Dedekind lattice - definição. O que é Dedekind lattice. Significado, conceito
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O que (quem) é Dedekind lattice - definição

MEET-JOIN LATTICE THAT SATISFIES THE SELF-DUAL MODULAR LAW
Diamond isomorphism theorem; Dedekind lattice; M-symmetric lattice; Modular pair; Modular law
  • ''st''-planar graph]].
  • Free modular lattice generated by three elements {x,y,z}
  • (''x''∨''a'')∧''b''}}.

Modular lattice         
In the branch of mathematics called order theory, a modular lattice is a lattice that satisfies the following self-dual condition,
Dedekind cut         
  • irrational]], [[real number]]s.
METHOD OF CONSTRUCTION OF THE REAL NUMBERS
Dedekind cuts; Dedekind section; Completion (order theory); Dedekind's Axiom; Dedekind Cut
In mathematics, Dedekind cuts, named after German mathematician Richard Dedekind but previously considered by Joseph Bertrand, are а method of construction of the real numbers from the rational numbers. A Dedekind cut is a partition of the rational numbers into two sets A and B, such that all elements of A are less than all elements of B, and A contains no greatest element.
Lattice (order)         
  • '''Pic.&nbsp;6:'''  Non-lattice poset: <math>c</math> and <math>d</math> have no common upper bound.
  • '''Pic.&nbsp;10:''' Smallest non-distributive (but modular) lattice M<sub>3</sub>.
  • '''Pic.&nbsp;9:''' Monotonic map <math>f</math> between lattices that preserves neither joins nor meets, since <math>f(u) \vee f(v) = u^{\prime} \vee u^{\prime}= u^{\prime}</math> <math>\neq</math> <math>1^{\prime} = f(1) = f(u \vee v)</math> and <math>f(u) \wedge f(v) = u^{\prime} \wedge u^{\prime} = u^{\prime}</math> <math>\neq</math> <math>0^{\prime} = f(0) = f(u \wedge v).</math>
  • '''Pic.&nbsp;11:''' Smallest non-modular (and hence non-distributive) lattice N<sub>5</sub>. <br>The labelled elements violate the distributivity equation <math>c \wedge (a \vee b) = (c \wedge a) \vee (c \wedge b),</math> but satisfy its dual <math>c \vee (a \wedge b) = (c \vee a) \wedge (c \vee b).</math>
  • '''Pic.&nbsp;7:''' Non-lattice poset: <math>b</math> and <math>c</math> have common upper bounds <math>d, e,</math> and <math>f,</math> but none of them is the [[least upper bound]].
  • '''Pic.&nbsp;8:''' Non-lattice poset: <math>a</math> and <math>b</math> have common lower bounds <math>0, d, g, h,</math> and <math>i,</math> but none of them is the [[greatest lower bound]].
PARTIALLY ORDERED SET THAT ADMITS GREATEST LOWER AND LEAST UPPER BOUNDS
Lattice theory; Bounded lattice; Lattice (algebra); Lattice (order theory); Lattice homomorphism; Lattice Homomorphism; Lattice Automorphism; Lattice automorphism; Lattice Endomorphism; Lattice endomorphism; Lattice Isomorphism; Lattice isomorphism; Sublattice; Lattice order; Conditionally complete lattice; Complement (order theory); Jordan–Dedekind chain condition; Jordan-Dedekind chain condition; Jordan-Dedekind property; Jordan-Dedekind lattice; Jordan-dedekind property; Jordan-dedekind lattice; Jordan–Dedekind lattice; Partial lattice; Join-irreducible; Meet-irreducible; Join-prime; Meet-prime; Separating lattice homomorphism; Complementation (lattice theory); Complement (lattice theory)
A lattice is an abstract structure studied in the mathematical subdisciplines of order theory and abstract algebra. It consists of a partially ordered set in which every pair of elements has a unique supremum (also called a least upper bound or join) and a unique infimum (also called a greatest lower bound or meet).

Wikipédia

Modular lattice

In the branch of mathematics called order theory, a modular lattice is a lattice that satisfies the following self-dual condition,

Modular law
ab implies a ∨ (xb) = (ax) ∧ b

where x, a, b are arbitrary elements in the lattice,  ≤  is the partial order, and  ∨  and  ∧ (called join and meet respectively) are the operations of the lattice. This phrasing emphasizes an interpretation in terms of projection onto the sublattice [a, b], a fact known as the diamond isomorphism theorem. An alternative but equivalent condition stated as an equation (see below) emphasizes that modular lattices form a variety in the sense of universal algebra.

Modular lattices arise naturally in algebra and in many other areas of mathematics. In these scenarios, modularity is an abstraction of the 2nd Isomorphism Theorem. For example, the subspaces of a vector space (and more generally the submodules of a module over a ring) form a modular lattice.

In a not necessarily modular lattice, there may still be elements b for which the modular law holds in connection with arbitrary elements x and a (for ab). Such an element is called a modular element. Even more generally, the modular law may hold for any a and a fixed pair (x, b). Such a pair is called a modular pair, and there are various generalizations of modularity related to this notion and to semimodularity.

Modular lattices are sometimes called Dedekind lattices after Richard Dedekind, who discovered the modular identity in several motivating examples.