ECF360A3D482
For each $n\geq 2$, the bowl is the entire graph $z=f(r)$, $r=|x|$ in $\mathbb R^ n$, moving by $z\mapsto z+t$. Its radial profile is specified by the regular ODE
This is an ODE characterization, not an elementary closed formula.
The bowl is complete, properly embedded, strictly convex, rotationally invariant, and diffeomorphic to $\mathbb R^ n$. For $n\geq 2$ it has one topological end and gives an eternal flow.
Up to a vertical additive constant, its height has asymptotic expansion
\[ f(r)=\frac{r^2}{2(n-1)}-\log r+C+O(r^{-1})\quad (r\to \infty ). \]A paraboloid is only a leading approximation, not the exact translator.
It is unique among entire rotationally invariant translating graphs, up to translation. In $\mathbb R^3$ it is the only complete entire translating graph, up to the natural rigid motions and normalization.
In $\mathbb R^3$, Brendle–Choi's theorem characterizes its flow among noncompact, strictly convex, noncollapsed ancient flows, up to scaling and ambient isometries. These are the hypotheses of the cited classification.
Graphical weighted stability holds. The stronger dynamical stability theorem of Clutterbuck–Schnürer–Schulze concerns continuous graphical initial data whose height difference from the bowl tends to zero at spatial infinity; the resulting height difference tends uniformly to zero as time tends to infinity.
The supplied notes [HIMWNotes19], Section 4 and Theorem 4.1, PDF pages 10–11, describe the construction and classification. The original ODE and asymptotic analysis is [CSS07], Section 2, Lemmas 2.1–2.2; its Theorem 1.1 gives the stated dynamical stability. The ancient classification is [BrendleChoi19], Theorem 1.1, printed page 36 (PDF page 2). The entropy is $\lambda (\mathrm{Bowl}^ n)=\lambda (S^{n-1}(\sqrt{2(n-1)}))$, in particular $\sqrt{2\pi /e}$ in $\mathbb R^3$. This follows from [SunWang2025], Example 3.6 and Corollary 2.4 with Lemma 2.5, PDF pp. 8–11; it is not an identity for the fixed-center Gaussian area of the bowl.
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