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Prove of the shape-derivative identity relating the shape and material derivative of a shape-dependent function
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Prove of the shape-derivative identity relating the shape and material derivative of a shape-dependent function
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revised
Prove of the shape-derivative identity relating the shape and material derivative of a shape-dependent function
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Prove of the shape-derivative identity relating the shape and material derivative of a shape-dependent function
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Prove of the shape-derivative identity relating the shape and material derivative of a shape-dependent function
This is probably me being silly, but isn't the second definition just the first one with $E_\Omega=L^1(\Omega)$ for all $\Omega\in \mathcal{A}$? Is there a difference beyond the space in which you take the limit?
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RKHS norm of Lipschitz functions
What's your definition of a RKHS? I think the usual one is just "a Hilbert space of functions on a set whose evaluation functionals are norm continuous", no?
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RKHS norm of Lipschitz functions
What happens when $\mathcal{X}=\mathbb{Z}$ and $\mathcal{H}=l^2$?
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Combinatorics of multivariate Faà di Bruno formula
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Isometries and complex differentials
Just a suggestion, but I think you might want to think about what you're taking as the codomains of $\partial$ and $\bar \partial$, and in what sense you want to be taking derivatives (assuming that's what $\partial$ and $\bar \partial$ stand for that is).
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Bound the operator norm of the Fréchet derivative of a Lipschitz function in this setting
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Bound the operator norm of the Fréchet derivative of a Lipschitz function in this setting
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Bound the operator norm of the Fréchet derivative of a Lipschitz function in this setting
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Bound the operator norm of the Fréchet derivative of a Lipschitz function in this setting
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Bound the operator norm of the Fréchet derivative of a Lipschitz function in this setting
NB: I'm using $\mathrm{limsup}_{y\to x}(*)$ to mean $\mathrm{lim}_{r\to 0}(\sup_{y\in \mathrm{Ball}(x,r)\setminus\{x\}}(*))$
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What is the analog of the symmetrized Jacobi matrix for delay equations?
This isn't my area, so I do apologise if I'm speaking out of turn, but... the construction you introduce To make it possible to talk about volumes doesn't seem at all to me like a natural step from what you're talking about at the start of your question. Is your main interest in evolution of volumes in $\mathbb{R}^d$ or are you more interested in abstract analogs of the Liouville trace formula?
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Useful notion for locally convex spaces - well known?
Have you considered whether Dini/Lipschitz continuity might be more what you're after here?