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Liouville's equation

For Liouville's equation in dynamical systems, see Liouville's theorem (Hamiltonian).
For Liouville's equation in quantum mechanics, see Von Neumann equation.
For Liouville's equation in Euclidean space, see Liouville–Bratu–Gelfand equation.

In differential geometry, Liouville's equation, named after Joseph Liouville, is the nonlinear partial differential equation satisfied by the conformal factor f of a metric f2(dx2 + dy2) on a surface of constant Gaussian curvature K:

where 0 is the flat Laplace operator

Liouville's equation appears in the study of isothermal coordinates in differential geometry: the independent variables x,y are the coordinates, while f can be described as the conformal factor with respect to the flat metric. Occasionally it is the square f2 that is referred to as the conformal factor, instead of f itself.

Liouville's equation was also taken as an example by David Hilbert in the formulation of his nineteenth problem.[1]

Other common forms of Liouville's equationEdit

By using the change of variables log f ↦ u, another commonly found form of Liouville's equation is obtained:


Other two forms of the equation, commonly found in the literature,[2] are obtained by using the slight variant 2 log f ↦ u of the previous change of variables and Wirtinger calculus:[3]


Note that it is exactly in the first one of the preceding two forms that Liouville's equation was cited by David Hilbert in the formulation of his nineteenth problem.[1][4]

A formulation using the Laplace–Beltrami operatorEdit

In a more invariant fashion, the equation can be written in terms of the intrinsic Laplace-Beltrami operator


as follows:



Relation to Gauss–Codazzi equationsEdit

Liouville's equation is a consequence of the Gauss–Codazzi equations when the metric is written in isothermal coordinates.

General solution of the equationEdit

In a simply connected domain Ω, the general solution of Liouville's equation can be found by using Wirtinger calculus.[5] Its form is given by


where f (z) is any meromorphic function such that


Liouville's equation can be used to prove the following classification results for surfaces:

Theorem.[6] A surface in the Euclidean 3-space with metric dl2 = g(z,_z)dzd_z, and with constant scalar curvature K is locally isometric to:

  1. the sphere if K > 0;
  2. the Euclidean plane if K = 0;
  3. the Lobachevskian plane if K < 0.

See alsoEdit

  • Liouville field theory, a two-dimensional conformal field theory whose classical equation of motion is a generalization of Liouville's equation


  1. ^ a b See (Hilbert 1900, p. 288): Hilbert does not cite explicitly Joseph Liouville.
  2. ^ See (Dubrovin, Novikov & Fomenko 1992, p. 118) and (Henrici, p. 294).
  3. ^ See (Henrici, pp. 287–294).
  4. ^ Hilbert assumes K = -1/2, therefore the equation appears as the following semilinear elliptic equation:
  5. ^ a b c See (Henrici, p. 294).
  6. ^ See (Dubrovin, Novikov & Fomenko 1992, pp. 118–120).