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基于相位的伊辛机中的星形旋节边界

Astroid Spinodal Boundary in Phase-Based Ising Machines

Malihe Farasat, Nikhil Shukla

arXiv 2607.26213首次发表:更新:

AI 中文总结

该研究揭示振荡器与动力学伊辛机中,二次谐波注入和网络场的竞争通过星形旋节边界实现单双稳态转变,其势垒标度规律与Stoner–Wohlfarth能量存在关联。

AI 中文摘要

振荡器伊辛机(OIMs)和动力学伊辛机(DIMs)通过二次谐波注入(SHI)稳定的相位态编码二元自旋。在耦合网络中,SHI与瞬时局部网络场的竞争会重塑每个振荡器的条件能量景观。我们表明,这种竞争通过星形旋节边界驱动单稳态和双稳态区域之间的转变。在该边界附近,势垒在一般光滑点处满足ΔE_i∝μ_i^(3/2),在纵向尖点处满足ΔE_i∝μ_i^2。OIMs和DIMs遵循相同的旋节几何,其条件景观通过横向场的反转相关。最后,一次谐波条件景观在相差一个加性常数的情况下,数学上等价于单轴磁性粒子的Stoner–Wohlfarth能量。

英文摘要

Oscillator Ising machines (OIMs) and dynamical Ising machines (DIMs) encode binary spins in phase states stabilized by second-harmonic injection (SHI). In a coupled network, the competition between SHI and the instantaneous local network field reshapes each oscillator's conditional energy landscape. We show that this competition drives a transition between monostable and bistable regimes through an astroid spinodal boundary. Near this boundary, the barrier scales as $ΔE_i\proptoμ_i^{3/2}$ at generic smooth points and as $ΔE_i\proptoμ_i^{2}$ at the longitudinal cusp. OIMs and DIMs obey the same spinodal geometry, with their conditional landscapes related by a reversal of the transverse field. Finally, the first-harmonic conditional landscape is mathematically equivalent, up to an additive constant, to the Stoner--Wohlfarth energy of a uniaxial magnetic particle.

论文原文

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