Encyclopedia Condensed Condensed Matter Strongly Correlated Electrons Structure Strongly Correlated Ele

ARTICLE 3 claims 2 theorems 1 model

Condensed Matter Strongly Correlated Electrons Structure Strongly Correlated Ele

A machine-checked theorem links the mathematics of strongly correlated electrons to the structural physics of glass transitions, without deriving any specific material property.

The structural bridge

In condensed matter physics, strongly correlated electrons are electrons whose mutual repulsion is so large that they cannot be treated as independent particles moving in a fixed background. Their collective behavior produces phenomena like high-temperature superconductivity and exotic magnetism, and it is notoriously hard to model. The Recognition Science framework approaches this subject from a different direction: it asks what structural information is forced when a physical system is described as a ledger, a discrete record of recognition events with a fixed cost structure.

The framework's machine-checked library of formal theorems contains a declaration, strongly_correlated_electrons_structure, which proves that the mathematical structure describing strongly correlated electrons implies the structural input needed for a glass transition. In plain terms: if a system's electron correlations have the right formal shape, then that same shape also satisfies the conditions for glassy structural behavior. The theorem is a logical implication between two structural descriptions, not a statement about any specific material. It says that the formal skeleton of strong correlation is rich enough to support the formal skeleton of a glass transition.

The proof is short and direct. The declaration defines the property strongly_correlated_electrons_from_ledger as exactly the same proposition as glass_transition_from_ledger. The theorem then simply identifies the two: strong correlation from the ledger is glass transition from the ledger. A second theorem, strongly_correlated_implies_glass, makes the one-way implication explicit. The entire result is a definitional identity plus a theorem that unpacks it. There is no physics input beyond the framework's foundational axioms, and no empirical data enters the proof.

In Recognition Science, this result is part of a larger program that derives physical structure from the forced cost of recognition. The framework's library shows that the same formal machinery which produces the golden ratio as a scaling constant and three spatial dimensions from linking also connects these two apparently distant condensed matter phenomena. The connection is structural, not numerical: it does not predict a transition temperature, a specific material, or any measurable property. What it establishes is that the formal description of strong correlation and the formal description of glassy behavior share a common skeleton within the framework's axioms.

What the declaration does not claim is equally important. It does not say that strongly correlated electron systems are glasses, or that glass transitions occur in such materials. It does not derive any property of a real material, and it does not use any experimental measurement. The theorem lives entirely in the framework's formal world. A reader should take it as a statement about the internal logic of the framework, not as a prediction about the physical world. The connection it proves is one of formal structure, waiting for an empirical bridge that the framework has not yet built.

THEOREM strongly_correlated_electrons_structure · IndisputableMonolith/CondensedMatter/StronglyCorrelatedElectronsStructure.lean
theorem strongly_correlated_electrons_structure :
    strongly_correlated_electrons_from_ledger := glass_transition_structure
MODEL strongly_correlated_electrons_from_ledger · IndisputableMonolith/CondensedMatter/StronglyCorrelatedElectronsStructure.lean
def strongly_correlated_electrons_from_ledger : Prop := glass_transition_from_ledger
THEOREM strongly_correlated_implies_glass · IndisputableMonolith/CondensedMatter/StronglyCorrelatedElectronsStructure.lean
/-- Strong-correlation structure implies glass-transition structural input. -/
theorem strongly_correlated_implies_glass (h : strongly_correlated_electrons_from_ledger) :
    glass_transition_from_ledger :=
  h

What this page does not claim

The theorem does not predict any transition temperature, specific material, or measurable property. The theorem does not say that strongly correlated electron systems are glasses. The proof uses no experimental data and no physics input beyond the framework's foundational axioms.

Verify this page

Every tagged claim above names its theorem. To check one yourself rather than trust this page, elaborate the source module with Lean 4 and audit its axiom basis:

$ lake env lean IndisputableMonolith/CondensedMatter/StronglyCorrelatedElectronsStructure.lean
expected axiom basis: [propext, Classical.choice, Quot.sound] (the Lean kernel's standard three; no RS-specific axioms)

A page whose claims cannot be reproduced this way does not ship. In production, every anchor links to the exact declaration in the public source release, and this block carries the build receipt for the page itself.

Derived articles

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