S.O.S. Mathematics CyberBoard

Your Resource for mathematics help on the web!
It is currently Wed, 22 May 2013 00:47:58 UTC

All times are UTC [ DST ]




Post new topic Reply to topic  [ 8 posts ] 
Author Message
 Post subject: Construction versus existence?
PostPosted: Tue, 4 Oct 2011 19:55:59 UTC 
Online
Moderator
User avatar

Joined: Wed, 30 Mar 2005 04:25:14 UTC
Posts: 12098
Location: Austin, TX
I'm given a function f:S\to\mathbb{R} and I'm asked to show every function g:S\to\mathbb{R} is measurable relative to (\sigma(f),\mathcal{B}(\mathbb{R})) iff \exists h:\mathbb{R}\to\mathbb{R} which is measurable relative to \mathcal{B}(\mathbb{R}) and g=f^*(h). One direction is trivial since the composition of measurable functions is measurable. Intuitively it makes sense as well, but I'm a little stuck on the other.

I know by definition g measurable in the sense indicated means \forall A\in\mathcal{B}(\mathbb{R})\;\exists A'\in\mathcal{B}(\mathbb{R}) such that g^{-1}(A)=f^{-1}(A').

And I feel it must only be a hop, skip, and a jump away from actually defining an h with this relation since point fibers partition off the domain, S, however I cannot quite see how to do it, so I think perhaps there is something sneakier I can do, such as letting \mathcal{A} be the family of all g such that the condition holds and somehow show it must be everything by appealing to some property of \sigma(f) or f^*, but I cannot see how to quite work this one.

Partial construction (?):

Consider the partition of S formed by $\coprod_{x\in\mathbb{R}} g^{-1}(\{x\}) where I throw out empty sets as irrelevant. Then \forall x\exists A_x\in\mathcal{B}(\mathbb{R}) such that g^{-1}(\{x\})=f^{-1}(A_x), and because fibers commute with unions, we have: $g^{-1}(\{x\})=\bigcup_{y\in A_x}f^{-1}(\{y\}), then I somehow get a partition of S by doing this for all points x\in\mathbb{R} and disjointifying the A_x by taking sufficient complements (which is fine, since we have a \sigma-algebra) and somehow producing h from this by demanding h(g^{-1}(\{x\}))\in A_x or even just h(g^{-1}(\{x\}))=y for some choice of y\in A_x which must be nonempty if g^{-1}(\{x\}) is. The axiom of choice should ensure that this works. Does this function as a workable argument? It feels a bit ad-hoc, but who knows. Any help appreciated.

_________________
(\ /)
(O.o)
(> <)
This is Bunny. Copy Bunny into your signature to help him on his way to world domination


Top
 Profile  
 
 Post subject: Re: Construction versus existence?
PostPosted: Tue, 4 Oct 2011 23:39:52 UTC 
Offline
Moderator
User avatar

Joined: Mon, 29 Dec 2008 17:49:32 UTC
Posts: 6007
Location: 127.0.0.1, ::1 (avatar courtesy of UDN)
Shadow wrote:
I'm given a function f:S\to\mathbb{R} and I'm asked to show every function g:S\to\mathbb{R} is measurable relative to (\sigma(f),\mathcal{B}(\mathbb{R})) iff \exists h:\mathbb{R}\to\mathbb{R} which is measurable relative to \mathcal{B}(\mathbb{R}) and g=f^*(h). One direction is trivial since the composition of measurable functions is measurable. Intuitively it makes sense as well, but I'm a little stuck on the other.

I know by definition g measurable in the sense indicated means \forall A\in\mathcal{B}(\mathbb{R})\;\exists A'\in\mathcal{B}(\mathbb{R}) such that g^{-1}(A)=f^{-1}(A').

And I feel it must only be a hop, skip, and a jump away from actually defining an h with this relation since point fibers partition off the domain, S, however I cannot quite see how to do it, so I think perhaps there is something sneakier I can do, such as letting \mathcal{A} be the family of all g such that the condition holds and somehow show it must be everything by appealing to some property of \sigma(f) or f^*, but I cannot see how to quite work this one.

Partial construction (?):

Consider the partition of S formed by $\coprod_{x\in\mathbb{R}} g^{-1}(\{x\}) where I throw out empty sets as irrelevant. Then \forall x\exists A_x\in\mathcal{B}(\mathbb{R}) such that g^{-1}(\{x\})=f^{-1}(A_x), and because fibers commute with unions, we have: $g^{-1}(\{x\})=\bigcup_{y\in A_x}f^{-1}(\{y\}), then I somehow get a partition of S by doing this for all points x\in\mathbb{R} and disjointifying the A_x by taking sufficient complements (which is fine, since we have a \sigma-algebra) and somehow producing h from this by demanding h(g^{-1}(\{x\}))\in A_x or even just h(g^{-1}(\{x\}))=y for some choice of y\in A_x which must be nonempty if g^{-1}(\{x\}) is. The axiom of choice should ensure that this works. Does this function as a workable argument? It feels a bit ad-hoc, but who knows. Any help appreciated.


No AC is needed, and you don't actually want to consider g^{-1} all that much. You can just construct h via a limit argument using the standard dyadic trick --- construct approximations h_n of h corresponding to approximations g_n=2^{-n}\lfloor 2^ng\rfloor of g, and then take the limit of h_n. There are a couple of traps along the way for the unenlightened.

Trap 1:
Spoiler:
You need to make sure you choose pairwise disjoint sets before you try to define h_n on those sets.


Trap 2:
Spoiler:
You need to make sure \lim h_n behaves, and doesn't spoil g=f^*h.


The procedure in detail:
Spoiler:
The sets A_{j,n}=\{\lfloor 2^ng\rfloor=j\}, for j\in\mathbb{Z} and fixed n, partitions S into disjoint subsets using \sigma(f). Let B_{j,n}\in\mathcal{B}(\mathbb{R}) such that f^{-1}(B_{j,n})=A_{j,n}. Now B_{j,n} may not be pairwise disjoint, but you can replace them with B^*_{j,n}=B_{j,n}\cap(\bigcup_{i\neq j}B_{i,n})^c which are pairwise disjoint Borels (remember for fixed n) with f^{-1}(B^*_{j,n})=A_{j,n}. Hence we have approximations
h_n(t)=
\begin{cases}
j2^{-n} & t\in B^*_{j,n}\text{ for some }j\\
0 & \text{otherwise}
\end{cases}.
Obviously h_n is Borel-measurable, so the set B=\{t\in\mathbb{R}\mid\lim_{n\to\infty}h_n(t)\text{ exists and is finite}\} is also Borel, hence
h(t)=
\begin{cases}
\lim h_n(t) & t\in B\\
0 & \text{otherwise}
\end{cases}
is Borel. All that remains is to check that f(S)\subseteq B, which is easy.


Edit: typo corrected.

_________________
\begin{aligned}
Spin(1)&=O(1)=\mathbb{Z}/2&\quad&\text{and}\\
Spin(2)&=U(1)=SO(2)&&\text{are obvious}\\
Spin(3)&=Sp(1)=SU(2)&&\text{by }q\mapsto(\mathop{\mathrm{Im}}\mathbb{H}\ni p\mapsto qp\bar{q})\\
Spin(4)&=Sp(1)\times Sp(1)&&\text{by }(q_1,q_2)\mapsto(\mathbb{H}\ni p\mapsto q_1p\bar{q_2})\\
Spin(5)&=Sp(2)&&\text{by }\mathbb{HP}^1\cong S^4_{round}\hookrightarrow\mathbb{R}^5\\
Spin(6)&=SU(4)&&\text{by the irrep }\Lambda_+\mathbb{C}^4
\end{aligned}


Top
 Profile  
 
 Post subject: Re: Construction versus existence?
PostPosted: Wed, 5 Oct 2011 23:08:59 UTC 
Online
Moderator
User avatar

Joined: Wed, 30 Mar 2005 04:25:14 UTC
Posts: 12098
Location: Austin, TX
outermeasure wrote:
Shadow wrote:
I'm given a function f:S\to\mathbb{R} and I'm asked to show every function g:S\to\mathbb{R} is measurable relative to (\sigma(f),\mathcal{B}(\mathbb{R})) iff \exists h:\mathbb{R}\to\mathbb{R} which is measurable relative to \mathcal{B}(\mathbb{R}) and g=f^*(h). One direction is trivial since the composition of measurable functions is measurable. Intuitively it makes sense as well, but I'm a little stuck on the other.

I know by definition g measurable in the sense indicated means \forall A\in\mathcal{B}(\mathbb{R})\;\exists A'\in\mathcal{B}(\mathbb{R}) such that g^{-1}(A)=f^{-1}(A').

And I feel it must only be a hop, skip, and a jump away from actually defining an h with this relation since point fibers partition off the domain, S, however I cannot quite see how to do it, so I think perhaps there is something sneakier I can do, such as letting \mathcal{A} be the family of all g such that the condition holds and somehow show it must be everything by appealing to some property of \sigma(f) or f^*, but I cannot see how to quite work this one.

Partial construction (?):

Consider the partition of S formed by $\coprod_{x\in\mathbb{R}} g^{-1}(\{x\}) where I throw out empty sets as irrelevant. Then \forall x\exists A_x\in\mathcal{B}(\mathbb{R}) such that g^{-1}(\{x\})=f^{-1}(A_x), and because fibers commute with unions, we have: $g^{-1}(\{x\})=\bigcup_{y\in A_x}f^{-1}(\{y\}), then I somehow get a partition of S by doing this for all points x\in\mathbb{R} and disjointifying the A_x by taking sufficient complements (which is fine, since we have a \sigma-algebra) and somehow producing h from this by demanding h(g^{-1}(\{x\}))\in A_x or even just h(g^{-1}(\{x\}))=y for some choice of y\in A_x which must be nonempty if g^{-1}(\{x\}) is. The axiom of choice should ensure that this works. Does this function as a workable argument? It feels a bit ad-hoc, but who knows. Any help appreciated.


No AC is needed, and you don't actually want to consider g^{-1} all that much. You can just construct h via a limit argument using the standard dyadic trick --- construct approximations h_n of h corresponding to approximations g_n=2^{-n}\lfloor 2^ng\rfloor of g, and then take the limit of h_n. There are a couple of traps along the way for the unenlightened.

Trap 1:
Spoiler:
You need to make sure you choose pairwise disjoint sets before you try to define h_n on those sets.


Trap 2:
Spoiler:
You need to make sure \lim h_n behaves, and doesn't spoil g=f^*h.


The procedure in detail:
Spoiler:
The sets A_{j,n}=\{\lfloor 2^ng\rfloor=j\}, for j\in\mathbb{Z} and fixed n, partitions S into disjoint subsets using \sigma(f). Let B_{j,n}\in\mathcal{B}(\mathbb{R}) such that g^{-1}(B_{j,n})=A_{j,n}. Now B_{j,n} may not be pairwise disjoint, but you can replace them with B^*_{j,n}=B_{j,n}\cap(\bigcup_{i\neq j}B_{i,n})^c which are pairwise disjoint Borels (remember for fixed n) with g^{-1}(B^*_{j,n})=A_{j,n}. Hence we have approximations
h_n(t)=
\begin{cases}
j2^{-n} & t\in B^*_{j,n}\text{ for some }j\\
0 & \text{otherwise}
\end{cases}.
Obviously h_n is Borel-measurable, so the set B=\{t\in\mathbb{R}\mid\lim_{n\to\infty}h_n(t)\text{ exists and is finite}\} is also Borel, hence
h(t)=
\begin{cases}
\lim h_n(t) & t\in B\\
0 & \text{otherwise}
\end{cases}
is Borel. All that remains is to check that f(S)\subseteq B, which is easy.


OK, so I think I mostly understand this, but in your notation: why should the B_{j,n} not be disjoint? It looks like it will just be sets like [{k\over 2^n},{k+1\over 2^n}) which ought to be disjoint. And why f(S)\subseteq B is still somewhat eluding me. Also, I wrote this with characteristic functions instead of a piecewise definition, presumably that's all good and kosher? In particular I have $h(x)=\lim_{n\to\infty} \chi_{_B}h_n(x).

Thanks again.

_________________
(\ /)
(O.o)
(> <)
This is Bunny. Copy Bunny into your signature to help him on his way to world domination


Top
 Profile  
 
 Post subject: Re: Construction versus existence?
PostPosted: Wed, 5 Oct 2011 23:14:51 UTC 
Offline
Moderator
User avatar

Joined: Mon, 29 Dec 2008 17:49:32 UTC
Posts: 6007
Location: 127.0.0.1, ::1 (avatar courtesy of UDN)
Shadow wrote:
OK, so I think I mostly understand this, but in your notation: why should the B_{j,n} not be disjoint? It looks like it will just be sets like [{k\over 2^n},{k+1\over 2^n}) which ought to be disjoint. And why f(S)\subseteq B is still somewhat eluding me. Also, I wrote this with characteristic functions instead of a piecewise definition, presumably that's all good and kosher? In particular I have $h(x)=\lim_{n\to\infty} \chi_{_B}h_n(x).

Thanks again.


Oops, some of the g should be f, corrected.

_________________
\begin{aligned}
Spin(1)&=O(1)=\mathbb{Z}/2&\quad&\text{and}\\
Spin(2)&=U(1)=SO(2)&&\text{are obvious}\\
Spin(3)&=Sp(1)=SU(2)&&\text{by }q\mapsto(\mathop{\mathrm{Im}}\mathbb{H}\ni p\mapsto qp\bar{q})\\
Spin(4)&=Sp(1)\times Sp(1)&&\text{by }(q_1,q_2)\mapsto(\mathbb{H}\ni p\mapsto q_1p\bar{q_2})\\
Spin(5)&=Sp(2)&&\text{by }\mathbb{HP}^1\cong S^4_{round}\hookrightarrow\mathbb{R}^5\\
Spin(6)&=SU(4)&&\text{by the irrep }\Lambda_+\mathbb{C}^4
\end{aligned}


Top
 Profile  
 
 Post subject: Re: Construction versus existence?
PostPosted: Wed, 5 Oct 2011 23:23:36 UTC 
Online
Moderator
User avatar

Joined: Wed, 30 Mar 2005 04:25:14 UTC
Posts: 12098
Location: Austin, TX
And how do we know the disjointification still gives us full image A_{j,n}? This one I feel must be obvious, but I'm missing it.

EDIT: Ignore that, inverse images commute with intersections, I get it.

_________________
(\ /)
(O.o)
(> <)
This is Bunny. Copy Bunny into your signature to help him on his way to world domination


Top
 Profile  
 
 Post subject: Re: Construction versus existence?
PostPosted: Wed, 5 Oct 2011 23:31:58 UTC 
Offline
Moderator
User avatar

Joined: Mon, 29 Dec 2008 17:49:32 UTC
Posts: 6007
Location: 127.0.0.1, ::1 (avatar courtesy of UDN)
Shadow wrote:
And how do we know the disjointification still gives us full image A_{j,n}? This one I feel must be obvious, but I'm missing it.


Recall inverse image behaves under unions, complements, and intersections, so
\begin{aligned}
f^{-1}(B_{j,n}\cap(\bigcup_{i\neq j} B_{i,n})^c)&=f^{-1}(B_{j,n})\cap(\bigcup_{i\neq j} f^{-1}B_{i,n})^c\\
&=A_{j,n}\cap(\bigcup_{i\neq j} A_{i,n})^c\\
&=A_{j,n}
\end{aligned}.

The condition f(S)\subseteq B means at every point of f(S) the h_n has a finite limit, which follows from \lim f^*h_n(s)=\lim h_n(f(s))=\lim g_n(s)=g(s) for all s\in S.

_________________
\begin{aligned}
Spin(1)&=O(1)=\mathbb{Z}/2&\quad&\text{and}\\
Spin(2)&=U(1)=SO(2)&&\text{are obvious}\\
Spin(3)&=Sp(1)=SU(2)&&\text{by }q\mapsto(\mathop{\mathrm{Im}}\mathbb{H}\ni p\mapsto qp\bar{q})\\
Spin(4)&=Sp(1)\times Sp(1)&&\text{by }(q_1,q_2)\mapsto(\mathbb{H}\ni p\mapsto q_1p\bar{q_2})\\
Spin(5)&=Sp(2)&&\text{by }\mathbb{HP}^1\cong S^4_{round}\hookrightarrow\mathbb{R}^5\\
Spin(6)&=SU(4)&&\text{by the irrep }\Lambda_+\mathbb{C}^4
\end{aligned}


Top
 Profile  
 
 Post subject: Re: Construction versus existence?
PostPosted: Wed, 5 Oct 2011 23:32:46 UTC 
Online
Moderator
User avatar

Joined: Wed, 30 Mar 2005 04:25:14 UTC
Posts: 12098
Location: Austin, TX
outermeasure wrote:
Shadow wrote:
And how do we know the disjointification still gives us full image A_{j,n}? This one I feel must be obvious, but I'm missing it.


Recall inverse image behaves under unions, complements, and intersections, so f^{-1}(B_{j,n}\cap(\bigcup B_{i,n})^c)=f^{-1}(B_{j,n})\cap(\bigcup f^{-1}B_{i,n})^c=A_{j,n}\cap(\bigcup A_{i,n})^c=A_{j,n}.

The condition f(S)\subseteq B means at every point of f(S) the h_n has a finite limit, which follows from \lim f^*h_n(s)=\lim h_n(f(s))=\lim g_n(s)=g(s) for all s\in S.


Ah, just changed it too. Sorry about that. Thanks for the f(S)\subseteq B though, that was still eluding me.

_________________
(\ /)
(O.o)
(> <)
This is Bunny. Copy Bunny into your signature to help him on his way to world domination


Top
 Profile  
 
 Post subject: Re: Construction versus existence?
PostPosted: Wed, 5 Oct 2011 23:50:03 UTC 
Offline
Moderator
User avatar

Joined: Mon, 29 Dec 2008 17:49:32 UTC
Posts: 6007
Location: 127.0.0.1, ::1 (avatar courtesy of UDN)
Essentially the same proof gives the following version:

Suppose X=(X,\mathcal{X}) and Y=(Y,\mathcal{Y}) are measurable space, Z a complete separable metric space (actually a Polish space would do, we don't care too much about the metric) with the Borel \sigma-algebra, f\colon X\to Y measurable which induces the sigma algebra \mathcal{X}_0 on Y. Then a Z-valued (\mathcal{Y},\mathcal{B}(Z))-measurable function g is (\mathcal{X}_0,\mathcal{B}(Z))-measurable if and only if there exists measurable function h\colon(Y,\mathcal{B})\to(Z,\mathcal{B}(Z)) such that g(x)=h(f(x)) for all x\in X.

_________________
\begin{aligned}
Spin(1)&=O(1)=\mathbb{Z}/2&\quad&\text{and}\\
Spin(2)&=U(1)=SO(2)&&\text{are obvious}\\
Spin(3)&=Sp(1)=SU(2)&&\text{by }q\mapsto(\mathop{\mathrm{Im}}\mathbb{H}\ni p\mapsto qp\bar{q})\\
Spin(4)&=Sp(1)\times Sp(1)&&\text{by }(q_1,q_2)\mapsto(\mathbb{H}\ni p\mapsto q_1p\bar{q_2})\\
Spin(5)&=Sp(2)&&\text{by }\mathbb{HP}^1\cong S^4_{round}\hookrightarrow\mathbb{R}^5\\
Spin(6)&=SU(4)&&\text{by the irrep }\Lambda_+\mathbb{C}^4
\end{aligned}


Top
 Profile  
 
Display posts from previous:  Sort by  
Post new topic Reply to topic  [ 8 posts ] 

All times are UTC [ DST ]


Who is online

Users browsing this forum: No registered users


You cannot post new topics in this forum
You cannot reply to topics in this forum
You cannot edit your posts in this forum
You cannot delete your posts in this forum

Search for:
Jump to:  
Contact Us | S.O.S. Mathematics Homepage
Privacy Statement | Search the "old" CyberBoard

users online during the last hour
Powered by phpBB © 2001, 2005-2011 phpBB Group.
Copyright © 1999-2013 MathMedics, LLC. All rights reserved.
Math Medics, LLC. - P.O. Box 12395 - El Paso TX 79913 - USA