DOI: 10.3390/universe12110317 ISSN: 2218-1997

Infrared Divergences as Itinerant Vacua

Masahiro Morikawa

Infrared divergences (IRDs) are usually treated as pathologies to be canceled, regularized, or hidden in dressed asymptotic states. This paper develops a complementary and constructive viewpoint: an IRD is the signature of an itinerant vacuum—a quantum vacuum that wanders continuously through a family of inequivalent states as a classical order parameter evolves. Each value of the order parameter carries its own coherent vacuum, so moving the order parameter means traversing a succession of orthogonal vacua. The IRD is the field-theoretic cost of this wandering, and the 1/f noise, gravitational memory, and non-Gaussian fluctuations that emerge from it are its observable classical remnants. The technical core is an exact separation in the real-time closed-time-path (CTP) effective action. For soft QED, we take the standard Faddeev–Kulish coherent dressing as the asymptotic, infrared-safe description; the new step is to promote its fixed in/out dressing profile α to a real-time history α[J(t)] along with the evolving current J(t). The infrared-enhanced symmetric part of the corresponding reduced CTP influence functional is then converted, by a Hubbard–Stratonovich identity, into a classical stochastic source. This step is an algebraic identity of the generating functional and requires no additional coarse graining once the reduced CTP effective action for the collective variable has been defined: the retarded kernel encodes the memory of past vacuum transitions, while the noise kernel encodes the quantum uncertainty of the next one. We apply this construction to four parallel arenas—soft QED, scalar fields in de Sitter space, soft gravitons, and non-equilibrium phase transitions—and show that the same itinerant-vacuum mechanism underlies 1/f current noise, the primordial power spectrum, gravitational memory, and order-parameter dynamics. A geometric formulation in terms of a Hilbert-space bundle over the vacuum manifold is outlined as an outlook.

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