Earth-centered inertial

In size theory, the natural pseudodistance between two size pairs $(M,\phi :M\to \mathbb{ℝ})$, $(N,\psi :N\to \mathbb{ℝ})$ is the value ${\inf }_h\Vert \phi -\psi \circ h{\Vert }_{\mathrm{\infty }}$, where $h$ varies in the set of all homeomorphisms from the manifold $M$ to the manifold $N$ and $\Vert \cdot {\Vert }_{\mathrm{\infty }}$ is the supremum norm. If $M$ and $N$ are not homeomorphic, then the natural pseudodistance is defined to be $\mathrm{\infty }$. It is usually assumed that $M$, $N$ are $C^1$ closed manifolds and the measuring functions $\phi ,\psi$ are $C^1$. Put another way, the natural pseudodistance measures the infimum of the change of the measuring function induced by the homeomorphisms from $M$ to $N$.

The concept of natural pseudodistance can be easily extended to size pairs where the measuring function $\phi$ takes values in ${\mathbb{ℝ}}^m$ .

Main properties

It can be proved that the natural pseudodistance always equals the Euclidean distance between two critical values of the measuring functions (possibly, of the same measuring function) divided by a suitable positive integer $k$. If $M$ and $N$ are surfaces, the number $k$ can be assumed to be $1$, $2$ or $3$. If $M$ and $N$ are curves, the number $k$ can be assumed to be $1$ or $2$. If an optimal homeomorphism $\overline{h}$ exists (i.e., $\Vert \phi -\psi \circ \overline{h}{\Vert }_{\mathrm{\infty }}={\inf }_h\Vert \phi -\psi \circ h{\Vert }_{\mathrm{\infty }}$), then $k$ can be assumed to be $1$.

See also

• Fréchet distance
• Size function
• Size functor
• Size homotopy group

References

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