Loading…
Loading…
comment
Classical Derivative, Weak Derivative and Integration by Parts
According to the distribution definition of the weak derivative of an $L^1_{loc}$ function, you have with $\phi\in C^\infty_c(U)$ $$ \langle \nabla_w f,\phi\rangle_{\mathscr D'(U),\mathscr D(U)}=-\int f \nabla \phi dx. $$ On the other hand you assume that the function $f$ is differentiable on $U$ with gradient $\nabla f$. Now the formulation of your question is not really meaningful: $\nabla_w f$ is defined weakly whereas $\nabla f$ has a point wise definition. So the meaning of equality or difference on a set of positive measure does not mean anything.
Loading…
Loading…
Loading…
comment
Hormander's bracket condition for the adjoint of an operator
Yes, Hörmander's ALPDO, Chapter 22.
Loading…
comment
An invariant method of stationary phase
You are certainly right that my notations are poorly chosen: it is indeed true that $c$ can depend on $t$, via the value of $\psi$ at the critical points. Again think about multiplying everything by $e^{it}$.
comment
Lagrangean uniqueness versus Eulerian uniqueness
@Luis Silvestre Thanks for your remarks. I certainly agree with the fact that the quoted paper by Ambrosio \& Bernard does not solve my question. The problem seems to come from the definition of the product of a measure by a measurable function, always possible in measure theory, but not in distribution theory. In particular, the definition of a weak solution for a PDE is indeed using distribution theory, with a formal integration by parts.
Loading…
Loading…
comment
An invariant method of stationary phase
The $e^{it\psi}$ must be there: the value of the phase at a critical point has to be taken into account. Imagine that you multiply everything by $i$. The signature is invariantly defined as well as the square root of the determinant, which is a half-density et the critical set.
comment
An invariant method of stationary phase
The notation $\vert \psi''(x)\vert^{1/2}$ means $$ \vert\det \psi''(x)\vert^{1/2}. $$
comment
An invariant method of stationary phase
The $c$ in my answer is, assuming $\phi=-i\psi$, $\psi$ real-valued Morse function $$ c=\sum_{x\in supp u,d\psi(x)=0}e^{it\psi(x)}\frac{e^{i\frac{\pi}{4}sign \psi''(x)}}{\vert \psi''(x)\vert^{1/2}} u(x), $$ a coordinate-free expression. Note that $sign \psi''(x)$ stands for the signature of the quadratic form $\psi''(x)$, that is the number of positive eigenvalues minus the number of negative eigenvalues. The sum above is finite by compactness of $supp u$.
Loading…
Loading…
comment
Differential equations and axiom of choice
The Cauchy-Lipschitz theorem in french or in any other language is dealing with the case where $f$ is locally Lipschitz continuous with respect to $x$, i.e. satisfies an estimate of type $$ \vert f(t,x_1)-f(t,x_2)\vert\le \alpha(t) \vert x_1-x_2\vert, $$ with $\alpha \in L^1_{loc}$. In that case, local uniqueness occurs for the ODE.
comment
Approximating a function by fractional powers
$f_\epsilon$ is an entire function, thus can be approximated uniformly by polynomials on compact sets.
Loading…