In General > s.a. 2D gravity; 2D
manifolds; Geometric Topology.
* Result: All metrics are conformally flat, i.e., they can be locally
written as
ds2 =
2(
,
)
(d
2
d
2)
,
where
and
are
conjugate harmonic coordinates.
* Riemannian: There are
3 different kinds of geometry; given any closed 2-manifold, it can be given
a (unique) metric such that we get one of the following:
R > 0: elliptic (S2);
R = 0: parabolic (T2);
R < 0: hyperbolic (all higher orientable g's).
* Lorentzian: The only compact 2-manifolds which admit a metric of signature
(–,+) are the 2-torus T2 and the Klein bottle (thus, e.g., S2 does not
admit a Lorentzian metric).
* Curvature: The Einstein
tensor vanishes identically, thus
M
R dv can only be a topological term plus a surface term (> see
the gauss-bonnet theorem for the
positive-definite
case); The
Riemann
tensor is
given
by
Rabcd = R ga[c gd]b .
* Gaussian curvature: For a surface V(x,y),
K = (Vxx Vyy – Vxy2) / (1 + Vxx2Vyy2)2 .
Special Metrics > s.a. Zollfrei
Metric.
* Constant curvature: In genus 0, the sphere S2; In genus 1, the
flat
torus T2; In genus 2, the double torus, which can be unfolded into an
octagon
in its universal covering, the hyperbolic space H2.
* Circular symmetry: In the Riemannian case, the metric can be written
as
ds2 = d
2
+ f 2(
)
d
2 ,
and the only nonvanishing connection coefficients in these coordinates are
122
= f f ' ,
212
=
221
= f –1f ' .
* Darboux spaces: Two-dimensional
spaces of non-constant curvature.
@ References: Kramer & Lorente JPA(02)gq/04 [double
torus]; Gallo JMP(04)gq [from
second-order differential equations]; Grosche PPN(06)qp/04 [path
integrals on Darboux spaces]; Bertotti et al m.HO/05-in
[constant negative Gaussian curvature].
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Send feedback and suggestions to bombelli at olemiss.edu – Modified
11 jun 2008