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Jul 26, 2010 at 20:47 answer added Willie Wong timeline score: 0
Jul 26, 2010 at 17:37 comment added tamir OK I understand this, but I'm still not sure how do I demonstrate that $ g^N $ would be diagonal. Intuitively - Suppose I have a "vertical vector" $ a \in M \subset N $ then in the local coordinates you showed me $ g^N * a $ as a matrix operating on a vector, should give me a vector which is in $ T_a N $ but not in $ T_a M $ And this shows that the matrix elements "*" would have to be zero. But again, this is intuitive, from linear algebra. Can you please help me to understand this delicate point? thanks for the time, Tamir
Jul 26, 2010 at 0:29 answer added Greg Kuperberg timeline score: 1
Jul 26, 2010 at 0:22 comment added Willie Wong (Of course when you do this you have to be careful when you compute the curvature; beware of taking additional vertical derivatives!)
Jul 26, 2010 at 0:19 comment added Willie Wong You don't need * to be all zero. You just need it to be zero along $M$. So just take an arbitrary local coordinate on $M$ to start. The metric defines along $M$ the normal direction. Choose a field of normal vectors, extend the field arbitrarily in a thickened slab around $M$. Flow $M$ along the vector field. Then the flow $t$ gives the "vertical coordinate". The lie transport of the local coordinates on $M$ gives the coordinate on the slab. And along $M$ the total metric $g^N$ is block diagonal.
Jul 26, 2010 at 0:06 history asked tamir CC BY-SA 2.5