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Mar 25, 2013 at 9:51 comment added Wouter Stekelenburg To see that $\pi_0: L\to X$ is a monomorphism, consider its kernel pair $l,r:Z\to L\times L$. Now $\pi_0\circ l =\pi_0\circ r$ by definition, and $\pi_1\circ l = \pi_1\circ r$ by uv), because the morphism $(\pi_0\circ l,\pi_1\circ l,\pi_1\circ r): Z\to X\times Y\times Y$ represents the subobject $\{ (x,y,y')| \lambda(x,y)\land\lambda(x,y') \}$. Because $\pi_i\circ l = \pi_i\circ r$, $l=r$. To conclude: every parallel pair $f,g:W\to L$ such that $\pi_0\circ f= \pi_0\circ g$ factors uniquely through $l,r$. Therefore every such pair satisfies $f=g$.
Jun 27, 2012 at 17:54 comment added Wouter Stekelenburg Left exact functors preserve posets, and $\Omega_F$ is an internal poset in $\mathcal F$. The lattice structures of $\mathcal E(X\times Y,f_*\Omega)$ and $\mathcal F(f^*X\times f^*Y,\Omega)$ coincide because they are the result of applying naturally isomorphic left exact functors -- $\mathcal E(X\times Y,f_*-)$ and $\mathcal F(f^*X\times f^*Y,−)$ -- to the same poset. This equivalence in natural in $X$ and $Y$. Now joins have a universal property relative in terms of the order, and therefore must commute with the isomorphism.
Jun 27, 2012 at 11:41 history edited Wouter Stekelenburg CC BY-SA 3.0
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Jun 26, 2012 at 21:35 history edited Wouter Stekelenburg CC BY-SA 3.0
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Jun 25, 2012 at 21:28 history edited Wouter Stekelenburg CC BY-SA 3.0
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Jun 25, 2012 at 8:09 history answered Wouter Stekelenburg CC BY-SA 3.0