pnas/pnas.tex
changeset 645 4e816ca8b5e2
parent 644 975c807661ca
child 646 895b57485dfa
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   282 Because we are mainly interested in the case of strong duality, we replace the intervals $[0,r]$ not with
   282 Because we are mainly interested in the case of strong duality, we replace the intervals $[0,r]$ not with
   283 a product of $k$ intervals (c.f. \cite{0909.2212}) but rather with any $k$-ball, that is, any $k$-manifold which is homeomorphic
   283 a product of $k$ intervals (c.f. \cite{0909.2212}) but rather with any $k$-ball, that is, any $k$-manifold which is homeomorphic
   284 to the standard $k$-ball $B^k$.
   284 to the standard $k$-ball $B^k$.
   285 \nn{maybe add that in addition we want functoriality}
   285 \nn{maybe add that in addition we want functoriality}
   286 
   286 
   287 By default our balls are oriented,
   287 By default our balls are unoriented,
   288 but it is useful at times to vary this,
   288 but it is useful at times to vary this,
   289 for example by considering unoriented or Spin balls.
   289 for example by considering oriented or Spin balls.
   290 We can also consider more exotic structures, such as balls with a map to some target space,
   290 We can also consider more exotic structures, such as balls with a map to some target space,
   291 or equipped with $m$ independent vector fields.
   291 or equipped with $m$ independent vector fields.
   292 (The latter structure would model $n$-categories with less duality than we usually assume.)
   292 (The latter structure would model $n$-categories with less duality than we usually assume.)
   293 
   293 
   294 \begin{axiom}[Morphisms]
   294 \begin{axiom}[Morphisms]