Theoretical framework derives a dissipation coefficient and geometric structure in order parameter systems, suggesting new dynamical behaviors.
Within the CTP (Schwinger-Keldysh) nonequilibrium field theory framework for an order-parameter--environment-field coupled system, we rigorously derive the microscopic expression for the dissipation coefficient and further prove that, in the infrared slow-dynamics limit, the effective action of the order parameter necessarily takes the form S_eff = ∫ (∂_t φ_c)² / g_ii(φ_c) dt, where g_ii = 1/γ_eff defines the order parameter space metric. This geometric structure is not an externally imposed postulate, but an inevitable emergence from CTP field theory in the infrared limit. The core result is a three-factor decomposition of the dissipation coefficient: γ_eff = C (Z' ∂_t φ_c)², where C is the phase-space and fluctuation factor, Z' is the derivative coupling strength, and ∂_t φ_c is the order parameter velocity. From this we define the intrinsic temporal thickness of a force, τ_F ≡ 1/[C (Z')² m_Φ²]—an inherent property of the force itself, uniquely determined by the microscopic structure of the coupling. When the derivative coupling tends to zero (Z' → 0), the dynamical dissipation channel is blockaded and the dissipative force ceases to act. From the geometric form of the effective action, we derive the irreversible equation of motion for the order parameter, in which the third term—the metric gradient force—is an exclusive dynamical prediction: in an inhomogeneous dissipative environment, the order parameter is pushed toward regions of larger metric (weaker dissipation), with an acceleration direction independent of the sign of the velocity. This paper provides the microscopic foundation for the postulates presented in a companion paper: "On the Irreversible Geometry of Order Parameter Space — The Principle of Minimum Irreversible Cost and Its Physical Consequences" by the same author.
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涛 翟 (2026) studied this question.
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