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thin equivalence relation (Definition)

1 Thin equivalence relation

Definition 1.1.

Let a,a: x y be paths in X. Then a is thinly equivalent to a, denoted a T a, if there is a thin relative homotopy between a and a.

We note that T is an equivalence relation, see [2]. We use a: x y to denote the T class of a path a : x y and call athe semitrack of a. The groupoid structure of ρ1(X) is induced by concatenation, +, of paths. Here one makes use of the fact that if a : x x, a: x′≃ x′′, a′′ : x′′≃ x′′′ are paths then there are canonical thin relative homotopies

         ′     ′′         ′   ′′       ′′′
   (a + a ) + a ≃ ′a + (a + a ) : x ≃ x′ (rescale)
a + ex′ ≃ a : x ≃ x ; ex + a ≃ a : x ≃ x (dilation)
             a + (− a) ≃ ex : x ≃ x (cancellation).

The source and target maps of ρ1(X) are given by

∂ −⟨a⟩ = x, ∂+ ⟨a⟩ = y,
  1           1

if a: x y is a semitrack. Identities and inverses are given by

𝜀(x) = ⟨ex⟩  resp.− ⟨a⟩ = ⟨− a⟩.

References

[1]   K.A. Hardie, K.H. Kamps and R.W. Kieboom, A homotopy 2-groupoid of a Hausdorff space, Applied Cat. Structures, 8 (2000): 209-234.

[2]   R. Brown, K.A. Hardie, K.H. Kamps and T. Porter, A homotopy double groupoid of a Hausdorff space, Theory and Applications of Categories 10,(2002): 71-93.


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Keywords:  thin equivalence relation

Cross-references: identities, target maps, groupoid, equivalence relation, homotopy, thinly equivalent

This is version 1 of thin equivalence relation, born on 2009-04-19.
Object id is 670, canonical name is ThinEquivalenceRelation.
Accessed 1902 times total.

Classification:
Physics Classification00. (GENERAL)
 02. (Mathematical methods in physics)
 03. (Quantum mechanics, field theories, and special relativity )
 03.65.Fd (Algebraic methods )
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