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单词 811GettingStarted
释义

8.1.1 Getting started


It is not too hard to define functions in both directions between Ω(𝕊1) and .By specializing \\autorefthm:looptothe to 𝗅𝗈𝗈𝗉:𝖻𝖺𝗌𝖾=𝖻𝖺𝗌𝖾, we have a function 𝗅𝗈𝗈𝗉:(𝖻𝖺𝗌𝖾=𝖻𝖺𝗌𝖾) defined (loosely speaking) by

𝗅𝗈𝗈𝗉n={𝗅𝗈𝗈𝗉\\centerdot𝗅𝗈𝗈𝗉\\centerdot\\centerdot𝗅𝗈𝗈𝗉nif n>0,𝗅𝗈𝗈𝗉-1\\centerdot𝗅𝗈𝗈𝗉-1\\centerdot\\centerdot𝗅𝗈𝗈𝗉-1-nif n<0,𝗋𝖾𝖿𝗅𝖻𝖺𝗌𝖾if n=0.

Defining a function g:Ω(𝕊1) in the other direction is a bit trickier.Note that the successor function 𝗌𝗎𝖼𝖼: is an equivalence,and hence induces a path 𝗎𝖺(𝗌𝗎𝖼𝖼):= in the universePlanetmathPlanetmath 𝒰.Thus, the recursion principle of 𝕊1 induces a map c:𝕊1𝒰 by c(𝖻𝖺𝗌𝖾): and 𝖺𝗉c(𝗅𝗈𝗈𝗉):=𝗎𝖺(𝗌𝗎𝖼𝖼).Then we have 𝖺𝗉c:(𝖻𝖺𝗌𝖾=𝖻𝖺𝗌𝖾)(=), and we can define g(p):𝗍𝗋𝖺𝗇𝗌𝗉𝗈𝗋𝗍XX(𝖺𝗉c(p),0).

With these definitions, we can even prove that g(𝗅𝗈𝗈𝗉n)=n for any n:, using the inductionMathworldPlanetmath principle \\autorefthm:sign-induction for n.(We will prove something more general a little later on.)However, the other equality 𝗅𝗈𝗈𝗉g(p)=p is significantly harder.The obvious thing to try is path induction, but path induction does not apply to loops such as p:(𝖻𝖺𝗌𝖾=𝖻𝖺𝗌𝖾) that have both endpoints fixed!A new idea is required, one which can be explained both in terms of classical homotopy theory and in terms of type theoryPlanetmathPlanetmath.We begin with the former.

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更新时间:2025/5/5 4:01:54