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Jul 19, 2013 at 3:24 history edited Craig CC BY-SA 3.0
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Jul 18, 2013 at 21:36 comment added Craig Igor, I am not sure of the correct way of saying this in words... $w_\lambda(x)$ is a dilated version of $w(x)$ and one can check that $-\Delta w_\lambda(x)=w_\lambda(x)^p$. Also $ w_1(x)=w(x)$ and hence taking derivative in $ \lambda$ and setting $ \lambda=1$ shows that $ \partial_\lambda w_\lambda(x)|_{\lambda=1}$ is in the kernel of $L$. I was confused as to whether it was independent of the other terms.
Jul 18, 2013 at 21:31 comment added Craig Michael. Thanks, that is a nice way to see it.
Jul 18, 2013 at 20:22 comment added Igor Khavkine Honestly, I'm having trouble following your definition of $\phi_{N+1}$. However, it sounds like you mean the result of the dilation operator acting on the solution $w$. If that's the case, then all of these $\phi_i$ should be in the kernel of $L$. This should follow from the general fact that symmetry generators acting on solutions create linearized solutions, which is fairly straight forward to work out for yourself.
Jul 18, 2013 at 19:33 comment added Michael Renardy It is easy to see that $\phi_{N+1}$ cannot be a linear combination of the others. Note that $\phi_{N+1}$ is radially symmetric, and all the others have zero average over the sphere.
Jul 18, 2013 at 19:01 history asked Craig CC BY-SA 3.0