An Algebraic Approach to Symmetry With Applications to Knot Theory
An Algebraic Approach to Symmetry With Applications to Knot Theory
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对称性的代数方法及其在纽结理论中的应用
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发表时间:
1979
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通讯作者:
D. E. Joyce
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作者:
D. E. Joyce
The usual algebraic construction used to study the symmetries of an object is the group of automorphisms of that object. In many geometric settings, however, one may interpret the symmetries in a more intimate manner by an algebraic structure on the object itself. Define a quandle to be a set equipped with two binary operations, (x, y) 7→ x . y and (x, y) 7→ x . y, which satisfies the axioms Q1. x . x = x. Q2. (x . y) . y = x = (x . y) . y. Q3. (x . y) . z = (x . z) .(y . z). Call the map S(y) sending x to x . y the symmetry at y. To each point y of a symmetric space there is a symmetry S(y) of the space. By defining x . y = x . y to be the image of x under S(y), the symmetric space becomes a quandle. Call a quandle satisfying x . y = x . y an involutory quandle. Loos [1] has defined a symmetric space as a manifold with an involutory quandle structure such that each point y is an isolated fixed point of S(y). The underlying set of a group G along with the operations of conjugation, x . y = y−1xy and x . y = yxy−1 form a quandle ConjG. Moreover, the theory of conjugation may be regarded as the theory of quandles in the sense that any equation in . and . holding in ConjG for all groups G also holds in any quandle. If the center of G is trivial, then ConjG determines G. Let G be a group and n ≥ 2. The n-core of G is the set {(x1, x2, . . . , xn) ∈ G |x1x2 . . . xn = 1} along with the operation (x1, x2, . . . , xn) .(y1, y2, . . . , yn) = (y −1 n xny1, y −1 1 x1y2, . . . , y −1 n−1xn−1yn). The n-core is an n-quandle, that is, each symmetry has order dividing n. The group G is simple if and only if its n-core is a simple quandle. Let G be a noncyclic simple group and Q a nontrivial conjugacy class in H viewed as a subquandle of ConjG. Then Q is a simple quandle.