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Landauer Cost of a Self-Model
Laflamme-3T Conjecture - Path 3 Step 2 - Feasibility Gate
Abstract
Before pursuing physical instantiation of AC-1, we must verify that a self-referential entropy-reducing system is thermodynamically feasible given available technology. This document derives the minimum power required to maintain a self-model, computes it across a range of parameters, and delivers a verdict on which research paths to pursue.
1. Landauer's Principle
Landauer's Principle (1961), proven experimentally by Bérut et al. (2012):
At room temperature (T = 293 K): Eerase ≥ 2.805 × 10-21 J/bit. No physical process can erase one bit of information for less energy than this. This is a proven physical law, not an approximation.
Application to a Self-Model
A self-model of Kolmogorov complexity K bits must be erased and rewritten on every update cycle. The minimum continuous power is:
This is the thermodynamic floor — technology-independent. Real implementations exceed this by an overhead factor η.
2. Technology Efficiency Spectrum
| Technology | η | Notes |
|---|---|---|
| Theoretical minimum | 1× | Landauer limit |
| Advanced reversible logic (~2040) | 10× | Research stage |
| Adiabatic CMOS (~2035) | 102× | Near-future |
| Biological brain | 103× | ~20 W for ~1016 synaptic ops/s |
| Neuromorphic (IBM TrueNorth) | 104× | State of art 2025 |
| Current silicon (CMOS) | 106× | ~10-15 J/op |
| Typical desktop | 108× | Commodity hardware |
3. Computed Power Requirements
Pmin ≈ 2.8 × 10-14 W. At current silicon (η = 106): ~28 nW.
Pmin ≈ 280 nW. At current silicon: ~280 W. At neuromorphic: ~2.8 mW.
Pmin ≈ 280 μW. At current silicon: ~280 kW. At neuromorphic: ~2.8 W. At biological efficiency: ~280 mW.
4. Biological Baseline
| Property | Value |
|---|---|
| Total metabolic power | ≈ 20 W |
| Number of neurons | ≈ 86 billion |
| Number of synapses | ≈ 100 trillion |
| Efficiency vs. Landauer | ≈ 103–104× |
The brain operates at roughly 103–104× the Landauer limit — far more efficient than current silicon. Most brain energy is spent on ion transport, not computation.
5. The Self-Referential Extension
For a self-referential system, the full power expression becomes:
For a well-calibrated self-model where ΔIself ≈ K, the self-referential penalty is at most a factor of 2 over the naive Landauer cost. It does not change the order-of-magnitude analysis.