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Classical Fermi Fluid and Geometric Action for $c=1$

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abstract

We formulate the $c=1$ matrix model as a quantum fluid and discuss its classical limit in detail, emphasizing the $\hbar$ corrections. We view the fermi fluid profiles as elements of \winf-coadjoint orbit and write down a geometric action for the classical phase space. In the specific representation of fluid profiles as `strings' the action is written in a four-dimensional form in terms of gauge fields built out of the embedding of the `string' in the phase plane. We show that the collective field action can be derived from the above action provided one restricts to quadratic fluid profiles and ignores the dynamics of their `turning points'.

fields

hep-th 1

years

2026 1

verdicts

UNVERDICTED 1

representative citing papers

Fate of "Space-like singularities" in $c=1$ Matrix Model

hep-th · 2026-06-30 · unverdicted · novelty 7.0

Space-like singularities in the c=1 matrix model are artifacts of the double scaling limit; beyond it, Fermi surface folds proliferate and the coarse-grained phase space density relaxes to equilibrium via a universal power-law independent of initial state details.

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  • Fate of "Space-like singularities" in $c=1$ Matrix Model hep-th · 2026-06-30 · unverdicted · none · ref 30 · internal anchor

    Space-like singularities in the c=1 matrix model are artifacts of the double scaling limit; beyond it, Fermi surface folds proliferate and the coarse-grained phase space density relaxes to equilibrium via a universal power-law independent of initial state details.