The phase-shift formula for multi-block box-ball systems

Let a box-ball system have nn blocks, with QkQ_k balls in the kk-th block, and suppose the blocks are separated sufficiently so that the asymptotic soliton structure can be identified by ordering (Qk)k=1n(Q_k)_{k=1}^n. After sufficiently many time steps, once all collisions have finished, the phase-shift conjecture. The total phase shift experienced by the kk-th block is

2j>k\Qj<Qkmin(Qj,Qk)2j<k\Qj>Qkmin(Qj,Qk).2\sum_{\substack{j>k\Q_j<Q_k}} \min(Q_j,Q_k)-2\sum_{\substack{j<k\Q_j>Q_k}} \min(Q_j,Q_k).

In particular, if Q1>Q2>>QnQ_1>Q_2>\cdots>Q_n, then the phase shift experienced by the kk-th block is

2j>kmin(Qj,Qk)2j<kmin(Qj,Qk).2\sum_{j>k} \min(Q_j,Q_k)-2\sum_{j<k} \min(Q_j,Q_k).

This extends the two-block phase-shift calculation and proposes the expected cumulative contribution of every collision; its general validity remains open in the source.

Sources & referencesView supporting material

Primary source

Nicholas M. Ercolani and Jonathan Ramalheira-Tsu, “The Ghost-Box-Ball System: A Unified Perspective on Soliton Cellular Automata, the RSK Algorithm and Phase Shifts”, arXiv:2101.07896 (2021).

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