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# Classical motion emerges from a sum over paths
## What it is (established result)
In the **Feynman path integral** (sum-over-histories) formulation of quantum
mechanics, the transition amplitude from an initial configuration to a final
configuration is obtained by summing contributions from **all possible paths**
connecting them. Each path contributes a complex phase determined by the
classical action \(S[x(t)]\):
\[
\langle x_f, t_f \mid x_i, t_i \rangle
\;=\;
\int \mathcal{D}x(t)\;
\exp\!\left(\frac{i}{\hbar} S[x(t)]\right).
\]
In the semiclassical (small-\(\hbar\)) regime, the dominant contribution comes
from paths near those for which the action is stationary (\(\delta S = 0\)),
recovering the **classical equations of motion** via the principle of least
action \([1,2]\).
---
## How RRT / RST uses it
RST uses the path-integral idea as an **engineering pattern**:
- The substrate does not “know” a single correct future. It can be modelled as
evaluating many candidate micro-updates (paths) and selecting the realised
update under a finite budget.
- The classical trajectory corresponds to the update history that maximises
delivered identity / fidelity for minimal workload cost (least relational
friction under A5-like constraints).
In code this becomes a **parallel-search update rule**: sample many candidate
micro-updates, score each by a fidelity-per-cost functional, and pick the
realised event. (See the `Reality Engine` application for the runnable toy
implementation.)
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## Links
| Role | Link |
|:---|:---|
| Simulator application | [[further applications/Reality Engine/Reality Engine (RST)]] |
| Simulator code | [[further applications/Reality Engine/Reality Engine - Code]] |
---
## References
[1] R. P. Feynman, "Space-Time Approach to Non-Relativistic Quantum Mechanics," *Reviews of Modern Physics* **20**, 367–387 (1948), `https://doi.org/10.1103/RevModPhys.20.367`.
[2] R. P. Feynman and A. R. Hibbs, *Quantum Mechanics and Path Integrals*, McGraw–Hill, 1965.