In mathematics, and more specifically in differential geometry, a Hermitian manifold is the complex analogue of a Riemannian manifold. More precisely, a Hermitian manifold is a complex manifold with a smoothly varying Hermitian inner product on each (holomorphic) tangent space. One can also define a Hermitian manifold as a real manifold with a Riemannian metric that preserves a complex structure. A complex structure is essentially an almost complex structure with an integrability condition, and this condition yields a unitary structure (U(n) structure) on the manifold. By dropping this condition, we get an almost Hermitian manifold. On any almost Hermitian manifold, we can introduce a fundamental 2-form (or cosymplectic structure) that depends only on the chosen metric and the almost complex structure. This form is always non-degenerate. With the extra integrability condition that it is closed (i.e., it is a symplectic form), we get an almost Kähler structure. If both the almost complex structure and the fundamental form are integrable, then we have a Kähler structure.
Formal definition A Hermitian metric on a complex vector bundle E {\displaystyle E} over a smooth manifold M {\displaystyle M} is a smoothly varying positive-definite Hermitian form on each fiber. Such a metric can be viewed as a smooth global section h {\displaystyle h} of the vector bundle ( E ⊗ E ¯ ) ∗ {\displaystyle (E\otimes {\overline {E}})^{*}} such that for every point p {\displaystyle p} in M {\displaystyle M} ,
h p ( η , ζ ¯ ) = h p ( ζ , η ¯ ) ¯ {\displaystyle h_{p}{\mathord {\left(\eta ,{\bar {\zeta }}\right)}}={\overline {h_{p}{\mathord {\left(\zeta ,{\bar {\eta }}\right)}}}}}
for all ζ {\displaystyle \zeta } , η {\displaystyle \eta } in the fiber E p {\displaystyle E_{p}} and
h p ( ζ , ζ ¯ ) > 0 {\displaystyle h_{p}{\mathord {\left(\zeta ,{\bar {\zeta }}\right)}}>0}
for all nonzero ζ {\displaystyle \zeta } in E p {\displaystyle E_{p}} . A Hermitian manifold is a complex manifold with a Hermitian metric on its holomorphic tangent bundle. Likewise, an almost Hermitian manifold is an almost complex manifold with a Hermitian metric on its holomorphic tangent bundle. On a Hermitian manifold the metric can be written in local holomorphic coordinates ( z α ) {\displaystyle (z^{\alpha })} as
h = h α β ¯ d z α ⊗ d z ¯ β {\displaystyle h=h_{\alpha {\bar {\beta }}}\,dz^{\alpha }\otimes d{\bar {z}}^{\beta }}
where h α β ¯ {\displaystyle h_{\alpha {\bar {\beta }}}} are the components of a positive-definite Hermitian matrix.
Riemannian metric and associated form A Hermitian metric h on an (almost) complex manifold M defines a Riemannian metric g on the underlying smooth manifold. The metric g is defined to be the real part of h:
g = 1 2 ( h + h ¯ ) . {\displaystyle g={1 \over 2}\left(h+{\bar {h}}\right).}
The form g is a symmetric bilinear form on TMC, the complexified tangent bundle. Since g is equal to its conjugate it is the complexification of a real form on TM. The symmetry and positive-definiteness of g on TM follow from the corresponding properties of h. In local holomorphic coordinates the metric g can be written
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