|  Lattice Theory | 
In General > s.a. posets.
  $ Def: A poset in which
    every pair of elements (x, y) has a least upper bound
    x ∨ y (l.u.b., or join) and a greatest lower
    bound x ∧ y (g.l.b., or meet).
  * Examples: The lattice of
    propositions in (quantum) logic; The lattice of partitions of a positive
    integer; The lattice of subsets of a set X, or of causally closed
    subsets of spacetime M, or of all closed vector subspaces of a
    Hilbert space \(\cal H\) (these are all orthocomplemented).
  > Online resources:
    see Wikipedia page.
Special Types and Related Concepts
  * Complete lattice: One in
    which the meet and the join exist for arbitrary families of elements.
  * Unit and zero elements: The
    greatest and least elements  in A (if they exist), i.e., elements
    0 and 1 such that for all x in A, 0 ≤ x ≤ 1.
  * Complement of an element:
    An operation x \(\mapsto\) x' defined on a bounded lattice
    with greatest element 1 and least element 0, such that x ∨ x'
    = 1 and x ∧ x' = 0.
  * Orthomodular lattice: One such
    that for all x, y in A, we have y ⊆
    x implies x ∧ (y ∨ x') = y;
    This condition is weaker than distributivity.
  * Result: An orthomodular
    lattice L is determined by its lattice of subalgebras Sub(L),
    as well as by its poset of Boolean subalgebras BSub(L).
  @ Orthomodular: Harding IJTP(04) [concrete];
    Greechie & Legan IJTP(06) [three classes];
    Brunet IJTP(07)qp [intrinsic topology];
    Harding & Navara a1009 [subalgebras].
References
  @ General: Szasz 63; Birkhoff 67;
    Grätzer 03,
    09,
    11.
  @ Examples: Latapy & Phan DM(09) [partitions of a positive integer].
  @ Special approaches:
    Grätzer 05 [finite lattices, proof-by-picture].
  @ Number of paths: Mohanty 79;
    Coker DM(03).
Lattices in the Sense of Spatial Patterns
  > Types: see crystals;
    ising model [Archimedean and Laves lattices]; non-commutative geometry.
  > Physical theories on lattices:
    see lattice field theory; Measurements;
    optics [optical lattices]; spin models.
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  send feedback and suggestions to bombelli at olemiss.edu – modified 17 jan 2016