Ascendant subgroupIn mathematics, in the field of group theory, a subgroup of a group is said to be ascendant if there is an ascending series starting from the subgroup and ending at the group, such that every term in the series is a normal subgroup of its successor. The series may be infinite. If the series is finite, then the subgroup is subnormal. Here are some properties of ascendant subgroups: Every subnormal subgroup is ascendant; every ascendant subgroup is serial. In a finite group, the properties of being ascendant and subnormal are equivalent.
Semi-locally simply connectedIn mathematics, specifically algebraic topology, semi-locally simply connected is a certain local connectedness condition that arises in the theory of covering spaces. Roughly speaking, a topological space X is semi-locally simply connected if there is a lower bound on the sizes of the “holes” in X. This condition is necessary for most of the theory of covering spaces, including the existence of a universal cover and the Galois correspondence between covering spaces and subgroups of the fundamental group.
Catégorie trianguléeEn mathématiques, une catégorie triangulée est une catégorie dotée d'une structure supplémentaire. De telles catégories ont été suggérées par Alexander Grothendieck et développées par Jean-Louis Verdier dans sa thèse de 1963 pour traiter les catégories dérivées. La notion de t-structure, qui y est directement liée, permet de reconstruire (en un sens partiel) une catégorie à partir d'une catégorie dérivée.
Théorème de factorisationEn mathématiques, le théorème de factorisation est un principe général qui permet de construire un morphisme d'une structure quotient dans un autre espace à partir d'un morphisme de vers , de façon à factoriser ce dernier par la surjection canonique de passage au quotient. Soit un ensemble muni d'une relation d'équivalence et la surjection canonique. L'unicité de g est immédiate et guide la preuve de son existence, dont voici plusieurs variantes : Preuve « naïve » : pour tout élément , on pose .
Espace totalement discontinuEn mathématiques, plus précisément en topologie, un espace totalement discontinu est un espace topologique qui est « le moins connexe possible » au sens où il n'a pas de partie connexe non triviale : dans tout espace topologique, l'ensemble vide et les singletons sont connexes ; dans un espace totalement discontinu, ce sont les seules parties connexes. Un exemple populaire d'espace totalement discontinu est l'ensemble de Cantor. Un autre exemple, important en théorie algébrique des nombres, est le corps Qp des nombres p-adiques.
Indefinite orthogonal groupIn mathematics, the indefinite orthogonal group, O(p, q) is the Lie group of all linear transformations of an n-dimensional real vector space that leave invariant a nondegenerate, symmetric bilinear form of signature (p, q), where n = p + q. It is also called the pseudo-orthogonal group or generalized orthogonal group. The dimension of the group is n(n − 1)/2. The indefinite special orthogonal group, SO(p, q) is the subgroup of O(p, q) consisting of all elements with determinant 1.
Covering groupIn mathematics, a covering group of a topological group H is a covering space G of H such that G is a topological group and the covering map p : G → H is a continuous group homomorphism. The map p is called the covering homomorphism. A frequently occurring case is a double covering group, a topological double cover in which H has index 2 in G; examples include the spin groups, pin groups, and metaplectic groups.
Fundamental pair of periodsIn mathematics, a fundamental pair of periods is an ordered pair of complex numbers that defines a lattice in the complex plane. This type of lattice is the underlying object with which elliptic functions and modular forms are defined. A fundamental pair of periods is a pair of complex numbers such that their ratio is not real. If considered as vectors in , the two are not collinear. The lattice generated by and is This lattice is also sometimes denoted as to make clear that it depends on and It is also sometimes denoted by or or simply by The two generators and are called the lattice basis.
