77 research outputs found

    A Weyl Entropy of Pure Spacetime Regions

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    We focus on the Penrose's Weyl Curvature Hypothesis in a general framework encompassing many specific models discussed in literature. We introduce a candidate density for the Weyl entropy in pure spacetime perfect fluid regions and show that it is monotonically increasing in time under very general assumptions. Then we consider the behavior of the Weyl entropy of compact regions, which is shown to be monotone in time as well under suitable hypotheses, and also maximal in correspondence with vacuum static metrics. The minimal entropy case is discussed too

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    Set-theoretic solutions to the Yang-Baxter equation and generalized semi-braces

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    This paper aims to introduce a construction technique of set-theoretic solutions of the Yang-Baxter equation, called strong semilattice of solutions. This technique, inspired by the strong semilattice of semigroups, allows one to obtain new solutions. In particular, this method turns out to be useful to provide non-bijective solutions of finite order. It is well-known braces, skew braces and semi-braces are closely linked with solutions. Hence, we introduce a generalization of the algebraic structure of semi-braces based on this new construction technique of solutions

    Set-theoretical solutions of the Yang-Baxter and pentagon equations on semigroups

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    The Yang-Baxter and pentagon equations are two well-known equations of Mathematical Physic. If SS is a set, a map s:S×S→S×Ss:S\times S\to S\times S is said to be a set theoretical solution of the Yang-Baxter equation if s23 s13 s12=s12 s13 s23, s_{23}\, s_{13}\, s_{12} = s_{12}\, s_{13}\, s_{23}, where s12=s×idSs_{12}=s\times id_S, s23=idS×ss_{23}=id_S\times s, and s13=(idS×τ) s12 (idS×τ)s_{13}=(id_S\times \tau)\,s_{12}\,(id_S\times \tau) and τ\tau is the flip map, i.e., the map on S×SS\times S given by τ(x,y)=(y,x)\tau(x,y)=(y,x). Instead, ss is called a set-theoretical solution of the pentagon equation if s23 s13 s12=s12 s23. s_{23}\, s_{13}\, s_{12}=s_{12}\, s_{23}. The main aim of this work is to display how solutions of the pentagon equation turn out to be a useful tool to obtain new solutions of the Yang-Baxter equation. Specifically, we present a new construction of solutions of the Yang-Baxter equation involving two specific solutions of the pentagon equation. To this end, we provide a method to obtain solutions of the pentagon equation on the matched product of two semigroups, that is a semigroup including the classical Zappa product

    Solutions of the Yang-Baxter equation and strong semilattices of skew braces

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    We prove that any set-theoretic solution of the Yang-Baxter equation associated to a dual weak brace is a strong semilattice of non-degenerate bijective solutions. This fact makes use of the description of any dual weak brace SS we provide in terms of strong semilattice YY of skew braces BαB_\alpha, with α∈Y\alpha \in Y. Additionally, we describe the ideals of SS and study its nilpotency by correlating it to that of each skew brace BαB_\alpha

    Inverse semi-braces and the Yang-Baxter equation

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    The main aim of this paper is to provide set-theoretical solutions of the Yang-Baxter equation that are not necessarily bijective, among these new idempotent ones. In the specific, we draw on both to the classical theory of inverse semigroups and to that of the most recently studied braces, to give a new research perspective to the open problem of finding solutions. Namely, we have recourse to a new structure, the inverse semi-brace, that is a triple (S,+,⋅)(S,+, \cdot) with (S,+)(S,+) a semigroup and (S,⋅)(S, \cdot) an inverse semigroup satisfying the relation a(b+c)=ab+a(a−1+c)a \left(b + c\right) = a b + a\left(a^{-1} + c\right), for all a,b,c∈Sa,b,c \in S, where a−1a^{-1} is the inverse of aa in (S,⋅)(S, \cdot). In particular, we give several constructions of inverse semi-braces which allow for obtaining solutions that are different from those until known.Comment: 43 page

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