Quantum
Prelocality No-Go Theorems and Exactly Solvable Relational History Hamiltonians
Publication: quant-ph updates on arXiv.org
Author: Maxim V. Churilov
Source published: 14/10/2026, 04:00:00 UTC
Briefing created: 25/10/2026, 20:12:44 UTC
Based on a feed excerpt; full article content has not been acquired. Source evidence retrieved 14/10/2026, 12:17:25 UTC.
Briefings
Research presents two exactly solvable relational history Hamiltonians: a cyclic clock with a unique ground state and a fixed-weight control penalty architecture. The clock model yields a gap scaling as $\Delta_{N,L}/E_* = \pi^2/(2L^2)-2\pi^2/L^3+O(L^{-4})$ independent of vertex count, while the alternative architecture achieves a size-independent gap of $E_*(1-1/\sqrt{2})$. These results establish finite resource tradeoffs between locality and clock resources but do not prove an emergent geometric phase.
Key points
- A cyclic clock with a reversible incidence update has a unique ground state.
- The gap of the clock model scales as $\Delta_{N,L}/E_* = \pi^2/(2L^2)-2\pi^2/L^3+O(L^{-4})$ independent of vertex count.
Context
This study provides exact finite results for relational history Hamiltonians, contrasting a cyclic clock model with a fixed-weight control penalty architecture. The findings offer quantitative tradeoffs between locality and clock resources without establishing an emergent geometric phase.
Limitations
The evidence is limited to two specific Hamiltonian models; no additional background on the broader field is supplied. Results are preprint status (arXiv:2610.14081v1) with uncertainty regarding the exact nature of the gap scaling and the absence of a geometric phase.
Generated by Bittrees-hosted qwen35-2b sha256:aaf42c8b7c3c on 25/10/2026, 20:12:44 UTC. Based on publisher-provided feed evidence; may not cover the full original article. Check the source for details.
View archived briefing on IPFS
bafybeihksjij7jgaoxecod23phlvzzas45pizt633dyrm7xogxrjkgzhoe