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Sufficiency of -cyclical monotonicity in a class of multi-marginal optimal transport problems 一类多边际最优运输问题中周期单调性的充分性
IF 1.9 4区 数学 Q1 Mathematics Pub Date : 2024-05-14 DOI: 10.1017/s0956792524000202
Luigi De Pascale, Anna Kausamo

$c$-cyclical monotonicity is the most important optimality condition for an optimal transport plan. While the proof of necessity is relatively easy, the proof of sufficiency is often more difficult or even elusive. We present here a new approach, and we show how known results are derived in this new framework and how this approach allows to prove sufficiency in situations previously not treatable.

c$周期单调性是最优运输计划最重要的最优性条件。必要性的证明相对容易,但充分性的证明往往比较困难,甚至难以捉摸。我们在此介绍一种新方法,并展示如何在这一新框架下推导出已知结果,以及这种方法如何在以前无法处理的情况下证明充分性。
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引用次数: 0
Unified framework for the separation property in binary phase-segregation processes with singular entropy densities 具有奇异熵密度的二元相分离过程中分离特性的统一框架
IF 1.9 4区 数学 Q1 Mathematics Pub Date : 2024-05-09 DOI: 10.1017/s0956792524000196
Ciprian G. Gal, Andrea Poiatti
This paper investigates the separation property in binary phase-segregation processes modelled by Cahn-Hilliard type equations with constant mobility, singular entropy densities and different particle interactions. Under general assumptions on the entropy potential, we prove the strict separation property in both two and three-space dimensions. Namely, in 2D, we notably extend the minimal assumptions on the potential adopted so far in the literature, by only requiring a mild growth condition of its first derivative near the singular points $pm 1$ , without any pointwise additional assumption on its second derivative. For all cases, we provide a compact proof using De Giorgi’s iterations. In 3D, we also extend the validity of the asymptotic strict separation property to the case of fractional Cahn-Hilliard equation, as well as show the validity of the separation when the initial datum is close to an ‘energy minimizer’. Our framework offers insights into statistical factors like particle interactions, entropy choices and correlations governing separation, with broad applicability.
本文研究了在具有恒定流动性、奇异熵密度和不同粒子相互作用的卡恩-希利亚德方程模拟的二元相分离过程中的分离特性。在熵势的一般假设下,我们证明了二维和三维空间的严格分离特性。也就是说,在二维空间中,我们显著地扩展了迄今为止文献中采用的对熵势的最小假设,只要求在奇点 $pm 1$ 附近对其一阶导数有一个温和的增长条件,而不对其二阶导数做任何点上的额外假设。对于所有情况,我们都用德乔吉迭代法给出了简洁的证明。在三维空间中,我们还将渐近严格分离性质的有效性扩展到分数卡恩-希利亚德方程的情况,并证明了当初始基准接近 "能量最小化 "时分离的有效性。我们的框架深入揭示了粒子相互作用、熵选择和相关性等统计因素对分离的影响,具有广泛的适用性。
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引用次数: 0
Threshold dynamics scenario of a plants-pollinators cooperative system with impulsive effect on a periodically evolving domain 周期性演化域上具有脉冲效应的植物-传粉者合作系统的阈值动力学情景
IF 1.9 4区 数学 Q1 Mathematics Pub Date : 2024-05-02 DOI: 10.1017/s0956792524000135
Jie Wang, Ruirui Yang, Jian Wang, Jianxiong Cao
Flowering plants depend on some animals for pollination and contribute to nourish the animals in natural environments. We call these animals pollinators and build a plants-pollinators cooperative model with impulsive effect on a periodically evolving domain. Next, we define the ecological reproduction index for single plant model and plants-pollinators system, respectively, whose threshold dynamics, including the extinction, persistence and coexistence, is established by the method of upper and lower solutions. Theoretical analysis shows that a large domain evolution rate has a positive influence on the survival of pollinators whether or not the impulsive effect occurs, and the pulse eliminates the pollinators even when the evolution rate is high. Moreover, some selective numerical simulations are still performed to explain our theoretical results.
在自然环境中,开花植物依靠一些动物授粉,并为动物提供营养。我们称这些动物为传粉者,并在一个周期性演化的领域中建立了一个具有脉冲效应的植物-传粉者合作模型。接下来,我们分别定义了单一植物模型和植物-传粉者系统的生态繁殖指数,并通过上解法和下解法建立了其阈值动态,包括灭绝、持续和共存。理论分析表明,无论是否发生脉冲效应,大的域进化速率都会对传粉昆虫的生存产生积极影响,即使在进化速率较高的情况下,脉冲也会淘汰传粉昆虫。此外,我们还进行了一些选择性数值模拟,以解释我们的理论结果。
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引用次数: 0
Emergent behaviours of a non-abelian quantum synchronisation model over the unitary group 单位群上非阿贝尔量子同步模型的新兴行为
IF 1.9 4区 数学 Q1 Mathematics Pub Date : 2024-04-30 DOI: 10.1017/s095679252400010x
Dohyun Kim, Jeongho Kim
We introduce a new non-abelian quantum synchronisation model over the unitary group, represented as a gradient flow, where state matrices asymptotically converge to a common one up to phase translation. We provide a sufficient framework leading to quantum synchronisation based on Riccati-type differential inequalities. In addition, uniform time-delayed interaction is considered for modelling realistic communication, and we demonstrate that quantum synchronisation is persistent when a small time delay is allowed. Finally, numerical simulation is performed to visualise qualitative behaviours and support theoretical results.
我们在单元群上引入了一个新的非阿贝尔量子同步模型,它以梯度流的形式表示,其中的状态矩阵在相位平移之前会渐近收敛到一个共同的状态矩阵。我们提供了一个基于里卡蒂式微分不等式的量子同步充分框架。此外,我们还考虑了统一的时间延迟相互作用,以模拟现实通信,并证明了在允许较小时间延迟的情况下,量子同步是持久的。最后,我们进行了数值模拟,以直观显示定性行为并支持理论结果。
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引用次数: 0
Flocking dynamics of agents moving with a constant speed and a randomly switching topology 以恒定速度和随机切换的拓扑结构移动的探针的成群动力学
IF 1.9 4区 数学 Q1 Mathematics Pub Date : 2024-04-30 DOI: 10.1017/s0956792524000214
Hyunjin Ahn, Woojoo Shim
In this paper, we present a sufficient framework to exhibit the sample path-wise asymptotic flocking dynamics of the Cucker–Smale model with unit-speed constraint and the randomly switching network topology. We employ a matrix formulation of the given equation, which allows us to evaluate the diameter of velocities with respect to the adjacency matrix of the network. Unlike the previous result on the randomly switching Cucker–Smale model, the unit-speed constraint disallows the system to be considered as a nonautonomous linear ordinary differential equation on velocity vector, which forces us to get a weaker form of the flocking estimate than the result for the original Cucker–Smale model.
在本文中,我们提出了一个充分的框架来展示具有单位速度约束和随机切换网络拓扑的 Cucker-Smale 模型的样本路径渐近成群动力学。我们对给定方程采用矩阵表述,这样就能评估相对于网络邻接矩阵的速度直径。与之前随机切换 Cucker-Smale 模型的结果不同,单位速度约束不允许将系统视为速度向量上的非自治线性常微分方程,这迫使我们得到比原始 Cucker-Smale 模型结果更弱的植群估计形式。
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引用次数: 0
Modelling of the fluid flow in a thin domain with injection through permeable boundary 通过渗透边界注入薄域中的流体流动建模
IF 1.9 4区 数学 Q1 Mathematics Pub Date : 2024-04-25 DOI: 10.1017/s0956792524000123
E. Marušić‐Paloka, Igor Pažanin
In this paper, we derive the effective model describing a thin-domain flow with permeable boundary through which the fluid is injected into the domain. We start with incompressible Stokes system and perform the rigorous asymptotic analysis. Choosing the appropriate scaling for the injection leads to a compressible effective model. In this paper, we derive the effective model describing a thin-domain flow with permeable boundary through which the fluid is injected into the domain. We start with incompressible Stokes system and perform the rigorous asymptotic analysis. Choosing the appropriate scaling for the injection leads to a compressible effective model.
在本文中,我们推导了描述具有渗透边界的薄域流动的有效模型,流体通过渗透边界注入薄域。我们从不可压缩斯托克斯系统入手,进行了严格的渐近分析。为注入流体选择适当的缩放比例可得到可压缩的有效模型。在本文中,我们推导了描述具有可渗透边界的薄域流动的有效模型,流体通过该边界注入域中。我们从不可压缩斯托克斯系统入手,进行了严格的渐近分析。为注入流体选择适当的缩放比例可得到可压缩的有效模型。
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引用次数: 0
Uniform propagation of chaos for a dollar exchange econophysics model 美元兑换经济物理模型的混乱均匀传播
IF 1.9 4区 数学 Q1 Mathematics Pub Date : 2024-04-22 DOI: 10.1017/s0956792524000184
Fei Cao, Roberto Cortez
We study the poor-biased model for money exchange introduced in Cao & Motsch ((2023) Kinet. Relat. Models 16(5), 764–794.): agents are being randomly picked at a rate proportional to their current wealth, and then the selected agent gives a dollar to another agent picked uniformly at random. Simulations of a stochastic system of finitely many agents as well as a rigorous analysis carried out in Cao & Motsch ((2023) Kinet. Relat. Models 16(5), 764–794.), Lanchier ((2017) J. Stat. Phys. 167(1), 160–172.) suggest that, when both the number of agents and time become large enough, the distribution of money among the agents converges to a Poisson distribution. In this manuscript, we establish a uniform-in-time propagation of chaos result as the number of agents goes to infinity, which justifies the validity of the mean-field deterministic infinite system of ordinary differential equations as an approximation of the underlying stochastic agent-based dynamics.
我们研究了 Cao & Motsch((2023)Kinet.Relat.Models 16(5), 764-794. )中提出的货币交换的穷人偏好模型:代理人按与其当前财富成正比的比率被随机选中,然后被选中的代理人给另一个统一随机选中的代理人一美元。Cao & Motsch((2023)Kinet.Relat.Models 16(5), 764-794.), Lanchier ((2017) J. Stat.Phys.167(1),160-172.)提出,当代理人数量和时间都变得足够大时,代理人之间的资金分布会收敛到泊松分布。在本手稿中,我们建立了一个当代理人数量达到无穷大时的均匀时间内混沌传播结果,这证明了均值场确定性无限常微分方程系统作为基于底层随机代理人动力学近似的有效性。
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引用次数: 0
Macroscopic limit of a Fokker-Planck model of swarming rigid bodies 蜂拥刚体的福克-普朗克模型的宏观极限
IF 1.9 4区 数学 Q1 Mathematics Pub Date : 2024-04-19 DOI: 10.1017/s0956792524000111
Pierre Degond, Amic Frouvelle
We consider self-propelled rigid bodies interacting through local body-attitude alignment modelled by stochastic differential equations. We derive a hydrodynamic model of this system at large spatio-temporal scales and particle numbers in any dimension $n geq 3$ . This goal was already achieved in dimension $n=3$ or in any dimension $n geq 3$ for a different system involving jump processes. However, the present work corresponds to huge conceptual and technical gaps compared with earlier ones. The key difficulty is to determine an auxiliary but essential object, the generalised collision invariant. We achieve this aim by using the geometrical structure of the rotation group, namely its maximal torus, Cartan subalgebra and Weyl group as well as other concepts of representation theory and Weyl’s integration formula. The resulting hydrodynamic model appears as a hyperbolic system whose coefficients depend on the generalised collision invariant.
我们考虑的是通过随机微分方程模拟的局部身体-姿态排列相互作用的自推进刚体。我们推导了该系统在任意维度 $n geq 3$ 的大时空尺度和粒子数下的流体力学模型。这一目标已经在维数 $n=3$ 或涉及跃迁过程的不同系统的任意维数 $n geq 3$ 中实现。然而,与先前的工作相比,目前的工作在概念和技术上存在巨大差距。关键的困难在于确定一个辅助但重要的对象--广义碰撞不变式。我们通过使用旋转群的几何结构,即其最大环、卡坦子代数和韦尔群,以及表示论和韦尔积分公式的其他概念来实现这一目标。由此产生的流体力学模型是一个双曲系统,其系数取决于广义碰撞不变式。
{"title":"Macroscopic limit of a Fokker-Planck model of swarming rigid bodies","authors":"Pierre Degond, Amic Frouvelle","doi":"10.1017/s0956792524000111","DOIUrl":"https://doi.org/10.1017/s0956792524000111","url":null,"abstract":"We consider self-propelled rigid bodies interacting through local body-attitude alignment modelled by stochastic differential equations. We derive a hydrodynamic model of this system at large spatio-temporal scales and particle numbers in any dimension <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0956792524000111_inline1.png\" /> <jats:tex-math> $n geq 3$ </jats:tex-math> </jats:alternatives> </jats:inline-formula>. This goal was already achieved in dimension <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0956792524000111_inline2.png\" /> <jats:tex-math> $n=3$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> or in any dimension <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" xlink:href=\"S0956792524000111_inline3.png\" /> <jats:tex-math> $n geq 3$ </jats:tex-math> </jats:alternatives> </jats:inline-formula> for a different system involving jump processes. However, the present work corresponds to huge conceptual and technical gaps compared with earlier ones. The key difficulty is to determine an auxiliary but essential object, the generalised collision invariant. We achieve this aim by using the geometrical structure of the rotation group, namely its maximal torus, Cartan subalgebra and Weyl group as well as other concepts of representation theory and Weyl’s integration formula. The resulting hydrodynamic model appears as a hyperbolic system whose coefficients depend on the generalised collision invariant.","PeriodicalId":51046,"journal":{"name":"European Journal of Applied Mathematics","volume":null,"pages":null},"PeriodicalIF":1.9,"publicationDate":"2024-04-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140630596","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
A finite-volume scheme for fractional diffusion on bounded domains 有界域上分数扩散的有限体积方案
IF 1.9 4区 数学 Q1 Mathematics Pub Date : 2024-04-16 DOI: 10.1017/s0956792524000172
Rafael Bailo, José A. Carrillo, Stefano Fronzoni, David Gómez-Castro

We propose a new fractional Laplacian for bounded domains, expressed as a conservation law and thus particularly suited to finite-volume schemes. Our approach permits the direct prescription of no-flux boundary conditions. We first show the well-posedness theory for the fractional heat equation. We also develop a numerical scheme, which correctly captures the action of the fractional Laplacian and its anomalous diffusion effect. We benchmark numerical solutions for the Lévy–Fokker–Planck equation against known analytical solutions. We conclude by numerically exploring properties of these equations with respect to their stationary states and long-time asymptotics.

我们为有界域提出了一种新的分数拉普拉斯,它以守恒定律的形式表示,因此特别适用于有限体积方案。我们的方法允许直接规定无流动边界条件。我们首先展示了分数热方程的拟合理论。我们还开发了一种数值方案,它能正确捕捉分数拉普拉斯的作用及其反常扩散效应。我们将 Lévy-Fokker-Planck 方程的数值解与已知的分析解进行比较。最后,我们用数值方法探讨了这些方程的静止状态和长时间渐近特性。
{"title":"A finite-volume scheme for fractional diffusion on bounded domains","authors":"Rafael Bailo, José A. Carrillo, Stefano Fronzoni, David Gómez-Castro","doi":"10.1017/s0956792524000172","DOIUrl":"https://doi.org/10.1017/s0956792524000172","url":null,"abstract":"<p>We propose a new fractional Laplacian for bounded domains, expressed as a conservation law and thus particularly suited to finite-volume schemes. Our approach permits the direct prescription of no-flux boundary conditions. We first show the well-posedness theory for the fractional heat equation. We also develop a numerical scheme, which correctly captures the action of the fractional Laplacian and its anomalous diffusion effect. We benchmark numerical solutions for the Lévy–Fokker–Planck equation against known analytical solutions. We conclude by numerically exploring properties of these equations with respect to their stationary states and long-time asymptotics.</p>","PeriodicalId":51046,"journal":{"name":"European Journal of Applied Mathematics","volume":null,"pages":null},"PeriodicalIF":1.9,"publicationDate":"2024-04-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140576039","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Large Péclet number forced convection from a circular wire in a uniform stream: hybrid approximations at small Reynolds numbers 均匀流中圆导线的大佩克莱特数强制对流:小雷诺数下的混合近似值
IF 1.9 4区 数学 Q1 Mathematics Pub Date : 2024-04-16 DOI: 10.1017/s0956792524000147
Ehud Yariv

We consider heat or mass transport from a circular cylinder under a uniform crossflow at small Reynolds numbers, $mathrm{Re}ll 1$. This problem has been thwarted in the past by limitations inherent in the classical analyses of the singular flow problem, which have used asymptotic expansions in inverse powers of $log mathrm{Re}$. We here make use of the hybrid approximation of Kropinski, Ward & Keller [(1995) SIAM J. Appl. Math. 55, 1484], based upon a robust asymptotic expansion in powers of $mathrm{Re}$. In that approximation, the “inner” streamfunction is provided by the product of a pre-factor $S$, a slowly varying function of $mathrm{Re}$, with a $mathrm{Re}$-independent “canonical” solution of a simple mathematical form. The pre-factor, in turn, is determined as an implicit function of $log mathrm{Re}$ via asymptotic matching with a numerical solution of the nonlinear single-scaled “outer” problem, where the cylinder appears as a point singularity. We exploit the hybrid approximation to analyse

我们考虑的是在小雷诺数($mathrm{Re}ll 1$)条件下,在均匀横流作用下圆柱体的热量或质量传输问题。过去,由于对奇异流动问题的经典分析中固有的局限性,这个问题一直受到阻碍,因为经典分析使用了$log mathrm{Re}$的反幂的渐近展开。在此,我们使用 Kropinski, Ward & Keller 的混合近似[(1995) SIAM J. Appl.在这种近似方法中,"内部 "流函数是由前因$S$(一个缓慢变化的$mathrm{Re}$函数)与一个独立于$mathrm{Re}$的、数学形式简单的 "典型 "解的乘积提供的。通过与非线性单尺度 "外部 "问题数值解的渐近匹配,预因子反过来被确定为$log mathrm{Re}$的隐含函数,其中圆柱体作为一个点奇点出现。我们利用混合近似来分析大佩克莱特数($mathrm{Pe}gg 1$)极限下的传输问题。在这一极限中,输运被限制在圆柱体表面的狭窄边界层中--这一区域包含在流动问题的内部区域中。以 $S$ 作为参数,很容易构建出边界层问题的相似解。它提供的努塞尔特数为 $0.5799(S,mathrm{Pe})^{1/3}$。这一渐近预测与精确问题的数值解[Dennis, Hudson & Smith (1968) Phys. Fluids 11, 933]非常接近,即使是中等的 $mathrm{Re}$ 值也是如此。
{"title":"Large Péclet number forced convection from a circular wire in a uniform stream: hybrid approximations at small Reynolds numbers","authors":"Ehud Yariv","doi":"10.1017/s0956792524000147","DOIUrl":"https://doi.org/10.1017/s0956792524000147","url":null,"abstract":"<p>We consider heat or mass transport from a circular cylinder under a uniform crossflow at small Reynolds numbers, <span><span><img data-mimesubtype=\"png\" data-type=\"\" src=\"https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20240415115644043-0058:S0956792524000147:S0956792524000147_inline1.png\"><span data-mathjax-type=\"texmath\"><span>$mathrm{Re}ll 1$</span></span></img></span></span>. This problem has been thwarted in the past by limitations inherent in the classical analyses of the singular flow problem, which have used asymptotic expansions in inverse powers of <span><span><img data-mimesubtype=\"png\" data-type=\"\" src=\"https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20240415115644043-0058:S0956792524000147:S0956792524000147_inline2.png\"><span data-mathjax-type=\"texmath\"><span>$log mathrm{Re}$</span></span></img></span></span>. We here make use of the hybrid approximation of Kropinski, Ward &amp; Keller [(1995) SIAM <span>J. Appl. Math.</span> <span>55</span>, 1484], based upon a robust asymptotic expansion in powers of <span><span><img data-mimesubtype=\"png\" data-type=\"\" src=\"https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20240415115644043-0058:S0956792524000147:S0956792524000147_inline3.png\"><span data-mathjax-type=\"texmath\"><span>$mathrm{Re}$</span></span></img></span></span>. In that approximation, the “inner” streamfunction is provided by the product of a pre-factor <span><span><img data-mimesubtype=\"png\" data-type=\"\" src=\"https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20240415115644043-0058:S0956792524000147:S0956792524000147_inline4.png\"><span data-mathjax-type=\"texmath\"><span>$S$</span></span></img></span></span>, a slowly varying function of <span><span><img data-mimesubtype=\"png\" data-type=\"\" src=\"https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20240415115644043-0058:S0956792524000147:S0956792524000147_inline5.png\"><span data-mathjax-type=\"texmath\"><span>$mathrm{Re}$</span></span></img></span></span>, with a <span><span><img data-mimesubtype=\"png\" data-type=\"\" src=\"https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20240415115644043-0058:S0956792524000147:S0956792524000147_inline6.png\"><span data-mathjax-type=\"texmath\"><span>$mathrm{Re}$</span></span></img></span></span>-independent “canonical” solution of a simple mathematical form. The pre-factor, in turn, is determined as an implicit function of <span><span><img data-mimesubtype=\"png\" data-type=\"\" src=\"https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20240415115644043-0058:S0956792524000147:S0956792524000147_inline7.png\"><span data-mathjax-type=\"texmath\"><span>$log mathrm{Re}$</span></span></img></span></span> via asymptotic matching with a numerical solution of the nonlinear single-scaled “outer” problem, where the cylinder appears as a point singularity. We exploit the hybrid approximation to analyse","PeriodicalId":51046,"journal":{"name":"European Journal of Applied Mathematics","volume":null,"pages":null},"PeriodicalIF":1.9,"publicationDate":"2024-04-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140602836","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
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European Journal of Applied Mathematics
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