εdjη(x−yεj)|dμα(x)d∑k=1|u(y)||fj(y)||yk|−12dμα(y)≤Cεj∫Rd+|1ϵdjη(x−yϵj)|dμα(x)d∑k=1∫Ω1|αk+12||u(y)||∞∑j=0fj(y)||yk|−32dμα(y)+Cεj∫Rd+|1ϵdjη(x−yϵj)|dμα(x)d∑k=1∫Ω1|u(y)||∞∑j=0fj(y)||yk|−12dμα(y)=Cεj∫Ω1|u(y)|d∑k=1|αk+12||yk|−32dμα(y)+Cεj∫Ω1|u(y)|d∑k=1|yk|−12dμα(y)≲ε, |
where we have used the facts that
{∫Ω1|u(y)|d∑k=1|yk|−12dμα(y)<∞,∫Ω1|u(y)|d∑k=1|αk+12||yk|−32dμα(y)<∞, | (2.5) |
and in the third inequality we have used the fact that
|yk+θ(xk−yk)|≥|yk|−θ|xk−yk|=(1−θ2)|yk|. |
Through taking the supremum over φ and considering the arbitrariness of ε>0, we prove the theorem.
Remark 2.5. By computation, we conclude that the function u∈BVLα(Ω) satisfies (2.5) in Theorem 2.4 when d≥3, at this time, Theorem 2.4 is valid for any open set Ω⊆Rd.
Additionally, the max-min property of the Lα-variation can be observed from Lemma 2.1 and Theorem 2.4.
Theorem 2.6. Let Ω1 be an open set defined in (1.3). Suppose u,v∈L1(Ω1,dμα), then
|∇Lαmax{u,v}|(Ω1)+|∇Lαmin{u,v}|(Ω1)≤|∇Lαu|(Ω1)+|∇Lαv|(Ω1). |
Proof. One may assume, without any loss of generality,
|∇Lαu|(Ω1)+|∇Lαv|(Ω1)<∞. |
By Theorem 2.4, we take two functions
uh,vh∈BVLα(Ω1)∩C∞c(Ω1), h=1,2,..., |
such that
{uh→u,vh→v in L1(Ω1,dμα),∫Ω1|∇Lαuh(x)|dμα(x)→|∇Lαu|(Ω1),∫Ω1|∇Lαvh(x)|dμα(x)→|∇Lαv|(Ω1). |
Since
max{uh,vh}→max{u,v} & min{uh,vh}→min{u,v} in L1(Ω1,dμα). |
Via Lemma 2.1, it follows that
|∇Lαmax{u,v}|(Ω1)+|∇Lαmin{u,v}|(Ω1)≤liminfh→∞∫Ω1|∇Lαmax{uh,vh}|dμα(x)+liminfh→∞∫Ω1|∇Lαmin{uh,vh}|dμα(x)≤liminfh→∞(∫Ω1|∇Lαmax{uh,vh}|dμα(x)+∫Ω1|∇Lαmin{uh,vh}|dμα(x))≤liminfh→∞(∫{x∈Ω1:uh≤vh}|∇Lαvh|dμα(x)+∫{x∈Ω1:uh>vh}|∇Lαuh|dμα(x)+∫{x∈Ω1:uh≤vh}|∇Lαuh|dμα(x)+∫{x∈Ω1:uh>vh}|∇Lαvh|dμα(x))=liminfh→∞∫Ω1|∇Lαuh(x)|dμα(x)+liminfh→∞∫Ω1|∇Lαvh(x)|dμα(x)≤limh→∞∫Ω1|∇Lαuh(x)|dμα(x)+limh→∞∫Ω1|∇Lαvh(x)|dμα(x)=|∇Lαu|(Ω1)+|∇Lαv|(Ω1). |
This subsection presents a new type of perimeter: the Laguerre perimeter (Lα-perimeter in short). Moreover, we establish the related results for it.
We define the Lα-perimeter of E⊂Ω as follows:
PLα(E,Ω)=|∇Lα1E|(Ω)=supφ∈F(Ω){∫EdivLαφ(x)dμα(x)}, | (2.6) |
where F(Ω) is defined in Section 2.1. Specifically, we will also use the notation
PLα(E,Rd+)=PLα(E). |
We immediately deduce Lemma 2.1 by replacing f with 1E.
Corollary 2.7. (Lower semicontinuity of PLα). Assume 1Ek→1E in L1loc(Ω,dμα), where E and Ek, k∈N, are subsets of Ω, then
PLα(E,Ω)≤liminfk→∞PLα(Ek,Ω). |
Additionally, utilizing Theorem 2.6 and selecting u=1E and v=1F for every compact subsets E,F in Ω1, we can promptly acquire the subsequent corollary. According to Xiao and Zhang's result in [14, Section 1.1 (ⅲ)], the equality condition of (2.7) is also provided by us.
Corollary 2.8. For all compact subsets E,F within Ω1, we get
PLα(E∩F,Ω1)+PLα(E∪F,Ω1)≤PLα(E,Ω1)+PLα(F,Ω1), | (2.7) |
where Ω1 is an open set defined in (1.3). Especially, if PLα(E∖(E∩F),Ω1)⋅PLα(F∖(F∩E),Ω1)=0, the equality of (2.7) holds true.
Proof. Given that (2.7) is true, we only need to demonstrate that its opposite inequality is also valid, provided that the above condition is satisfied. It is evident that the condition PLα(E∖(E∩F),Ω1)⋅PLα(F∖(E∩F),Ω1)=0 leads to PLα(E∖(E∩F),Ω1)=0 or PLα(F∖(E∩F),Ω1)=0. Suppose PLα(E∖(E∩F),Ω1)=0. By (2.7), we have
PLα(E,Ω1)=PLα((E∖(E∩F))∪(E∩F),Ω1)≤PLα(E∖(E∩F),Ω1)+PLα(E∩F,Ω1)=PLα(E∩F,Ω1). | (2.8) |
Via (2.6) and E∪F=F∪(E∖(E∩F)), we have
PLα(F,Ω1)=supφ∈F(Ω1){∫FdivLαφ(x)dμα(x)}=supφ∈F(Ω1){∫E∪FdivLαφ(x)dμα(x)−∫E∖(E∩F)divLαφ(x)dμα(x)}≤supφ∈F(Ω1){∫E∪FdivLαφ(x)dμα(x)}+supφ∈F(Ω1){∫E∖(E∩F)divLαφ(x)dμα(x)}=PLα(E∪F,Ω1)+PLα(E∖(E∩F),Ω1)=PLα(E∪F,Ω1). | (2.9) |
Combining (2.8) with (2.9) deduces that
PLα(E,Ω1)+PLα(F,Ω1)≤PLα(E∪F,Ω1)+PLα(E∩F,Ω1), |
the desired result can be obtained from it. Another similar case can be proven as well, but the details are omitted.
We will now demonstrate that sets with finite Lα-perimeter satisfy the Gauss-Green formula.
Theorem 2.9. (Gauss-Green formula). Let E⊆Ω be subset with finite Lα-perimeter. Then we have
∫E~divLαφ(x)dμα(x)=−∫∂Ec(√x1φ1(x),⋯,√xdφd(x))⋅→nω(x)dHd−1(x)−∫Ed∑i=1αi+12−xi√xiφi(x)ω(x)dx, |
where the outward normal to E is represented by the unit vector →n(x) and ~divLα(⋅) is defined in (2.4).
Proof. By calculating, we have
∫E~divLαφ(x)dμα(x)=∫E(d∑i=1√xi∂∂xiφi(x))ω(x)dx=∫Ediv(√x1φ1(x)ω(x),⋯,√xdφd(x)ω(x))dx−∫Ed∑i=1√xiφi(x)∂∂xiω(x)dx−12∫Ed∑i=11√xiφi(x)ω(x)dx=−∫∂Ec(√x1φ1(x),⋯,√xdφd(x))⋅→nω(x)dHd−1(x)−∫Ed∑i=1√xiφi(x)∂∂xiω(x)dx−12∫Ed∑i=11√xiφi(x)ω(x)dx=−∫∂Ec(√x1φ1(x),⋯,√xdφd(x))⋅→nω(x)dHd−1(x)−∫Ed∑i=1αi+12−xi√xiφi(x)ω(x)dx, |
where we have used the classical Gauss-Green formula and the following facts regarding the derivatives of ω(x):
∂∂xi(d∏j=1xjαje−xjΓ(αj+1))=d∏j=1,j≠ixjαje−xjΓ(αj+1)1Γ(αi+1)(−e−xixiαi+αie−xixiαi−1)=(−1+αixi)ω(x) |
for 1≤i≤d. This completes the proof.
Lemma 2.10. If a set E is in Ω and has finite Lα-perimeter, then
PLα(E,Ω)=PLα(Ω∖E,Ω). |
Proof. For any φ∈F(Rd+), since PLα(E,Ω)<∞, then
supφ∈F(Rd+)∫EdivLαφ(x)dμα(x)<∞. |
Via the extended Gauss-Green formula (Theorem 2.9) and taking into consideration the fact that φ has a compact support, we obtain
∫EdivLαφ(x)dμα(x)=−∫E~divLα(φ1(x),…,φd(x))dμα(x)−∫Ed∑k=1αi+12−xi√xiφi(x)dμα(x)=∫∂Ec(√x1φ1(x),⋯,√xdφd(x))⋅→nω(x)dHd−1(x)+∫Ed∑k=1αi+12−xi√xiφi(x)dμα(x)−∫Ed∑k=1αi+12−xi√xiφi(x)dμα(x)=∫∂E(√x1φ1(x),⋯,√xdφd(x))⋅→nω(x)dHd−1(x)=−∫Ec~divLαφ(x)dμα(x)−∫Ecd∑k=1αi+12−xi√xiφi(x)dμα(x)=∫EcdivLαφ(x)dμα(x), |
where the unit exterior normal vector to E at x is denoted by →n(x). The arbitrary nature of φ results in the attainment of
PLα(E,Ω)=PLα(Ω∖E,Ω) |
through the use of supremum.
Below we prove the coarea formula and the Sobolev inequality for Lα-perimeter.
Theorem 2.11. Let Ω1 be an open set defined in (1.3). If f∈BVLα(Ω1), then
|∇Lαf|(Ω1)≈∫+∞−∞PLα(Et,Ω1)dt, | (2.10) |
where Et={x∈Ω1:f(x)>t} for t∈R.
Proof. At first, assume
φ=(φ1,φ2,…,φd)∈C1c(Ω1,Rd). |
It is straightforward to prove that for i=1,2,…,d,
∫Ω1f(x)√xi∂∂xiφi(x)dμα(x)=∫+∞−∞(∫Et√xi∂∂xiφi(x)dμα(x))dt, |
and
∫Ω1f(x)αi+12−xi√xiφi(x)dμα(x)=∫+∞−∞(∫Etαi+12−xi√xiφi(x)dμα(x))dt, |
where the proof of [9, Section 5.5, Theorem 1] displays the latter. Therefore,
∫Ω1f(x)divLαφ(x)dμα(x)=∫+∞−∞(∫EtdivLαφ(x)dμα(x))dt. |
Therefore, we conclude that for all φ∈F(Ω1),
∫Ω1f(x)divLαφ(x)dμα(x)≤∫+∞−∞PLα(Et,Ω1)dt. |
Furthermore,
|∇Lαf|(Ω1)≤∫+∞−∞PLα(Et,Ω1)dt. |
Secondly, it can be assumed without any loss of generality that we simply need to confirm that
|∇Lαf|(Ω1)≥∫+∞−∞PLα(Et,Ω1)dt |
holds for f∈BVLα(Ω1)⋂C∞(Ω1). The idea of [15, Proposition 4.2] can be referenced in this proof. Denote by
m(t)=∫{x∈Ω1: f(x)≤t}|d∑i=1√xi∂∂xif(x)|dμα(x). |
Obviously,
∫+∞−∞m′(t)dt=∫Ω1|d∑i=1√xi∂∂xif(x)|dμα(x). |
Define the following function gh as
gh(s):={0,if s≤t,h(s−t),if t≤s≤t+1/h,1,if s≥t+1/h, |
where t∈R. Set the sequence vh(x):=gh(f(x)). At this time, vh→1Et in L1(Ω1,dμα). In fact,
∫Ω1|vh(x)−1Et|dμα(x)=∫{x∈Ω1:t<f(x)≤t+1/h}|gh(f(x))−1|dμα(x)≤∫{x∈Ω1:t<f(x)≤t+1/h}dμα(x)→0. |
As h→∞, {x∈Ω1:t<f(x)≤t+1/h}→∅, we then obtain
∫Ω1|∇Lαvh(x)|dμα(x)=∫{x∈Ω1:t<f(x)≤t+1/h}|∇Lα(h(f(x)−t))|dμα(x)+∫{x∈Ω1:f(x)≥t+1/h}|∇Lα1|dμα(x)=h∫{x∈Ω1:t<f(x)≤t+1/h}|d∑i=1√xi∂∂xif(x)|dμα(x). |
By utilizing Theorem 2.4 and taking the limit as h→∞ we can derive
|∇Lα1Et|(Ω1)≤limsuph→∞∫Ω1|∇Lαvh(x)|dμα(x)=hlimsuph→∞∫{x∈Ω1:t<f(x)≤t+1/h}|d∑i=1√xi∂∂xif(x)|dμα(x)=m′(t). | (2.11) |
Integrating (2.11) reaches
∫+∞−∞PLα(Et,Ω1)dt≤∫+∞−∞m′(t)dt=∫Ω1|d∑i=1√xi∂∂xif(x)|dμα(x)≲∫Ω1|∇Lαf(x)|dμα(x). |
Ultimately, through approximation and using the lower semicontinuity of the Lα-perimeter, we can deduce that (2.10) is valid for every f∈BVLα(Ω1).
We can eventually establish the Sobolev inequality and the isoperimetric inequality for Lα-BV functions. Since the domain Ω1 is a reasonable substitute of Ω, we can obtain the isoperimetric inequality and the Sobolev inequality for f∈BVLα(Ω1), where Ω1 is given in (1.3).
Theorem 2.12.
(i) (Sobolev inequality). Let Ω1 be an open set defined in (1.3). Then for all f∈BVLα(Ω1), we have
‖f‖Ldd−1(Ω1,dμα)≲|∇Lαf|(Ω1). | (2.12) |
(ii) (Isoperimetric inequality). Suppose that E is a bounded set having finite Lα-perimeter in Ω1. Then
μα(E)d−1d≲PLα(E,Ω1). | (2.13) |
(iii) The two statements mentioned above are equivalent.
Proof. (ⅰ) Let
fk∈C∞c(Ω1)∩BVLα(Ω1), k=1,2,…, |
such that
{fk→f in L1(Ω1,dμα),∫Ω1|∇Lαfk(x)|dμα(x)→∥∇Lαf∥(Ω1). |
Since Ω1=Ω∖{x∈Rd+:∃i∈1,⋯,d such that √xi<1}, then for any i=1,⋯,d, we obtain √xi≥1. It is easy to see that
|∇f(x)|≤|∇Lαf(x)|=(d∑i=1(√xi∂∂xif(x))2)12. | (2.14) |
After applying Fatou's lemma and the weighted Gagliardo-Nirenberg-Sobolev inequality, we get
‖f‖Ldd−1(Ω1,dμα)≤lim infk→∞‖fk‖Ldd−1(Ω1,dμα)≲limk→∞‖∇f‖L1(Ω1,dμα)≲limk→∞‖∇Lαf‖L1(Ω1,dμα)=|∇Lαf|(Ω1), |
where the relation between the gradient ∇ and the Laguerre gradient ∇Lα has been applied in (2.14).
(ⅱ) By setting f=1E in (2.12), it can be demonstrated that (2.13) is true.
(ⅲ) Apparently, the implication from (ⅰ) to (ⅱ) has been proved. The statement below demonstrates that (ⅱ) implies (ⅰ). Let 0≤f∈C∞c(Ω1). Applying the coarea formula from Theorem 2.11 and (ⅱ), we obtain
∫Ω1|∇Lαf(x)|dμα(x)=∫+∞0|∇Lα1Et|(Ω1)dt≳∫+∞0|Et|d−1ddt, |
where Et={x∈Ω1: f(x)>t}. Let
ft=min{t,f} & χ(t)=(∫Ω1fdd−1t(x)dμα(x))d−1d, ∀ t∈R. |
One can easily observe that
limt→∞χ(t)=(∫Ω1|f(x)|dd−1dμα(x))d−1d. |
Moreover, we can verify that χ(t) increases monotonically on (0,∞) and for any positive h,
0≤χ(t+h)−χ(t)≤(∫Ω1|ft+h(x)−ft(x)|dd−1dμα(x))d−1d≤h|Et|d−1d. |
Then χ(t) can be considered a Lipschitz function locally and χ′(t)≤|Et|d−1d for a.e. t∈(0,∞). Thus,
(∫Ω1|f(x)|dd−1dμα(x))d−1d=∫∞0χ′(t)dt≤∫∞0|Et|d−1ddt≲∫Ω1|∇Lαf(x)|dμα(x). |
Finally, Theorem 2.4 establishes the validity of (2.12) for all f∈BVLα(Ω1).
As a direct result of the proof of (ⅰ) in Theorem 2.12, we can get the following corollary.
Corollary 2.13. Let 1<p<d and let Ω1 be an open set defined in (1.3). For any f∈W1,1Lα(Ω1) one has
‖f‖Ldpd−p(Ω1,dμα)≲‖∇Lαf‖Lp(Ω1,dμα). | (2.15) |
Proof. For some γ>1 to be fixed later, via the Lemma 2.1 (ⅰ) and Hölder inequality we obtain
(∫Ω1|f(x)|γdd−1dμα(x))d−1d≲∫Ω1|f(x)|γ−1|∇Lαf(x)|dμα(x)≲(∫Ω1|f(x)|p(γ−1)p−1dμα(x))1−1p(∫Ω1|∇Lαf(x)|pdμα(x))1p. |
Choosing
γ=p(d−1)d−p |
and noting
γ−1=d(p−1)d−p, |
then we conclude that (2.15) holds true.
The main concern of this section is to determine if the mean curvature of every set with finite Lα-perimeter in Ω1⊆Rd+ belongs to L1(Ω1,dμα). To obtain comprehensive information on the classical case, kindly consult [13]. In order to prove Theorem 3.1, it is necessary to use the important result for the Laguerre perimeter in Corollary 2.8. Therefore, we assume that the dimension d≥3 via Remark 2.5.
For a given u∈L1(Ω1,dμα), the functional corresponding to the Lα-perimeter, known as Massari type, is given by
Fu,Lα(E):=PLα(E,Ω1)+∫Eu(x)dμα(x), |
where an arbitrary set of finite Lα-perimeter in Rd+ is denoted by E.
Theorem 3.1. For every set E⊂Rd+ that has finite Lα-perimeter, a function u belonging to L1(Rd+,dμα) exists such that
Fu,Lα(E)≤Fu,Lα(F) |
is satisfied for every set F⊂Ω1 with finite Lα-perimeter.
Proof. Initially, we must identify a function u∈L1(Ω1,dμα) for a specified set E such that
Fu,Lα(E)≤Fu,Lα(F) | (3.1) |
is true for every F with either F⊂E or E⊂F, then Theorem 3.1 is demonstrated, indicating that (3.1) applies to every F⊂Ω1. By including the inequality (3.1) that pertains to the test sets E∩F and E∪F, we have
{PLα(E,Ω1)+∫Eu(x)dμα(x)≤PLα(E∩F,Ω1)+∫E∩Fu(x)dμα(x),PLα(E,Ω1)+∫Eu(x)dμα(x)≤PLα(E∪F,Ω1)+∫E∪Fu(x)dμα(x). |
After taking that
PLα(E∩F,Ω1)+PLα(E∪F,Ω1)≤PLα(E,Ω1)+PLα(F,Ω1), | (3.2) |
we can get
2PLα(E,Ω1)+2∫Eu(x)dμα(x)≤PLα(E∩F,Ω1)+PLα(E∪F,Ω1)+∫E∩Fu(x)dμα(x)+∫E∪Fu(x)dμα(x)≤PLα(E,Ω1)+PLα(F,Ω1)+∫Eu(x)dμα(x)+∫Fu(x)dμα(x), |
that is, (3.1) holds for arbitrary F. Moreover, if (3.1) is vaild for a set F⊂E, then it is also applicable to the set F such that E⊂F, i.e. Ω1∖F⊂Ω1∖E,
PLα(E,Ω1)+∫Eu(x)dμα(x)=PLα(Ω1∖E,Ω1)+∫Ω1∖Eu(x)dμα(x)−∫Ω1∖Eu(x)dμα(x)+∫Eu(x)dμα(x)≤PLα(Ω1∖F,Ω1)+∫Ω1∖Fu(x)dμα(x)−∫Ω1∖Eu(x)dμα(x)+∫Eu(x)dμα(x)=PLα(F,Ω1)+∫Ω1∖Fu(x)dμα(x)−∫Ω1∖Eu(x)dμα(x)+∫Eu(x)dμα(x)=Fu,Lα(F)−∫Fu(x)dμα(x)+∫Ω1∖Fu(x)dμα(x)−∫Ω1∖Eu(x)dμα(x)+∫Eu(x)dμα(x)=Fu,Lα(F)+∫F∖Eu(x)dμα(x)−∫(Ω1∖E)/(Ω1∖F)u(x)dμα(x)=Fu,Lα(F), |
where we have utilized lemma 2.10 along with the property that u equals zero outside of the set E. Therefore, it is sufficient to prove that the integrability of u on E is established and that (3.1) is valid for every F⊂E.
Step I. Let h(⋅) be a measurable function on E such that h>0 and ∫Eh(x)dμα(x)<∞, and let Λ be a measure that is both positive and totally finite:
Λ(F)=∫Fh(x)dμα(x), F⊂E. |
Since Λ(F)=0 if and only if μα(F)=0 is clearly true. For λ>0 and F⊂E, we will examine the following functional
Fλ(F):=PLα(F,Ω1)+λΛ(E∖F). |
A commonly recognized fact is that any minimizing sequence is compact within L1loc(Ω1,dμα), and this functional is lower semi-continuous in regards to the same convergence. Thus, we can deduce that, for any positive value of λ, there is a solution Eλ to the problem:
Fλ(F)→min, F⊂E. |
Select a strictly increasing sequence of positive numbers {λi} that tend to ∞ and use Ei≡Eλi to refer to the associated solutions, so that ∀i≥1,
Fλi(Ei)≤Fλi(F), ∀ F⊂E. | (3.3) |
Given i<j. Let F=Ei∩Ej. It follows from (3.3) that
Fλi(Ei)≤Fλi(Ei∩Ej), |
that is,
PLα(Ei,Ω1)+λiΛ(E∖Ei)≤PLα(Ei∩Ej,Ω1)+λiΛ(E∖(Ei∩Ej)), |
this suggests
PLα(Ei,Ω1)+λi∫E∖Eih(x)dμα(x)≤PLα(Ei∩Ej,Ω1)+λi∫E∖(Ei∩Ej)h(x)dμα(x). |
A direct computation gives
PLα(Ei,Ω1)≤λi∫Ei∖Ejh(x)dμα(x)+PLα(Ei∩Ej,Ω1). |
Conversely, by choosing F=Ei∪Ej⊂E from (3.3), we can obtain Fλj(Ej)≤Fλj(Ei∪Ej). Hence,
PLα(Ej,Ω1)+λj∫E∖Ejh(x)dμα(x)≤PLα(Ei∪Ej,Ω1)+λj∫E∖(Ei∪Ej)h(x)dμα(x), |
equivalently,
PLα(Ej,Ω1)+λj∫Ei∖Ejh(x)dμα(x)≤PLα(Ei∪Ej,Ω1) |
which implies that
PLα(Ei,Ω1)+PLα(Ej,Ω1)+λj∫Ei∖Ejh(x)dμα(x)≤PLα(Ei∪Ej,Ω1)+λi∫Ei∖Ejh(x)dμα(x)+PLα(Ei∩Ej,Ω1). |
Remember that h is a positive number. The previous estimate, along with (3.2) and the condition λi<λj, suggests that
(λj−λi)Λ(Ei∖Ej)=(λj−λi)∫Ei∖Ejh(x)dμα(x)=0, |
i.e., Ei⊂Ej and the sequence of minimizers {Ei} is monotonically increasing. Conversely, by letting F=E, we get
PLα(Ei,Ω1)+λiΛ(E∖Ei)≤PLα(E,Ω1)+λiΛ(E∖E)=PLα(E,Ω1) ∀ i≥1, |
which infers that Ei converges to E in a monotonic manner and within L1loc(Rd+,dμα). Using Lemma 2.1 (ⅱ), we have
{PLα(E,Ω1)≤liminfi→∞PLα(Ei,Ω1)≤PLα(E,Ω1),PLα(E,Ω1)≤liminfi→∞PLα(Ei,Ω1)≤limsupi→∞PLα(Ei,Ω1)≤PLα(E), |
which means
PLα(E,Ω1)=limi→∞PLα(Ei,Ω1). | (3.4) |
Step II. Define λ0=0 and E0=∅, and let
u(x)={−λih(x), x∈Ei∖Ei−1, i≥1,0, otherwise. |
It is evident that u is negative almost everywhere on E, and
∫Rd+|u(x)|dμα(x)=∫∪∞i=0Ei+1∖Ei|u(x)|dμα(x)=∞∑i=0∫Ei+1∖Eiλi+1h(x)dμα(x)=∞∑i=0λi+1Λ(Ei+1∖Ei). |
In (3.3), taking F=Ei+1, we have
PLα(Ei,Ω1)+λiΛ(E∖Ei)≤PLα(Ei+1,Ω1)+λiΛ(E∖Ei+1), |
that is, for every i≥0,
λiΛ(Ei+1∖Ei)≤PLα(Ei+1,Ω1)−PLα(Ei,Ω1). |
For values of N that are large enough, we have
N∑i=0λiΛ(Ei+1∖Ei)≤N∑i=0[PLα(Ei+1,Ω1)−PLα(Ei,Ω1)]=PLα(EN,Ω1)−PLα(E0,Ω1)=PLα(EN,Ω1). |
Letting N→∞, (3.4) indicates that
∑∞i=0λiΛ(Ei+1∖Ei)≤PLα(E,Ω1). |
Let's assume an additional condition that 0<λi+1−λi≤c, i≥0, where c is a constant that doesn't depend on i, we can say that for any N>0,
N∑i=0(λi+1−λi)Λ(Ei+1∖Ei)≤cN∑i=0Λ(Ei+1∖Ei)=cN∑i=0∫Ei+1∖Eih(x)dμα(x)=c∫∪Ni=0(Ei+1∖Ei)h(x)dμα(x), |
which gives
∞∑i=0(λi+1−λi)Λ(Ei+1∖Ei)≤cΛ(E). |
Then
∫Rd+|u(x)|dμα(x)=∞∑i=0λi+1Λ(Ei+1∖Ei)=∞∑i=0(λi+1−λi)Λ(Ei+1∖Ei)+∞∑i=0λiΛ(Ei+1∖Ei)≤cΛ(E)+PLα(E,Ω1)<∞. |
In conclusion, u∈L1(Rd+,dμα).
Step III. We contend that the inequality
PLα(Ei,Ω1)≤PLα(F,Ω1)+∑ij=1λjΛ((Ej∖Ej−1)∖F) | (3.5) |
is vaild for all F⊂E and every i≥1.
If i=1, then Ei−1=E0=∅. Substituting this into (3.5) yields
PLα(E1,Ω1)≤PLα(F,Ω1)+λ1Λ(E1∖F), |
which coincides with (3.3) for i=1.
Now we assume that (3.5) holds for a fixed i≥1 and every F⊂E. Take F∩Ei as a test set. Observe that {Ej} is increasing. It is evidently clear to show that
(Ej∖Ej−1)∖(F∩Ei)=(Ej∖Ej−1)∖F. |
Then
PLα(Ei,Ω1)≤PLα(F∩Ei,Ω1)+i∑j=1λjΛ((Ej∖Ej−1)∖(F∩Ei))=PLα(F∩Ei,Ω1)+i∑j=1λjΛ((Ej∖Ej−1)∖F). |
Conversely, Fλi+1 is minimized by Ei+1. Hence,
Fλi+1(Ei+1)≤Fλi+1(F∪Ei), |
and noticing that
E∖Ei=(E∖Ei+1)∪(Ei+1∖Ei), |
it is possible for us to obtain
E∖(F∪Ei)=((E∖Ei+1)∖F)∪((Ei+1∖Ei)∖F). |
This deduces
PLα(Ei+1,Ω1)+λi+1Λ(E∖Ei+1)≤PLα(F∪Ei,Ω1)+λi+1Λ(E∖(F∪Ei))≤PLα(F∪Ei,Ω1)+λi+1Λ((E∖Ei+1)∖F)+λi+1Λ((Ei+1∖Ei)∖F). |
Therefore, we obtain that
PLα(Ei,Ω1)+PLα(Ei+1,Ω1)+λi+1Λ(E∖Ei+1)≤PLα(F∩Ei,Ω1)+i∑j=1λjΛ((Ej∖Ej−1)∖F)+PLα(F∪Ei,Ω1)+λi+1Λ((E∖Ei+1)∖F)+λi+1Λ((Ei+1∖Ei)∖F)≤PLα(Ei,Ω1)+PLα(F,Ω1)+i+1∑j=1λjΛ((Ej∖Ej−1)∖F)+λi+1Λ((E∖Ei+1)∖F)≤PLα(Ei,Ω1)+PLα(F,Ω1)+i+1∑j=1λjΛ((Ej∖Ej−1)∖F)+λi+1Λ(E∖Ei+1), |
i.e., (3.5) is true for i+1. Last but not least,
PLα(E,Ω1)=limi→∞PLα(Ei,Ω1)≤PLα(F,Ω1)+limi→∞i∑j=1λjΛ((Ej∖Ej−1)∖F)=PLα(F,Ω1)−∫∪∞j=0(Ej∖Ej−1)∖Fu(x)dμα(x)=PLα(F,Ω1)−∫E∖Fu(x)dμα(x), |
which gives (3.3).
This work was supported by National Natural Science Foundation of China (No. 11671031, No. 12271042) and Beijing Natural Science Foundation of China (No. 1232023).
The authors declare there is no conflict of interest.
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