NANAOCPSMar 30

Critical phase transitions in minimum-energy configurations for the exponential kernel family $e^{-|x-y|^q}$ on the unit interval

arXiv:2603.2817940.0h-index: 1
Predicted impact top 27% in NA · last 90 daysOriginality Incremental advance
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This addresses a theoretical problem in mathematical physics and optimization, focusing on kernel interpolation and energy minimization, with incremental contributions to understanding phase transitions in such systems.

The paper tackles the problem of optimal point placement on a unit interval for exponential kernels, identifying critical phase transitions where configurations shift from collision-free to endpoint-collapsed as the parameter q varies, with exact and numerical transition values provided for different numbers of points.

We study the optimal placement of $k$ ordered points on the unit interval for the bounded pair potential \[ K_q(d)=e^{-d^q}, \qquad q>0. \] The family interpolates between strongly cusp-like kernels for $0<q<1$, the threshold kernel $e^{-d}$, and the flatter Gaussian-type regime $q>1$. Our emphasis is on the transition from collision-free minimizers to endpoint-collapsed minimizers. We reformulate the problem in gap variables, record convexity, symmetry, and the Karush-Kuhn-Tucker conditions, and give a short proof that collisions are impossible for $0<q<1$. At the threshold $q=1$ we recover the endpoint-clustering law for $e^{-d}$, while for $q>1$ we identify critical exponents $q_k$ beyond which interior points are no longer optimal. For odd $k$ we derive the exact universal value \[ q_{2m+1} = \frac{\log(1/(-\log((1+e^{-1})/2)))}{\log 2} \approx 1.396363475, \] and for even $k=4,6,\dots,20$ we compute the numerical transition values \[ \begin{aligned} &q_4\approx 1.062682507,\quad q_6\approx 1.155601329,\quad q_8\approx 1.206132611,\quad q_{10}\approx 1.238523533,\\ &q_{12}\approx 1.261308114,\quad q_{14}\approx 1.278305167,\quad q_{16}\approx 1.291510874,\quad q_{18}\approx 1.302082885,\\ &q_{20}\approx 1.310744185. \end{aligned} \] We also include comparison tables and diagrams for the kernels $e^{-\sqrt d}$, $e^{-d}$, and $e^{-d^2}$, briefly relate the bounded family to the singular Riesz kernel $d^{-s}$, and identify the $q\to 0^+$ limit with the Fekete/Chebyshev--Lobatto configuration on $[0,1]$.

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