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Loop Space of $BU times mathbbZ$



The 2019 Stack Overflow Developer Survey Results Are InWhat's the loop space of a circle?Showing that the loopspace $Omega S^infty$ is homotopic to $S^infty$.$pi_0(SO(N))$ and $pi_0(O(N))$: Inconsistency between Bott periodicity and basic understanding of $pi_0$Homotopy groups of spectraClassifying Space for What is the Infinite Unitary Group?What, exactly, is the fundamental group of a free loop space?Relation of $mathbbZ_2$-cohomology and interger cohomologyConstruction of the Stiefel-Whitney ClassesChern Classes IdentificationConsequences from Bott Periodicity










2












$begingroup$


I have a question about an argument that occurred in the discussion about consequences of Bott periodicity in A Concise Course in Algebraic Topology by P. May on page 207. Here is the excerpt:




Could anybody explain the "little argument with $H$-spaces" which May has in mind to show that $Omega^2(BU times mathbbZ) $ is equivalent to $(Omega^2_0BU) times mathbbZ$ as $H$-spaces?




My considerations: As explained above the loop space "sees" only the component of the base point so $Omega^2BU= Omega^2_0BU$.



The problem reduces to two questions:



Does $Omega^2$ respect products like $pi_k(-)$?



And which role does the fact $pi_2(BU) = mathbbZ$ play? This is a statement about homotopy classes of loops $Omega^2(BU)$ but in the considerations above we haven't passed to homotopy classes so here we would "lose" some information.



Does anybody see the correct argument? Thanks in advance.










share|cite|improve this question











$endgroup$
















    2












    $begingroup$


    I have a question about an argument that occurred in the discussion about consequences of Bott periodicity in A Concise Course in Algebraic Topology by P. May on page 207. Here is the excerpt:




    Could anybody explain the "little argument with $H$-spaces" which May has in mind to show that $Omega^2(BU times mathbbZ) $ is equivalent to $(Omega^2_0BU) times mathbbZ$ as $H$-spaces?




    My considerations: As explained above the loop space "sees" only the component of the base point so $Omega^2BU= Omega^2_0BU$.



    The problem reduces to two questions:



    Does $Omega^2$ respect products like $pi_k(-)$?



    And which role does the fact $pi_2(BU) = mathbbZ$ play? This is a statement about homotopy classes of loops $Omega^2(BU)$ but in the considerations above we haven't passed to homotopy classes so here we would "lose" some information.



    Does anybody see the correct argument? Thanks in advance.










    share|cite|improve this question











    $endgroup$














      2












      2








      2





      $begingroup$


      I have a question about an argument that occurred in the discussion about consequences of Bott periodicity in A Concise Course in Algebraic Topology by P. May on page 207. Here is the excerpt:




      Could anybody explain the "little argument with $H$-spaces" which May has in mind to show that $Omega^2(BU times mathbbZ) $ is equivalent to $(Omega^2_0BU) times mathbbZ$ as $H$-spaces?




      My considerations: As explained above the loop space "sees" only the component of the base point so $Omega^2BU= Omega^2_0BU$.



      The problem reduces to two questions:



      Does $Omega^2$ respect products like $pi_k(-)$?



      And which role does the fact $pi_2(BU) = mathbbZ$ play? This is a statement about homotopy classes of loops $Omega^2(BU)$ but in the considerations above we haven't passed to homotopy classes so here we would "lose" some information.



      Does anybody see the correct argument? Thanks in advance.










      share|cite|improve this question











      $endgroup$




      I have a question about an argument that occurred in the discussion about consequences of Bott periodicity in A Concise Course in Algebraic Topology by P. May on page 207. Here is the excerpt:




      Could anybody explain the "little argument with $H$-spaces" which May has in mind to show that $Omega^2(BU times mathbbZ) $ is equivalent to $(Omega^2_0BU) times mathbbZ$ as $H$-spaces?




      My considerations: As explained above the loop space "sees" only the component of the base point so $Omega^2BU= Omega^2_0BU$.



      The problem reduces to two questions:



      Does $Omega^2$ respect products like $pi_k(-)$?



      And which role does the fact $pi_2(BU) = mathbbZ$ play? This is a statement about homotopy classes of loops $Omega^2(BU)$ but in the considerations above we haven't passed to homotopy classes so here we would "lose" some information.



      Does anybody see the correct argument? Thanks in advance.







      general-topology algebraic-topology homology-cohomology topological-k-theory loop-spaces






      share|cite|improve this question















      share|cite|improve this question













      share|cite|improve this question




      share|cite|improve this question








      edited Mar 23 at 8:51









      Andrews

      1,2812423




      1,2812423










      asked Mar 23 at 0:51









      KarlPeterKarlPeter

      6551316




      6551316




















          1 Answer
          1






          active

          oldest

          votes


















          1












          $begingroup$

          The loop functor $Omega$ is defined on a space $X$ as $Omega X=Map_*(S^1,X)$. For compactly generated spaces you combine the adjunction homeomorphism $Map_*(S^1,Map_*(S^1,X))cong Map(S^1wedge S^1,X)$ with $S^1wedge S^1cong S^2$ and iterate to get a homeomorphism



          $$Omega^kXcong Map_*(S^k,X).$$



          In fact many people would take this as the definition of $Omega^k$, and use the previous isomorphisms backwards to identify



          $$Omega(Omega^k-1)congOmega^k.$$



          Anyway, the point is that for a space $X$ you literally have



          $$pi_k(X)congpi_0(Omega^kX)$$



          for each $kgeq 0$. Moreover if $Y$ is another compactly generated space then you also have



          $$Omega^k(Xtimes Y)=Map_*(S^k,X^ktimes Y)cong Map_*(S^k,X)times Map_*(S^k,Y)=Omega^k XtimesOmega^k Y$$



          and this follows from the properties of the mapping functor. May discusses these adjunctions in Chapter 5 Compactly Generated Spaces.



          Now the statement you are interested in is actually something more general. What May is referencing is the the fact that




          If $X$ is any grouplike H-space with a homotopy associative multiplication, then there is a homotopy equivalence $$Xsimeq X_0timespi_0X$$ where $X_0$ denotes the path component of $X$ containing the basepoint. Moreover, this equivalence is one of $H$-spaces if $X$ is homotopy commutative.




          I'll discuss this general case below but you can apply it to your case as follows. I'll shortly give a definition for "grouplike", and you will see that any loop space is grouplike. Since a loop space is also homotopy associative - and a double loop space is homotopy commutative - we can apply the above to $Omega^2(BUtimesmathbbZ)$ to solve your problem.



          Start by observing that $pi_2(BUtimesmathbbZ)congpi_2(BU)opluspi_2(mathbbZ)congpi_2(BU)congmathbbZ$ since $pi_2BU_1congpi_2K(mathbbZ,2)congmathbbZ$ and $BU_1rightarrow BU$ is 3-connected. This means that



          $$pi_0(Omega^2(BUtimesmathbbZ))congpi_2(BUtimesmathbbZ)congmathbbZ.$$



          The basepoint in $Omega^2(BUtimesmathbbZ)$ is the constant loop $S^2rightarrow BUtimesmathbbZ$, $tmapsto (ast,0)$ which is contained in $Omega^2_0BUcong Omega^2_0(BU)times0subseteqOmega^2(BU)timesOmega^2(mathbbZ)congOmega^2(BUtimesmathbbZ)$. Hence we have from the above that



          $$Omega^2(BUtimesmathbbZ)simeq Omega^2_0(BUtimesmathbbZ)timespi_0(Omega^2(BUtimesmathbbZ))congOmega^2_0BUtimesmathbbZ$$



          as H-spaces, as claimed by May.



          Now, onto the discussion. An H-space $(X,m)$ is said to be grouplike if $pi_0X$ becomes a group under the operation induced by the multiplication $m$. Clearly this holds when $Xsimeq Omega X'$ is a loop space, since in this case $pi_0Xcongpi_0(Omega X')congpi_1X'$ is a group.



          To see that the operation induced by $m$ coincides with the loop addition you must use the fact that $m$ extends the fold map $nabla:Xvee Xrightarrow X$, and the comutiplication $c:S^1rightarrow S^1vee S^1$, which induces the loop sum, lifts the diagonal $S^1rightarrow S^1times S^1$. If you do not see this immediately I urge you to draw a diagram, taking loops $k,l:S^1rightarrow X$ and forming the coposite $mcirc(ktimes l)circDelta$ on the top row, and the composite $nablacirc(kvee l)circ c$ on the bottom.



          Now to prove the theorem, let us take a homotopy associative, grouplike H-space $X$ with multiplication $m$. Choose a representative $x_g$ for each coset in $pi_0$, making sure to pick the H-space unit $ast$ for the basepoint component. Now form the map



          $$Psi:X_0timespi_0Xrightarrow X$$



          by setting



          $$Psi(x,[x_g])=m(x,x_g):=xcdot x_g.$$



          We claim that this map is a homotopy equivalence. Indeed, it has an inverse $Theta:Xrightarrow X_0timespi_0X$ which we define as follows. Assume $xin X$ lies in $[x_g]inpi_0X$. Then since $pi_0X$ is a group the inverse $[x_g]^-1$ exists and we have $[x_g]^-1=[x_h]$ for some $x_hin X$. Set



          $$Theta(x)=(xcdot x_h,x_g).$$



          Clearly $[xcdot x_h]=[x_gcdot x_h]=[x_g]cdot[x_h]=[ast]$, so $xcdot x_h$ indeed lies in $X_0$ and we take the above as the definition of $Theta$.



          We have



          $$PsicircTheta(x)=Psi(xcdot x_h,x_g)=(xcdot x_h)cdot x_gsimeq xcdot(x_gcdot x_h)$$



          and since $[x_h]=[xcdot x_g]^-1=[x_g]^-1$ we have $[x_gcdot x_h]=[ast]$ and get a homotopy $psicircThetasimeq id$ by choosing a path from $x_gcdot x_h$ to the identity for each index. Similarly we find that $ThetacircPsisimeq id$.



          If in addition we assume that the multiplication on $X$ is homotopy commutative then we find



          $$Psi((x,[x_g])cdot(y,[x_h]))=Psi(xcdot y,[x_g][x_h])=Psi(xcdot y,[x_gx_h])=(xcdot y))cdot x_k$$



          where $[x_gcdot x_h]=[x_k]$. Continuing on we get



          $$(xcdot y)cdot x_ksimeq (xcdot y)cdot (x_gcdot x_h)simeq(xcdot (ycdot x_g))cdot x_hsimeq (xcdot (x_gcdot y))cdot x_hsimeq(xcdot x_g)cdot (ycdot y_h)$$



          where we have used the canonical homotopy associativity and commutativity of $m$. But this last expression is exactly $Psi(x,[x_g])cdot Psi(y,[x_h])$. Hence we have



          $$Psi(-cdot-)simeq Psi(-)cdotPsi(-)$$



          showing that $Psi$ is an equivalence of H-spaces. I'll leave you to check the last couple of details.






          share|cite|improve this answer









          $endgroup$













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            $begingroup$

            The loop functor $Omega$ is defined on a space $X$ as $Omega X=Map_*(S^1,X)$. For compactly generated spaces you combine the adjunction homeomorphism $Map_*(S^1,Map_*(S^1,X))cong Map(S^1wedge S^1,X)$ with $S^1wedge S^1cong S^2$ and iterate to get a homeomorphism



            $$Omega^kXcong Map_*(S^k,X).$$



            In fact many people would take this as the definition of $Omega^k$, and use the previous isomorphisms backwards to identify



            $$Omega(Omega^k-1)congOmega^k.$$



            Anyway, the point is that for a space $X$ you literally have



            $$pi_k(X)congpi_0(Omega^kX)$$



            for each $kgeq 0$. Moreover if $Y$ is another compactly generated space then you also have



            $$Omega^k(Xtimes Y)=Map_*(S^k,X^ktimes Y)cong Map_*(S^k,X)times Map_*(S^k,Y)=Omega^k XtimesOmega^k Y$$



            and this follows from the properties of the mapping functor. May discusses these adjunctions in Chapter 5 Compactly Generated Spaces.



            Now the statement you are interested in is actually something more general. What May is referencing is the the fact that




            If $X$ is any grouplike H-space with a homotopy associative multiplication, then there is a homotopy equivalence $$Xsimeq X_0timespi_0X$$ where $X_0$ denotes the path component of $X$ containing the basepoint. Moreover, this equivalence is one of $H$-spaces if $X$ is homotopy commutative.




            I'll discuss this general case below but you can apply it to your case as follows. I'll shortly give a definition for "grouplike", and you will see that any loop space is grouplike. Since a loop space is also homotopy associative - and a double loop space is homotopy commutative - we can apply the above to $Omega^2(BUtimesmathbbZ)$ to solve your problem.



            Start by observing that $pi_2(BUtimesmathbbZ)congpi_2(BU)opluspi_2(mathbbZ)congpi_2(BU)congmathbbZ$ since $pi_2BU_1congpi_2K(mathbbZ,2)congmathbbZ$ and $BU_1rightarrow BU$ is 3-connected. This means that



            $$pi_0(Omega^2(BUtimesmathbbZ))congpi_2(BUtimesmathbbZ)congmathbbZ.$$



            The basepoint in $Omega^2(BUtimesmathbbZ)$ is the constant loop $S^2rightarrow BUtimesmathbbZ$, $tmapsto (ast,0)$ which is contained in $Omega^2_0BUcong Omega^2_0(BU)times0subseteqOmega^2(BU)timesOmega^2(mathbbZ)congOmega^2(BUtimesmathbbZ)$. Hence we have from the above that



            $$Omega^2(BUtimesmathbbZ)simeq Omega^2_0(BUtimesmathbbZ)timespi_0(Omega^2(BUtimesmathbbZ))congOmega^2_0BUtimesmathbbZ$$



            as H-spaces, as claimed by May.



            Now, onto the discussion. An H-space $(X,m)$ is said to be grouplike if $pi_0X$ becomes a group under the operation induced by the multiplication $m$. Clearly this holds when $Xsimeq Omega X'$ is a loop space, since in this case $pi_0Xcongpi_0(Omega X')congpi_1X'$ is a group.



            To see that the operation induced by $m$ coincides with the loop addition you must use the fact that $m$ extends the fold map $nabla:Xvee Xrightarrow X$, and the comutiplication $c:S^1rightarrow S^1vee S^1$, which induces the loop sum, lifts the diagonal $S^1rightarrow S^1times S^1$. If you do not see this immediately I urge you to draw a diagram, taking loops $k,l:S^1rightarrow X$ and forming the coposite $mcirc(ktimes l)circDelta$ on the top row, and the composite $nablacirc(kvee l)circ c$ on the bottom.



            Now to prove the theorem, let us take a homotopy associative, grouplike H-space $X$ with multiplication $m$. Choose a representative $x_g$ for each coset in $pi_0$, making sure to pick the H-space unit $ast$ for the basepoint component. Now form the map



            $$Psi:X_0timespi_0Xrightarrow X$$



            by setting



            $$Psi(x,[x_g])=m(x,x_g):=xcdot x_g.$$



            We claim that this map is a homotopy equivalence. Indeed, it has an inverse $Theta:Xrightarrow X_0timespi_0X$ which we define as follows. Assume $xin X$ lies in $[x_g]inpi_0X$. Then since $pi_0X$ is a group the inverse $[x_g]^-1$ exists and we have $[x_g]^-1=[x_h]$ for some $x_hin X$. Set



            $$Theta(x)=(xcdot x_h,x_g).$$



            Clearly $[xcdot x_h]=[x_gcdot x_h]=[x_g]cdot[x_h]=[ast]$, so $xcdot x_h$ indeed lies in $X_0$ and we take the above as the definition of $Theta$.



            We have



            $$PsicircTheta(x)=Psi(xcdot x_h,x_g)=(xcdot x_h)cdot x_gsimeq xcdot(x_gcdot x_h)$$



            and since $[x_h]=[xcdot x_g]^-1=[x_g]^-1$ we have $[x_gcdot x_h]=[ast]$ and get a homotopy $psicircThetasimeq id$ by choosing a path from $x_gcdot x_h$ to the identity for each index. Similarly we find that $ThetacircPsisimeq id$.



            If in addition we assume that the multiplication on $X$ is homotopy commutative then we find



            $$Psi((x,[x_g])cdot(y,[x_h]))=Psi(xcdot y,[x_g][x_h])=Psi(xcdot y,[x_gx_h])=(xcdot y))cdot x_k$$



            where $[x_gcdot x_h]=[x_k]$. Continuing on we get



            $$(xcdot y)cdot x_ksimeq (xcdot y)cdot (x_gcdot x_h)simeq(xcdot (ycdot x_g))cdot x_hsimeq (xcdot (x_gcdot y))cdot x_hsimeq(xcdot x_g)cdot (ycdot y_h)$$



            where we have used the canonical homotopy associativity and commutativity of $m$. But this last expression is exactly $Psi(x,[x_g])cdot Psi(y,[x_h])$. Hence we have



            $$Psi(-cdot-)simeq Psi(-)cdotPsi(-)$$



            showing that $Psi$ is an equivalence of H-spaces. I'll leave you to check the last couple of details.






            share|cite|improve this answer









            $endgroup$

















              1












              $begingroup$

              The loop functor $Omega$ is defined on a space $X$ as $Omega X=Map_*(S^1,X)$. For compactly generated spaces you combine the adjunction homeomorphism $Map_*(S^1,Map_*(S^1,X))cong Map(S^1wedge S^1,X)$ with $S^1wedge S^1cong S^2$ and iterate to get a homeomorphism



              $$Omega^kXcong Map_*(S^k,X).$$



              In fact many people would take this as the definition of $Omega^k$, and use the previous isomorphisms backwards to identify



              $$Omega(Omega^k-1)congOmega^k.$$



              Anyway, the point is that for a space $X$ you literally have



              $$pi_k(X)congpi_0(Omega^kX)$$



              for each $kgeq 0$. Moreover if $Y$ is another compactly generated space then you also have



              $$Omega^k(Xtimes Y)=Map_*(S^k,X^ktimes Y)cong Map_*(S^k,X)times Map_*(S^k,Y)=Omega^k XtimesOmega^k Y$$



              and this follows from the properties of the mapping functor. May discusses these adjunctions in Chapter 5 Compactly Generated Spaces.



              Now the statement you are interested in is actually something more general. What May is referencing is the the fact that




              If $X$ is any grouplike H-space with a homotopy associative multiplication, then there is a homotopy equivalence $$Xsimeq X_0timespi_0X$$ where $X_0$ denotes the path component of $X$ containing the basepoint. Moreover, this equivalence is one of $H$-spaces if $X$ is homotopy commutative.




              I'll discuss this general case below but you can apply it to your case as follows. I'll shortly give a definition for "grouplike", and you will see that any loop space is grouplike. Since a loop space is also homotopy associative - and a double loop space is homotopy commutative - we can apply the above to $Omega^2(BUtimesmathbbZ)$ to solve your problem.



              Start by observing that $pi_2(BUtimesmathbbZ)congpi_2(BU)opluspi_2(mathbbZ)congpi_2(BU)congmathbbZ$ since $pi_2BU_1congpi_2K(mathbbZ,2)congmathbbZ$ and $BU_1rightarrow BU$ is 3-connected. This means that



              $$pi_0(Omega^2(BUtimesmathbbZ))congpi_2(BUtimesmathbbZ)congmathbbZ.$$



              The basepoint in $Omega^2(BUtimesmathbbZ)$ is the constant loop $S^2rightarrow BUtimesmathbbZ$, $tmapsto (ast,0)$ which is contained in $Omega^2_0BUcong Omega^2_0(BU)times0subseteqOmega^2(BU)timesOmega^2(mathbbZ)congOmega^2(BUtimesmathbbZ)$. Hence we have from the above that



              $$Omega^2(BUtimesmathbbZ)simeq Omega^2_0(BUtimesmathbbZ)timespi_0(Omega^2(BUtimesmathbbZ))congOmega^2_0BUtimesmathbbZ$$



              as H-spaces, as claimed by May.



              Now, onto the discussion. An H-space $(X,m)$ is said to be grouplike if $pi_0X$ becomes a group under the operation induced by the multiplication $m$. Clearly this holds when $Xsimeq Omega X'$ is a loop space, since in this case $pi_0Xcongpi_0(Omega X')congpi_1X'$ is a group.



              To see that the operation induced by $m$ coincides with the loop addition you must use the fact that $m$ extends the fold map $nabla:Xvee Xrightarrow X$, and the comutiplication $c:S^1rightarrow S^1vee S^1$, which induces the loop sum, lifts the diagonal $S^1rightarrow S^1times S^1$. If you do not see this immediately I urge you to draw a diagram, taking loops $k,l:S^1rightarrow X$ and forming the coposite $mcirc(ktimes l)circDelta$ on the top row, and the composite $nablacirc(kvee l)circ c$ on the bottom.



              Now to prove the theorem, let us take a homotopy associative, grouplike H-space $X$ with multiplication $m$. Choose a representative $x_g$ for each coset in $pi_0$, making sure to pick the H-space unit $ast$ for the basepoint component. Now form the map



              $$Psi:X_0timespi_0Xrightarrow X$$



              by setting



              $$Psi(x,[x_g])=m(x,x_g):=xcdot x_g.$$



              We claim that this map is a homotopy equivalence. Indeed, it has an inverse $Theta:Xrightarrow X_0timespi_0X$ which we define as follows. Assume $xin X$ lies in $[x_g]inpi_0X$. Then since $pi_0X$ is a group the inverse $[x_g]^-1$ exists and we have $[x_g]^-1=[x_h]$ for some $x_hin X$. Set



              $$Theta(x)=(xcdot x_h,x_g).$$



              Clearly $[xcdot x_h]=[x_gcdot x_h]=[x_g]cdot[x_h]=[ast]$, so $xcdot x_h$ indeed lies in $X_0$ and we take the above as the definition of $Theta$.



              We have



              $$PsicircTheta(x)=Psi(xcdot x_h,x_g)=(xcdot x_h)cdot x_gsimeq xcdot(x_gcdot x_h)$$



              and since $[x_h]=[xcdot x_g]^-1=[x_g]^-1$ we have $[x_gcdot x_h]=[ast]$ and get a homotopy $psicircThetasimeq id$ by choosing a path from $x_gcdot x_h$ to the identity for each index. Similarly we find that $ThetacircPsisimeq id$.



              If in addition we assume that the multiplication on $X$ is homotopy commutative then we find



              $$Psi((x,[x_g])cdot(y,[x_h]))=Psi(xcdot y,[x_g][x_h])=Psi(xcdot y,[x_gx_h])=(xcdot y))cdot x_k$$



              where $[x_gcdot x_h]=[x_k]$. Continuing on we get



              $$(xcdot y)cdot x_ksimeq (xcdot y)cdot (x_gcdot x_h)simeq(xcdot (ycdot x_g))cdot x_hsimeq (xcdot (x_gcdot y))cdot x_hsimeq(xcdot x_g)cdot (ycdot y_h)$$



              where we have used the canonical homotopy associativity and commutativity of $m$. But this last expression is exactly $Psi(x,[x_g])cdot Psi(y,[x_h])$. Hence we have



              $$Psi(-cdot-)simeq Psi(-)cdotPsi(-)$$



              showing that $Psi$ is an equivalence of H-spaces. I'll leave you to check the last couple of details.






              share|cite|improve this answer









              $endgroup$















                1












                1








                1





                $begingroup$

                The loop functor $Omega$ is defined on a space $X$ as $Omega X=Map_*(S^1,X)$. For compactly generated spaces you combine the adjunction homeomorphism $Map_*(S^1,Map_*(S^1,X))cong Map(S^1wedge S^1,X)$ with $S^1wedge S^1cong S^2$ and iterate to get a homeomorphism



                $$Omega^kXcong Map_*(S^k,X).$$



                In fact many people would take this as the definition of $Omega^k$, and use the previous isomorphisms backwards to identify



                $$Omega(Omega^k-1)congOmega^k.$$



                Anyway, the point is that for a space $X$ you literally have



                $$pi_k(X)congpi_0(Omega^kX)$$



                for each $kgeq 0$. Moreover if $Y$ is another compactly generated space then you also have



                $$Omega^k(Xtimes Y)=Map_*(S^k,X^ktimes Y)cong Map_*(S^k,X)times Map_*(S^k,Y)=Omega^k XtimesOmega^k Y$$



                and this follows from the properties of the mapping functor. May discusses these adjunctions in Chapter 5 Compactly Generated Spaces.



                Now the statement you are interested in is actually something more general. What May is referencing is the the fact that




                If $X$ is any grouplike H-space with a homotopy associative multiplication, then there is a homotopy equivalence $$Xsimeq X_0timespi_0X$$ where $X_0$ denotes the path component of $X$ containing the basepoint. Moreover, this equivalence is one of $H$-spaces if $X$ is homotopy commutative.




                I'll discuss this general case below but you can apply it to your case as follows. I'll shortly give a definition for "grouplike", and you will see that any loop space is grouplike. Since a loop space is also homotopy associative - and a double loop space is homotopy commutative - we can apply the above to $Omega^2(BUtimesmathbbZ)$ to solve your problem.



                Start by observing that $pi_2(BUtimesmathbbZ)congpi_2(BU)opluspi_2(mathbbZ)congpi_2(BU)congmathbbZ$ since $pi_2BU_1congpi_2K(mathbbZ,2)congmathbbZ$ and $BU_1rightarrow BU$ is 3-connected. This means that



                $$pi_0(Omega^2(BUtimesmathbbZ))congpi_2(BUtimesmathbbZ)congmathbbZ.$$



                The basepoint in $Omega^2(BUtimesmathbbZ)$ is the constant loop $S^2rightarrow BUtimesmathbbZ$, $tmapsto (ast,0)$ which is contained in $Omega^2_0BUcong Omega^2_0(BU)times0subseteqOmega^2(BU)timesOmega^2(mathbbZ)congOmega^2(BUtimesmathbbZ)$. Hence we have from the above that



                $$Omega^2(BUtimesmathbbZ)simeq Omega^2_0(BUtimesmathbbZ)timespi_0(Omega^2(BUtimesmathbbZ))congOmega^2_0BUtimesmathbbZ$$



                as H-spaces, as claimed by May.



                Now, onto the discussion. An H-space $(X,m)$ is said to be grouplike if $pi_0X$ becomes a group under the operation induced by the multiplication $m$. Clearly this holds when $Xsimeq Omega X'$ is a loop space, since in this case $pi_0Xcongpi_0(Omega X')congpi_1X'$ is a group.



                To see that the operation induced by $m$ coincides with the loop addition you must use the fact that $m$ extends the fold map $nabla:Xvee Xrightarrow X$, and the comutiplication $c:S^1rightarrow S^1vee S^1$, which induces the loop sum, lifts the diagonal $S^1rightarrow S^1times S^1$. If you do not see this immediately I urge you to draw a diagram, taking loops $k,l:S^1rightarrow X$ and forming the coposite $mcirc(ktimes l)circDelta$ on the top row, and the composite $nablacirc(kvee l)circ c$ on the bottom.



                Now to prove the theorem, let us take a homotopy associative, grouplike H-space $X$ with multiplication $m$. Choose a representative $x_g$ for each coset in $pi_0$, making sure to pick the H-space unit $ast$ for the basepoint component. Now form the map



                $$Psi:X_0timespi_0Xrightarrow X$$



                by setting



                $$Psi(x,[x_g])=m(x,x_g):=xcdot x_g.$$



                We claim that this map is a homotopy equivalence. Indeed, it has an inverse $Theta:Xrightarrow X_0timespi_0X$ which we define as follows. Assume $xin X$ lies in $[x_g]inpi_0X$. Then since $pi_0X$ is a group the inverse $[x_g]^-1$ exists and we have $[x_g]^-1=[x_h]$ for some $x_hin X$. Set



                $$Theta(x)=(xcdot x_h,x_g).$$



                Clearly $[xcdot x_h]=[x_gcdot x_h]=[x_g]cdot[x_h]=[ast]$, so $xcdot x_h$ indeed lies in $X_0$ and we take the above as the definition of $Theta$.



                We have



                $$PsicircTheta(x)=Psi(xcdot x_h,x_g)=(xcdot x_h)cdot x_gsimeq xcdot(x_gcdot x_h)$$



                and since $[x_h]=[xcdot x_g]^-1=[x_g]^-1$ we have $[x_gcdot x_h]=[ast]$ and get a homotopy $psicircThetasimeq id$ by choosing a path from $x_gcdot x_h$ to the identity for each index. Similarly we find that $ThetacircPsisimeq id$.



                If in addition we assume that the multiplication on $X$ is homotopy commutative then we find



                $$Psi((x,[x_g])cdot(y,[x_h]))=Psi(xcdot y,[x_g][x_h])=Psi(xcdot y,[x_gx_h])=(xcdot y))cdot x_k$$



                where $[x_gcdot x_h]=[x_k]$. Continuing on we get



                $$(xcdot y)cdot x_ksimeq (xcdot y)cdot (x_gcdot x_h)simeq(xcdot (ycdot x_g))cdot x_hsimeq (xcdot (x_gcdot y))cdot x_hsimeq(xcdot x_g)cdot (ycdot y_h)$$



                where we have used the canonical homotopy associativity and commutativity of $m$. But this last expression is exactly $Psi(x,[x_g])cdot Psi(y,[x_h])$. Hence we have



                $$Psi(-cdot-)simeq Psi(-)cdotPsi(-)$$



                showing that $Psi$ is an equivalence of H-spaces. I'll leave you to check the last couple of details.






                share|cite|improve this answer









                $endgroup$



                The loop functor $Omega$ is defined on a space $X$ as $Omega X=Map_*(S^1,X)$. For compactly generated spaces you combine the adjunction homeomorphism $Map_*(S^1,Map_*(S^1,X))cong Map(S^1wedge S^1,X)$ with $S^1wedge S^1cong S^2$ and iterate to get a homeomorphism



                $$Omega^kXcong Map_*(S^k,X).$$



                In fact many people would take this as the definition of $Omega^k$, and use the previous isomorphisms backwards to identify



                $$Omega(Omega^k-1)congOmega^k.$$



                Anyway, the point is that for a space $X$ you literally have



                $$pi_k(X)congpi_0(Omega^kX)$$



                for each $kgeq 0$. Moreover if $Y$ is another compactly generated space then you also have



                $$Omega^k(Xtimes Y)=Map_*(S^k,X^ktimes Y)cong Map_*(S^k,X)times Map_*(S^k,Y)=Omega^k XtimesOmega^k Y$$



                and this follows from the properties of the mapping functor. May discusses these adjunctions in Chapter 5 Compactly Generated Spaces.



                Now the statement you are interested in is actually something more general. What May is referencing is the the fact that




                If $X$ is any grouplike H-space with a homotopy associative multiplication, then there is a homotopy equivalence $$Xsimeq X_0timespi_0X$$ where $X_0$ denotes the path component of $X$ containing the basepoint. Moreover, this equivalence is one of $H$-spaces if $X$ is homotopy commutative.




                I'll discuss this general case below but you can apply it to your case as follows. I'll shortly give a definition for "grouplike", and you will see that any loop space is grouplike. Since a loop space is also homotopy associative - and a double loop space is homotopy commutative - we can apply the above to $Omega^2(BUtimesmathbbZ)$ to solve your problem.



                Start by observing that $pi_2(BUtimesmathbbZ)congpi_2(BU)opluspi_2(mathbbZ)congpi_2(BU)congmathbbZ$ since $pi_2BU_1congpi_2K(mathbbZ,2)congmathbbZ$ and $BU_1rightarrow BU$ is 3-connected. This means that



                $$pi_0(Omega^2(BUtimesmathbbZ))congpi_2(BUtimesmathbbZ)congmathbbZ.$$



                The basepoint in $Omega^2(BUtimesmathbbZ)$ is the constant loop $S^2rightarrow BUtimesmathbbZ$, $tmapsto (ast,0)$ which is contained in $Omega^2_0BUcong Omega^2_0(BU)times0subseteqOmega^2(BU)timesOmega^2(mathbbZ)congOmega^2(BUtimesmathbbZ)$. Hence we have from the above that



                $$Omega^2(BUtimesmathbbZ)simeq Omega^2_0(BUtimesmathbbZ)timespi_0(Omega^2(BUtimesmathbbZ))congOmega^2_0BUtimesmathbbZ$$



                as H-spaces, as claimed by May.



                Now, onto the discussion. An H-space $(X,m)$ is said to be grouplike if $pi_0X$ becomes a group under the operation induced by the multiplication $m$. Clearly this holds when $Xsimeq Omega X'$ is a loop space, since in this case $pi_0Xcongpi_0(Omega X')congpi_1X'$ is a group.



                To see that the operation induced by $m$ coincides with the loop addition you must use the fact that $m$ extends the fold map $nabla:Xvee Xrightarrow X$, and the comutiplication $c:S^1rightarrow S^1vee S^1$, which induces the loop sum, lifts the diagonal $S^1rightarrow S^1times S^1$. If you do not see this immediately I urge you to draw a diagram, taking loops $k,l:S^1rightarrow X$ and forming the coposite $mcirc(ktimes l)circDelta$ on the top row, and the composite $nablacirc(kvee l)circ c$ on the bottom.



                Now to prove the theorem, let us take a homotopy associative, grouplike H-space $X$ with multiplication $m$. Choose a representative $x_g$ for each coset in $pi_0$, making sure to pick the H-space unit $ast$ for the basepoint component. Now form the map



                $$Psi:X_0timespi_0Xrightarrow X$$



                by setting



                $$Psi(x,[x_g])=m(x,x_g):=xcdot x_g.$$



                We claim that this map is a homotopy equivalence. Indeed, it has an inverse $Theta:Xrightarrow X_0timespi_0X$ which we define as follows. Assume $xin X$ lies in $[x_g]inpi_0X$. Then since $pi_0X$ is a group the inverse $[x_g]^-1$ exists and we have $[x_g]^-1=[x_h]$ for some $x_hin X$. Set



                $$Theta(x)=(xcdot x_h,x_g).$$



                Clearly $[xcdot x_h]=[x_gcdot x_h]=[x_g]cdot[x_h]=[ast]$, so $xcdot x_h$ indeed lies in $X_0$ and we take the above as the definition of $Theta$.



                We have



                $$PsicircTheta(x)=Psi(xcdot x_h,x_g)=(xcdot x_h)cdot x_gsimeq xcdot(x_gcdot x_h)$$



                and since $[x_h]=[xcdot x_g]^-1=[x_g]^-1$ we have $[x_gcdot x_h]=[ast]$ and get a homotopy $psicircThetasimeq id$ by choosing a path from $x_gcdot x_h$ to the identity for each index. Similarly we find that $ThetacircPsisimeq id$.



                If in addition we assume that the multiplication on $X$ is homotopy commutative then we find



                $$Psi((x,[x_g])cdot(y,[x_h]))=Psi(xcdot y,[x_g][x_h])=Psi(xcdot y,[x_gx_h])=(xcdot y))cdot x_k$$



                where $[x_gcdot x_h]=[x_k]$. Continuing on we get



                $$(xcdot y)cdot x_ksimeq (xcdot y)cdot (x_gcdot x_h)simeq(xcdot (ycdot x_g))cdot x_hsimeq (xcdot (x_gcdot y))cdot x_hsimeq(xcdot x_g)cdot (ycdot y_h)$$



                where we have used the canonical homotopy associativity and commutativity of $m$. But this last expression is exactly $Psi(x,[x_g])cdot Psi(y,[x_h])$. Hence we have



                $$Psi(-cdot-)simeq Psi(-)cdotPsi(-)$$



                showing that $Psi$ is an equivalence of H-spaces. I'll leave you to check the last couple of details.







                share|cite|improve this answer












                share|cite|improve this answer



                share|cite|improve this answer










                answered Mar 23 at 15:14









                TyroneTyrone

                5,31711226




                5,31711226



























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