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ExampleConstruction: AI-generatedVerification: AI-generatedPipeline-generatedverified 2026-10-15 (gpt-6-luna, gpt-6.1-sol, and delegated Codex review/repair agents; see completed run evidence)
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Two minimizers in a reduced coexistence model

Physical scope

A dimensionless coarse-grained order-parameter example illustrating a possible failure of a singleton variational-minimizer assumption; it is not a continuum Gibbs-potential calculation.

Example

Consider the reduced coarse-grained variational model with scalar dimensionless order parameter m∈[−1,1] and dimensionless free-energy function g(m)=(m2−1)2. Its global minimizers are m=−1 and m=1. This model shows why uniqueness must be stated as a parameter-specific assumption. It does not identify these two minimizers with Gibbs measures of a continuum pair potential.

Facts & Assumptions

[F1]

Selected grand-variational phase uniqueness: the selected continuum conclusion is licensed only when the relevant minimizer set on the finite-intensity stationary-law domain is a singleton.

[A1]

Adopt the stated toy variational function g(m)=(m2−1)2 on the closed interval [−1,1]; m and g are dimensionless.

Verification

Given: The domain [−1,1], the explicit function g, and the limited illustrative scope.

1.1givenA1algebra

For every m∈[−1,1], g(m)=(1−m2)2≥0. Equality holds exactly when m2=1, namely at m=−1 or m=1.

2.1givenF1step 1.1∎

The two equality points are distinct, so this scalar model's global-minimizer set is {−1,1} and is not a singleton. This illustrates the need for a separate uniqueness assumption in a variational model. The domain in [F1] consists of stationary configuration laws, whereas this domain is [−1,1]; no map identifying their minimizers has been specified. Thus this calculation neither instantiates nor refutes the continuum assumption [F1].

Depends on

Dependency tree · 2 levels