Problem about frame bundle in Kobayashi's book











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I'm reading Kobayashi's book "Transformation Groups in Differential Geometry" and I have a problem in the proof of this lemma:



enter image description here



At the converse part he says this: enter image description here
My question is about $f,$ namely, how is $f$ defined?










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    up vote
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    down vote

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    I'm reading Kobayashi's book "Transformation Groups in Differential Geometry" and I have a problem in the proof of this lemma:



    enter image description here



    At the converse part he says this: enter image description here
    My question is about $f,$ namely, how is $f$ defined?










    share|cite|improve this question
























      up vote
      0
      down vote

      favorite









      up vote
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      down vote

      favorite











      I'm reading Kobayashi's book "Transformation Groups in Differential Geometry" and I have a problem in the proof of this lemma:



      enter image description here



      At the converse part he says this: enter image description here
      My question is about $f,$ namely, how is $f$ defined?










      share|cite|improve this question













      I'm reading Kobayashi's book "Transformation Groups in Differential Geometry" and I have a problem in the proof of this lemma:



      enter image description here



      At the converse part he says this: enter image description here
      My question is about $f,$ namely, how is $f$ defined?







      fiber-bundles principal-bundles






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      asked Nov 18 at 19:50









      Hurjui Ionut

      458211




      458211






















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          Let $pi:L(M)to M$ by the projection onto the base. Define $f:Mto M$ by $f(x) := pi(F(p))$, where $pin pi^{-1}(x)subset L(M)$ is arbitrary. Since $F:L(M)to L(M)$ is fibre-preserving (and so maps the fibre $pi^{-1}(x)$ into some other fibre $pi^{-1}(y)$), this definition is independent of the choice of $pin pi^{-1}(x)$, and so gives a function satisfying $fcirc pi = picirc F$.






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            1 Answer
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            1 Answer
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            active

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            active

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            up vote
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            accepted










            Let $pi:L(M)to M$ by the projection onto the base. Define $f:Mto M$ by $f(x) := pi(F(p))$, where $pin pi^{-1}(x)subset L(M)$ is arbitrary. Since $F:L(M)to L(M)$ is fibre-preserving (and so maps the fibre $pi^{-1}(x)$ into some other fibre $pi^{-1}(y)$), this definition is independent of the choice of $pin pi^{-1}(x)$, and so gives a function satisfying $fcirc pi = picirc F$.






            share|cite|improve this answer

























              up vote
              0
              down vote



              accepted










              Let $pi:L(M)to M$ by the projection onto the base. Define $f:Mto M$ by $f(x) := pi(F(p))$, where $pin pi^{-1}(x)subset L(M)$ is arbitrary. Since $F:L(M)to L(M)$ is fibre-preserving (and so maps the fibre $pi^{-1}(x)$ into some other fibre $pi^{-1}(y)$), this definition is independent of the choice of $pin pi^{-1}(x)$, and so gives a function satisfying $fcirc pi = picirc F$.






              share|cite|improve this answer























                up vote
                0
                down vote



                accepted







                up vote
                0
                down vote



                accepted






                Let $pi:L(M)to M$ by the projection onto the base. Define $f:Mto M$ by $f(x) := pi(F(p))$, where $pin pi^{-1}(x)subset L(M)$ is arbitrary. Since $F:L(M)to L(M)$ is fibre-preserving (and so maps the fibre $pi^{-1}(x)$ into some other fibre $pi^{-1}(y)$), this definition is independent of the choice of $pin pi^{-1}(x)$, and so gives a function satisfying $fcirc pi = picirc F$.






                share|cite|improve this answer












                Let $pi:L(M)to M$ by the projection onto the base. Define $f:Mto M$ by $f(x) := pi(F(p))$, where $pin pi^{-1}(x)subset L(M)$ is arbitrary. Since $F:L(M)to L(M)$ is fibre-preserving (and so maps the fibre $pi^{-1}(x)$ into some other fibre $pi^{-1}(y)$), this definition is independent of the choice of $pin pi^{-1}(x)$, and so gives a function satisfying $fcirc pi = picirc F$.







                share|cite|improve this answer












                share|cite|improve this answer



                share|cite|improve this answer










                answered Nov 19 at 4:24









                user17945

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