Loading [MathJax]/jax/output/SVG/jax.js
Research article Special Issues

Laguerre BV spaces, Laguerre perimeter and their applications

  • 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

    Related Papers:

    [1] Siegfried Carl . Quasilinear parabolic variational-hemivariational inequalities in RN×(0,τ) under bilateral constraints. Communications in Analysis and Mechanics, 2025, 17(1): 41-60. doi: 10.3934/cam.2025003
    [2] Lovelesh Sharma . Brezis Nirenberg type results for local non-local problems under mixed boundary conditions. Communications in Analysis and Mechanics, 2024, 16(4): 872-895. doi: 10.3934/cam.2024038
    [3] Jizheng Huang, Shuangshuang Ying . Hardy-Sobolev spaces of higher order associated to Hermite operator. Communications in Analysis and Mechanics, 2024, 16(4): 858-871. doi: 10.3934/cam.2024037
    [4] Heng Yang, Jiang Zhou . Some estimates of multilinear operators on tent spaces. Communications in Analysis and Mechanics, 2024, 16(4): 700-716. doi: 10.3934/cam.2024031
    [5] Xiaotian Hao, Lingzhong Zeng . Eigenvalues of the bi-Xin-Laplacian on complete Riemannian manifolds. Communications in Analysis and Mechanics, 2023, 15(2): 162-176. doi: 10.3934/cam.2023009
    [6] Panyu Deng, Jun Zheng, Guchuan Zhu . Well-posedness and stability for a nonlinear Euler-Bernoulli beam equation. Communications in Analysis and Mechanics, 2024, 16(1): 193-216. doi: 10.3934/cam.2024009
    [7] Xiulan Wu, Yaxin Zhao, Xiaoxin Yang . On a singular parabolic p-Laplacian equation with logarithmic nonlinearity. Communications in Analysis and Mechanics, 2024, 16(3): 528-553. doi: 10.3934/cam.2024025
    [8] Ming Liu, Binhua Feng . Grand weighted variable Herz-Morrey spaces estimate for some operators. Communications in Analysis and Mechanics, 2025, 17(1): 290-316. doi: 10.3934/cam.2025012
    [9] Shaoqiang Shang . Characterizations of ball-covering of separable Banach space and application. Communications in Analysis and Mechanics, 2023, 15(4): 831-846. doi: 10.3934/cam.2023040
    [10] Zhiyong Wang, Kai Zhao, Pengtao Li, Yu Liu . Boundedness of square functions related with fractional Schrödinger semigroups on stratified Lie groups. Communications in Analysis and Mechanics, 2023, 15(3): 410-435. doi: 10.3934/cam.2023020
  • 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=di=1[xi2xi2+(αi+1xi)xi].

    Let the probabilistic gamma measure μα in Rd+=(0,)d be defined as

    dμα(x)=di=1xiαiexiΓ(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=xixi,

    see [7] or [8]. The operator Lα has the following decomposition:

    Lα=di=1δiδi,

    where

    δi=xi(xi+αi+12xixi)

    is the formal adjoint of δi in L2(Rd+,dμα). Throughout this paper, suppose that ΩRd+ be an open set. For uC1(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:=δ1φ1+δ2φ2++δdφd,

    which also gives

    Lαu=divLα(Lαu)=di=1[xi2xi2+(αi+1xi)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 Cc-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 ERd is defined as

    P(E)=supφF(Rd){Edivφ(x)dx},

    here let F(Rd) be the set that contains all functions

    φ=(φ1,,φd)C1c(Rd,Rd)

    satisfying

    φ=supxE{(|φ1(x)|2++|φd(x)|2)12}1.

    As we all know that

    P(E)=P(Ec), ERd (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

    fLdd1(Ω1,dμα)|Lαf|(Ω1) (1.2)

    shares equivalence with the Sobolev type inequality

    μα(E)d1dPLα(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{xRd+:i1,,d such that xi<1} (1.3)

    of Ω which is a reasonable substitute of Ω and whose figure is given as follows:

    Figure 1.  Set for the Sobolev inequality in the Laguerre setting on R2+.

    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; AB means that 1CABCA and the notation XY is used to indicate that XCY with a positive constant C independent of significant quantities. Similarly, one writes XY for XCY.

    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 fL1(Ω,dμα) is defined by

    |Lαf|(Ω)=supφF(Ω){Ωf(x)divLαφ(x)dμα(x)},

    where F(Ω) denotes the class of all functions

    φ=(φ1,φ2,,φd)C1c(Ω,Rd)

    satisfying

    φL=supxΩ{(|φ1(x)|2++|φd(x)|2)12}1.

    We say that an function fL1(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

    fBVLα(Ω)=fL1(Ω,dμα)+|Lαf|(Ω).

    Definition 2.1. Suppose Ω is an open set in Rd+. Let 1p. The Sobolev space Wk,pLα(Ω) associated with Lα is defined as the set of all functions fLp(Ω,dμα) such that

    δj1δjmfLp(Ω,dμα), 1j1,,jmd, 1mk.

    The norm of fWk,pLα(Ω) is given by

    fWk,pLα:=1j1jmd, 1mkδj1δjmfLp(Ω,dμα)+fLp(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 fW1,1Lα(Ω), then

    |Lαf|(Ω)=Ω|Lαf(x)|dμα(x),

    which implies W1,1Lα(Ω)BVLα(Ω).

    (ii) (Lower semicontinuity). Suppose fkBVLα(Ω), kN and fkf 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 fBVLα(Ω). Then there exists a Radon measure μLα on Ω such that

    Ωf(x)divLαφ(x)dμα(x)=Ωφ(x)dμLα(x)

    for every φCc(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 uBVLα(Ω1), then there exists a sequence {uh}hNBVLα(Ω1)C(Ω1) such that

    limhuhuL1(Ω1,dμα)=0

    and

    limhΩ1|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 uεC(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:={xΩ1:dist(x,Ω1)>1m+j}B(0,m+j), jN,

    where dist(x,Ω1)=inf{|xy|:yΩ1}. Note that Ω1,jΩ1,j+1Ω1, jN and j=0Ω1,j=Ω1. Since |Lαu|() is a measure, then choose a value mN to be sufficiently large such that

    |Lαu|(Ω1Ω1,0)<ε. (2.1)

    Set U0:=Ω1,0 and Uj:=Ω1,j+1¯Ω1,j1 for j1. 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}jN. Namely, there exist functions {fj}jNCc(Uj) such that 0fj1, j0 and j=0fj=1 on Ω1. Thus we have the fact that

    j=0Lαfj=(x1x1(j=0fj),x2x2(j=0fj),,xdxd(j=0fj))=0 (2.2)

    on Ω1. Given ε>0 and uL1(Ω1,R), extended to zero out of Ω1, the regularization can be defined as

    uε(x):=1εdB(x,ε)η(xyε)u(y)dμα(y),

    where ηCc(Rd+) is a nonnegative radial function satisfying

    1ϵdjRd+η(xyϵj)dμα(x)=1,  jN,

    and supp ηB(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|(uLαfj)εj(x)uLαfj(x)|dμα(x)<ε2(j+1). (2.3)

    Construct

    vε(x):=j=0(ufj)εj(x).

    In some neighborhood of each point xΩ1, there are only finitely many nonzero terms in this sum, hence vεC(Ω1) and u=j=0ufj. Therefore, by a simple computation, we obtain

    vεuL1(Ω1,dμα)j=0Ω1|(fju)εj(x)fj(x)u(x)|dμα(x)<ε.

    Consequently,

    vεu  in  L1(Ω1,dμα)  as  ε0.

    Now, assume φC1c(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=0Ω1(ufj)εj(x)(δ1φ1(x)+δ2φ2(x)++δdφd(x))dμα(x):=I+II,

    where

    {I:=j=0Ω1(ufj)εj(x)(x1x1φ1(x)++xdxdφd(x))dμα(x),II:=j=0Ω1(ufj)εj(x)(α1+12x1x1φ1(x)++αd+12xdxdφd(x))dμα(x).

    For the sake of research, let

    ~divLαφ=δ1φ1+δ2φ2++δdφd. (2.4)

    As for I, we obtain

    I=j=0Ω1(ufj)εj(x)~divLαφ(x)dμα(x)=j=0Ω1(ufj)(y)~divLα(ηεjφ(y))dμα(y)=j=0Ω1u(y)~divLα(fj(ηεjφ))(y)dμα(y)+j=0Ω1u(y)Lαfj(ηεjφ)(y)dμα(y)=j=0Ω1u(y)~divLα(fj(ηεjφ))(y)dμα(y)j=0Ω1φ(y)(ηεj(uLαfj)(y)uLαfj(y))dμα(y):=I1+I2,

    where in the last equality we have used the fact (2.2). In fact, when φL1, then |fj(ηεjφ)(x)|1, jN, 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=0Ω1(ufj)εj(x)(α1+12x1x1φ1(x)++αd+12xdxdφd(x))dμα(x)=j=0Ω1Ω11εdjη(xyεj)u(y)fj(y)(dk=1αk+12ykykφk(x))dμα(y)dμα(x)j=0Ω1Ω11εdjη(xyεj)u(y)fj(y)×(dk=1(αk+12xkxkαk+12ykyk)φk(x))dμα(y)dμα(x)=j=0Ω1u(y)fj(y)((dk=1αk+12ykykφk)ηεj(y))dμα(y)j=0Ω1Ω11εdjη(xyεj)u(y)fj(y)×(dk=1(αk+12xkxkαk+12ykyk)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=0Ω1u(y)~div(fj(ηεjφ))(y)dμα(y)j=0Ω1u(y)fj(y)(dk=1αk+12ykyk(φkηεj(y)))dμα(y)|

    and

    J2:=|j=0Ω1Ω11εdjη(xyεj)u(y)fj(y)×(dk=1(αk+12xkxkαk+12ykyk)φk(x))dμα(y)dμα(x)|.

    Furthermore,

    J1=|j=0Ω1u(y)~divLα(fj(ηεjφ))(y)dμα(y)j=0Ω1u(y)fj(y)(dk=1αk+12ykykφkηεj(y))dμα(y)||Ω1u(y)~divLα(f0(ηε0φ))(y)dμα(y)Ω1u(y)f0(y)(dk=1αk+12ykykφkηε0(y))dμα(y)|+|j=1Ω1u(y)~divLα(fj(ηεjφ))(y)dμα(y)j=1Ω1u(y)fj(y)(dk=1αk+12ykykφkηεj(y))dμα(y)||Lαu|(Ω1)+j=1|Lαu|(Uj)|Lαu|(Ω1)+|Lαu|(Ω1Ω1,0)|Lαu|(Ω1)+3ε,

    where we applied the fact (2.1) in the final inequality. Note that ψ(xk)=αk+12xkxk, φL1 and supp ηB(0,1)Rd+. Assuming |xkyk|<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(xkyk))32+12(yk+θ(xkyk))12||xkyk|(|αk+12|2|yk+θ(xkyk)|32+12|yk+θ(xkyk)|12)|xkyk|.

    Consequently, we obtain

    J2=|j=0Ω1Ω11εdjη(xyεj)u(y)fj(y)(dk=1(αk+12xkxkαk+12ykyk)φk(x))×dμα(y)dμα(x)|εj2j=0Ω1Ω1|1εdjη(xyεj)u(y)fj(y)|dk=1|αk+12||yk+θ(xyk)|32×|φk(x)|dμα(y)dμα(x)+εj2j=0Ω1Ω1|1εdjη(xyεj)u(y)fj(y)|dk=1|yk+θ(xkyk)|12×|φk(x)|dμα(y)dμα(x)Cεjj=0Ω1Ω1|1εdjη(xyεj)u(y)fj(y)|dk=1|αk+12||yk|32dμα(y)dμα(x)+Cεjj=0Ω1Ω1|1εdjη(xyεj)u(y)fj(y)|dk=1|yk|12dμα(y)dμα(x)Cεjj=0Ω1Ω1|1εdjη(xyεj)|dμα(x)dk=1|αk+12||u(y)||fj(y)||yk|32dμα(y)+Cεjj=0Ω1Ω1|1εdjη(xyεj)|dμα(x)dk=1|u(y)||fj(y)||yk|12dμα(y)CεjRd+|1ϵdjη(xyϵj)|dμα(x)dk=1Ω1|αk+12||u(y)||j=0fj(y)||yk|32dμα(y)+CεjRd+|1ϵdjη(xyϵj)|dμα(x)dk=1Ω1|u(y)||j=0fj(y)||yk|12dμα(y)=CεjΩ1|u(y)|dk=1|αk+12||yk|32dμα(y)+CεjΩ1|u(y)|dk=1|yk|12dμα(y)ε,

    where we have used the facts that

    {Ω1|u(y)|dk=1|yk|12dμα(y)<,Ω1|u(y)|dk=1|αk+12||yk|32dμα(y)<, (2.5)

    and in the third inequality we have used the fact that

    |yk+θ(xkyk)||yk|θ|xkyk|=(1θ2)|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 uBVLα(Ω) satisfies (2.5) in Theorem 2.4 when d3, at this time, Theorem 2.4 is valid for any open set ΩRd.

    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,vL1(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,vhBVLα(Ω1)Cc(Ω1),  h=1,2,...,

    such that

    {uhu,vhv  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)liminfhΩ1|Lαmax{uh,vh}|dμα(x)+liminfhΩ1|Lαmin{uh,vh}|dμα(x)liminfh(Ω1|Lαmax{uh,vh}|dμα(x)+Ω1|Lαmin{uh,vh}|dμα(x))liminfh({xΩ1:uhvh}|Lαvh|dμα(x)+{xΩ1:uh>vh}|Lαuh|dμα(x)+{xΩ1:uhvh}|Lαuh|dμα(x)+{xΩ1:uh>vh}|Lαvh|dμα(x))=liminfhΩ1|Lαuh(x)|dμα(x)+liminfhΩ1|Lαvh(x)|dμα(x)limhΩ1|Lαuh(x)|dμα(x)+limhΩ1|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 EΩ as follows:

    PLα(E,Ω)=|Lα1E|(Ω)=supφF(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 1Ek1E in L1loc(Ω,dμα), where E and Ek, kN, are subsets of Ω, then

    PLα(E,Ω)liminfkPLα(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(EF,Ω1)+PLα(EF,Ω1)PLα(E,Ω1)+PLα(F,Ω1), (2.7)

    where Ω1 is an open set defined in (1.3). Especially, if PLα(E(EF),Ω1)PLα(F(FE),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(EF),Ω1)PLα(F(EF),Ω1)=0 leads to PLα(E(EF),Ω1)=0 or PLα(F(EF),Ω1)=0. Suppose PLα(E(EF),Ω1)=0. By (2.7), we have

    PLα(E,Ω1)=PLα((E(EF))(EF),Ω1)PLα(E(EF),Ω1)+PLα(EF,Ω1)=PLα(EF,Ω1). (2.8)

    Via (2.6) and EF=F(E(EF)), we have

    PLα(F,Ω1)=supφF(Ω1){FdivLαφ(x)dμα(x)}=supφF(Ω1){EFdivLαφ(x)dμα(x)E(EF)divLαφ(x)dμα(x)}supφF(Ω1){EFdivLαφ(x)dμα(x)}+supφF(Ω1){E(EF)divLαφ(x)dμα(x)}=PLα(EF,Ω1)+PLα(E(EF),Ω1)=PLα(EF,Ω1). (2.9)

    Combining (2.8) with (2.9) deduces that

    PLα(E,Ω1)+PLα(F,Ω1)PLα(EF,Ω1)+PLα(EF,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 EΩ be subset with finite Lα-perimeter. Then we have

    E~divLαφ(x)dμα(x)=Ec(x1φ1(x),,xdφd(x))nω(x)dHd1(x)Edi=1αi+12xixiφi(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(di=1xixiφi(x))ω(x)dx=Ediv(x1φ1(x)ω(x),,xdφd(x)ω(x))dxEdi=1xiφi(x)xiω(x)dx12Edi=11xiφi(x)ω(x)dx=Ec(x1φ1(x),,xdφd(x))nω(x)dHd1(x)Edi=1xiφi(x)xiω(x)dx12Edi=11xiφi(x)ω(x)dx=Ec(x1φ1(x),,xdφd(x))nω(x)dHd1(x)Edi=1αi+12xixiφi(x)ω(x)dx,

    where we have used the classical Gauss-Green formula and the following facts regarding the derivatives of ω(x):

    xi(dj=1xjαjexjΓ(αj+1))=dj=1,jixjαjexjΓ(αj+1)1Γ(αi+1)(exixiαi+αiexixiαi1)=(1+αixi)ω(x)

    for 1id. This completes the proof.

    Lemma 2.10. If a set E is in Ω and has finite Lα-perimeter, then

    PLα(E,Ω)=PLα(ΩE,Ω).

    Proof. For any φF(Rd+), since PLα(E,Ω)<, then

    supφF(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)Edk=1αi+12xixiφi(x)dμα(x)=Ec(x1φ1(x),,xdφd(x))nω(x)dHd1(x)+Edk=1αi+12xixiφi(x)dμα(x)Edk=1αi+12xixiφi(x)dμα(x)=E(x1φ1(x),,xdφd(x))nω(x)dHd1(x)=Ec~divLαφ(x)dμα(x)Ecdk=1αi+12xixiφi(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(ΩE,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 fBVLα(Ω1), then

    |Lαf|(Ω1)+PLα(Et,Ω1)dt, (2.10)

    where Et={xΩ1:f(x)>t} for tR.

    Proof. At first, assume

    φ=(φ1,φ2,,φd)C1c(Ω1,Rd).

    It is straightforward to prove that for i=1,2,,d,

    Ω1f(x)xixiφi(x)dμα(x)=+(Etxixiφi(x)dμα(x))dt,

    and

    Ω1f(x)αi+12xixiφi(x)dμα(x)=+(Etαi+12xixiφi(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 φF(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 fBVLα(Ω1)C(Ω1). The idea of [15, Proposition 4.2] can be referenced in this proof. Denote by

    m(t)={xΩ1: f(x)t}|di=1xixif(x)|dμα(x).

    Obviously,

    +m(t)dt=Ω1|di=1xixif(x)|dμα(x).

    Define the following function gh as

    gh(s):={0,if st,h(st),if tst+1/h,1,if st+1/h,

    where tR. Set the sequence vh(x):=gh(f(x)). At this time, vh1Et in L1(Ω1,dμα). In fact,

    Ω1|vh(x)1Et|dμα(x)={xΩ1:t<f(x)t+1/h}|gh(f(x))1|dμα(x){xΩ1:t<f(x)t+1/h}dμα(x)0.

    As h, {xΩ1:t<f(x)t+1/h}, we then obtain

    Ω1|Lαvh(x)|dμα(x)={xΩ1:t<f(x)t+1/h}|Lα(h(f(x)t))|dμα(x)+{xΩ1:f(x)t+1/h}|Lα1|dμα(x)=h{xΩ1:t<f(x)t+1/h}|di=1xixif(x)|dμα(x).

    By utilizing Theorem 2.4 and taking the limit as h we can derive

    |Lα1Et|(Ω1)limsuphΩ1|Lαvh(x)|dμα(x)=hlimsuph{xΩ1:t<f(x)t+1/h}|di=1xixif(x)|dμα(x)=m(t). (2.11)

    Integrating (2.11) reaches

    +PLα(Et,Ω1)dt+m(t)dt=Ω1|di=1xixif(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 fBVLα(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 fBVLα(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 fBVLα(Ω1), we have

    fLdd1(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)d1dPLα(E,Ω1). (2.13)

    (iii) The two statements mentioned above are equivalent.

    Proof. (ⅰ) Let

    fkCc(Ω1)BVLα(Ω1), k=1,2,,

    such that

    {fkf in L1(Ω1,dμα),Ω1|Lαfk(x)|dμα(x)→∥Lαf(Ω1).

    Since Ω1=Ω{xRd+:i1,,d such that xi<1}, then for any i=1,,d, we obtain xi1. It is easy to see that

    |f(x)||Lαf(x)|=(di=1(xixif(x))2)12. (2.14)

    After applying Fatou's lemma and the weighted Gagliardo-Nirenberg-Sobolev inequality, we get

    fLdd1(Ω1,dμα)lim infkfkLdd1(Ω1,dμα)limkfL1(Ω1,dμα)limkLαfL1(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 0fCc(Ω1). Applying the coarea formula from Theorem 2.11 and (ⅱ), we obtain

    Ω1|Lαf(x)|dμα(x)=+0|Lα1Et|(Ω1)dt+0|Et|d1ddt,

    where Et={xΩ1: f(x)>t}. Let

    ft=min{t,f}  &  χ(t)=(Ω1fdd1t(x)dμα(x))d1d,  tR.

    One can easily observe that

    limtχ(t)=(Ω1|f(x)|dd1dμα(x))d1d.

    Moreover, we can verify that χ(t) increases monotonically on (0,) and for any positive h,

    0χ(t+h)χ(t)(Ω1|ft+h(x)ft(x)|dd1dμα(x))d1dh|Et|d1d.

    Then χ(t) can be considered a Lipschitz function locally and χ(t)|Et|d1d for a.e. t(0,). Thus,

    (Ω1|f(x)|dd1dμα(x))d1d=0χ(t)dt0|Et|d1ddtΩ1|Lαf(x)|dμα(x).

    Finally, Theorem 2.4 establishes the validity of (2.12) for all fBVLα(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 fW1,1Lα(Ω1) one has

    fLdpdp(Ω1,dμα)LαfLp(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)|γdd1dμα(x))d1dΩ1|f(x)|γ1|Lαf(x)|dμα(x)(Ω1|f(x)|p(γ1)p1dμα(x))11p(Ω1|Lαf(x)|pdμα(x))1p.

    Choosing

    γ=p(d1)dp

    and noting

    γ1=d(p1)dp,

    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 Ω1Rd+ 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 d3 via Remark 2.5.

    For a given uL1(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 ERd+ 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 FΩ1 with finite Lα-perimeter.

    Proof. Initially, we must identify a function uL1(Ω1,dμα) for a specified set E such that

    Fu,Lα(E)Fu,Lα(F) (3.1)

    is true for every F with either FE or EF, then Theorem 3.1 is demonstrated, indicating that (3.1) applies to every FΩ1. By including the inequality (3.1) that pertains to the test sets EF and EF, we have

    {PLα(E,Ω1)+Eu(x)dμα(x)PLα(EF,Ω1)+EFu(x)dμα(x),PLα(E,Ω1)+Eu(x)dμα(x)PLα(EF,Ω1)+EFu(x)dμα(x).

    After taking that

    PLα(EF,Ω1)+PLα(EF,Ω1)PLα(E,Ω1)+PLα(F,Ω1), (3.2)

    we can get

    2PLα(E,Ω1)+2Eu(x)dμα(x)PLα(EF,Ω1)+PLα(EF,Ω1)+EFu(x)dμα(x)+EFu(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 FE, then it is also applicable to the set F such that EF, i.e. Ω1FΩ1E,

    PLα(E,Ω1)+Eu(x)dμα(x)=PLα(Ω1E,Ω1)+Ω1Eu(x)dμα(x)Ω1Eu(x)dμα(x)+Eu(x)dμα(x)PLα(Ω1F,Ω1)+Ω1Fu(x)dμα(x)Ω1Eu(x)dμα(x)+Eu(x)dμα(x)=PLα(F,Ω1)+Ω1Fu(x)dμα(x)Ω1Eu(x)dμα(x)+Eu(x)dμα(x)=Fu,Lα(F)Fu(x)dμα(x)+Ω1Fu(x)dμα(x)Ω1Eu(x)dμα(x)+Eu(x)dμα(x)=Fu,Lα(F)+FEu(x)dμα(x)(Ω1E)/(Ω1F)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 FE.

    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), FE.

    Since Λ(F)=0 if and only if μα(F)=0 is clearly true. For λ>0 and FE, we will examine the following functional

    Fλ(F):=PLα(F,Ω1)+λΛ(EF).

    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, FE.

    Select a strictly increasing sequence of positive numbers {λi} that tend to and use EiEλi to refer to the associated solutions, so that i1,

    Fλi(Ei)Fλi(F),  FE. (3.3)

    Given i<j. Let F=EiEj. It follows from (3.3) that

    Fλi(Ei)Fλi(EiEj),

    that is,

    PLα(Ei,Ω1)+λiΛ(EEi)PLα(EiEj,Ω1)+λiΛ(E(EiEj)),

    this suggests

    PLα(Ei,Ω1)+λiEEih(x)dμα(x)PLα(EiEj,Ω1)+λiE(EiEj)h(x)dμα(x).

    A direct computation gives

    PLα(Ei,Ω1)λiEiEjh(x)dμα(x)+PLα(EiEj,Ω1).

    Conversely, by choosing F=EiEjE from (3.3), we can obtain Fλj(Ej)Fλj(EiEj). Hence,

    PLα(Ej,Ω1)+λjEEjh(x)dμα(x)PLα(EiEj,Ω1)+λjE(EiEj)h(x)dμα(x),

    equivalently,

    PLα(Ej,Ω1)+λjEiEjh(x)dμα(x)PLα(EiEj,Ω1)

    which implies that

    PLα(Ei,Ω1)+PLα(Ej,Ω1)+λjEiEjh(x)dμα(x)PLα(EiEj,Ω1)+λiEiEjh(x)dμα(x)+PLα(EiEj,Ω1).

    Remember that h is a positive number. The previous estimate, along with (3.2) and the condition λi<λj, suggests that

    (λjλi)Λ(EiEj)=(λjλi)EiEjh(x)dμα(x)=0,

    i.e., EiEj and the sequence of minimizers {Ei} is monotonically increasing. Conversely, by letting F=E, we get

    PLα(Ei,Ω1)+λiΛ(EEi)PLα(E,Ω1)+λiΛ(EE)=PLα(E,Ω1)   i1,

    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)liminfiPLα(Ei,Ω1)PLα(E,Ω1),PLα(E,Ω1)liminfiPLα(Ei,Ω1)limsupiPLα(Ei,Ω1)PLα(E),

    which means

    PLα(E,Ω1)=limiPLα(Ei,Ω1). (3.4)

    Step II. Define λ0=0 and E0=, and let

    u(x)={λih(x), xEiEi1, i1,0, otherwise.

    It is evident that u is negative almost everywhere on E, and

    Rd+|u(x)|dμα(x)=i=0Ei+1Ei|u(x)|dμα(x)=i=0Ei+1Eiλi+1h(x)dμα(x)=i=0λi+1Λ(Ei+1Ei).

    In (3.3), taking F=Ei+1, we have

    PLα(Ei,Ω1)+λiΛ(EEi)PLα(Ei+1,Ω1)+λiΛ(EEi+1),

    that is, for every i0,

    λiΛ(Ei+1Ei)PLα(Ei+1,Ω1)PLα(Ei,Ω1).

    For values of N that are large enough, we have

    Ni=0λiΛ(Ei+1Ei)Ni=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+1Ei)PLα(E,Ω1).

    Let's assume an additional condition that 0<λi+1λic, i0, where c is a constant that doesn't depend on i, we can say that for any N>0,

    Ni=0(λi+1λi)Λ(Ei+1Ei)cNi=0Λ(Ei+1Ei)=cNi=0Ei+1Eih(x)dμα(x)=cNi=0(Ei+1Ei)h(x)dμα(x),

    which gives

    i=0(λi+1λi)Λ(Ei+1Ei)cΛ(E).

    Then

    Rd+|u(x)|dμα(x)=i=0λi+1Λ(Ei+1Ei)=i=0(λi+1λi)Λ(Ei+1Ei)+i=0λiΛ(Ei+1Ei)cΛ(E)+PLα(E,Ω1)<.

    In conclusion, uL1(Rd+,dμα).

    Step III. We contend that the inequality

    PLα(Ei,Ω1)PLα(F,Ω1)+ij=1λjΛ((EjEj1)F) (3.5)

    is vaild for all FE and every i1.

    If i=1, then Ei1=E0=. Substituting this into (3.5) yields

    PLα(E1,Ω1)PLα(F,Ω1)+λ1Λ(E1F),

    which coincides with (3.3) for i=1.

    Now we assume that (3.5) holds for a fixed i1 and every FE. Take FEi as a test set. Observe that {Ej} is increasing. It is evidently clear to show that

    (EjEj1)(FEi)=(EjEj1)F.

    Then

    PLα(Ei,Ω1)PLα(FEi,Ω1)+ij=1λjΛ((EjEj1)(FEi))=PLα(FEi,Ω1)+ij=1λjΛ((EjEj1)F).

    Conversely, Fλi+1 is minimized by Ei+1. Hence,

    Fλi+1(Ei+1)Fλi+1(FEi),

    and noticing that

    EEi=(EEi+1)(Ei+1Ei),

    it is possible for us to obtain

    E(FEi)=((EEi+1)F)((Ei+1Ei)F).

    This deduces

    PLα(Ei+1,Ω1)+λi+1Λ(EEi+1)PLα(FEi,Ω1)+λi+1Λ(E(FEi))PLα(FEi,Ω1)+λi+1Λ((EEi+1)F)+λi+1Λ((Ei+1Ei)F).

    Therefore, we obtain that

    PLα(Ei,Ω1)+PLα(Ei+1,Ω1)+λi+1Λ(EEi+1)PLα(FEi,Ω1)+ij=1λjΛ((EjEj1)F)+PLα(FEi,Ω1)+λi+1Λ((EEi+1)F)+λi+1Λ((Ei+1Ei)F)PLα(Ei,Ω1)+PLα(F,Ω1)+i+1j=1λjΛ((EjEj1)F)+λi+1Λ((EEi+1)F)PLα(Ei,Ω1)+PLα(F,Ω1)+i+1j=1λjΛ((EjEj1)F)+λi+1Λ(EEi+1),

    i.e., (3.5) is true for i+1. Last but not least,

    PLα(E,Ω1)=limiPLα(Ei,Ω1)PLα(F,Ω1)+limiij=1λjΛ((EjEj1)F)=PLα(F,Ω1)j=0(EjEj1)Fu(x)dμα(x)=PLα(F,Ω1)EFu(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.



    [1] E. De Giorgi, Su alcune generalizzazioni della nozione di perimetro, in Equazioni differenziali e calcolo delle variazioni, Quaderni UMI (1992), 237–250.
    [2] J. Huang, P. Li, Y. Liu, Capacity & perimeter from α-Hermite bounded variation, Calc. Var. Partial Differential Equations, 59 (2020), 186. https://doi.org/10.1007/s00526-020-01851-0 doi: 10.1007/s00526-020-01851-0
    [3] P. Alonso-Ruiz, F. Baudoin, L. Chen, L. G. Rogers, N. Shanmugalingam, A. Teplyaev, Besov class via heat semigroup on Dirichlet spaces Ⅱ: BV functions and Gaussian heat kernel estimates, Calc. Var. Partial Differential Equations, 59 (2020), 1–32. https://doi.org/10.1007/s00526-020-01750-4 doi: 10.1007/s00526-020-01750-4
    [4] G. Da Prato, A. Lunardi, BV functions in Hilbert spaces, Math. Ann., 381 (2021), 1653–1722. https://doi.org/10.1007/s00208-020-02037-x doi: 10.1007/s00208-020-02037-x
    [5] J. Huang, P. Li, Y. Liu, Gaussian BV functions and gaussian BV capacity on stratified groups, Anal. Theory Appl., 37 (2021), 311–329. https://doi.org/10.4208/ata.2021.lu80.03 doi: 10.4208/ata.2021.lu80.03
    [6] P. Lahti, The variational 1-capacity and BV functions with zero boundary values on doubling metric spaces, Adv. Calc. Var., 14 (2021), 171–192. https://doi.org/10.1515/acv-2018-0024 doi: 10.1515/acv-2018-0024
    [7] C. E. Gutiérrez, A. Incognito, J. L. Torrea, Riesz transforms, g-functions, and multipliers for the Laguerre semigroup, Houston J. Math., 27 (2001), 579–592. https://doi.org/10.1007/s003730170016 doi: 10.1007/s003730170016
    [8] P. Graczyk, J. J. Loeb, I.A. López, A. Nowak, W. Urbina, Higher order Riesz transforms, fractional derivatives, and Sobolev spaces for Laguerre expansions, J. Math. Pures Appl., 84 (2005), 375–405. https://doi.org/10.1016/j.matpur.2004.09.003 doi: 10.1016/j.matpur.2004.09.003
    [9] L. C. Evans, R. F. Gariepy, Measure Theory and Fine Properties of Functions, CRC Press, Boca Raton, FL, 1992. https://doi.org/10.1201/9780203747940
    [10] E. De Giorgi, F. Colombini, L. C. Piccinini, Frontiere orientate di misura minima e questioni collegate, Scuola Normale Superiore, Pisa, 1972.
    [11] E. Giusti, Minimal Surfaces and Functions of Bounded Variation, Birkhäuser Verlag, Basel, 1984. https://doi.org/10.1007/978-1-4684-9486-0
    [12] U. Massari, M. Miranda, Minimal surfaces of codimension one, North-Holland Publishing Co., Amsterdam, 1984. https://doi.org/10.1016/s0304-0208(08)x7038-0
    [13] E, Barozzi, E. Gonzalez, I.Tamanini, The mean curvature of a set of finite perimeter, Proc. Amer. Math.Soc., 99 (1987), 313–316. https://doi.org/10.2307/2046631 doi: 10.2307/2046631
    [14] J. Xiao, N. Zhang, Flux & radii within the subconformal capacity, Calc. Var. Partial Differential Equations, 60 (2021), 120. https://doi.org/10.1007/s00526-021-01989-5 doi: 10.1007/s00526-021-01989-5
    [15] M. Miranda Jr, Functions of bounded variation on "good" metric spaces, J. Math. Pures Appl., 82 (2003), 975–1004. https://doi.org/10.1016/s0021-7824(03)00036-9 doi: 10.1016/s0021-7824(03)00036-9
  • Reader Comments
  • © 2023 the Author(s), licensee AIMS Press. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Metrics

Article views(1108) PDF downloads(133) Cited by(0)

Other Articles By Authors

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return

Catalog