# Determing Hodges Maps by their Essential Algebraic Properties

Let $M$ be a complex manifold of real dimension $2N$, equipped with a Hermitian metric. The corresponding Hodge map $\ast$ has the following properties:

(i) It is a ${\bf C}$-linear map $\ast:\Omega^k(M) \to \Omega^{2N-k}(M)$;

(ii) $\ast(\Omega^{(p,q)}(M)) = \Omega^{(N-p,N-q)}$(M);

(iii) $\ast^2 = (-1)^{k}$ on $\Omega^k(M)$.

Now I would guess that there exist other maps on $\Omega(M)$ with these properties which do not arise as Hodge maps from some Hermitian metric. So my question is, do there exist extra (algebraic) properties of $\ast$, which when put together with $(i),(ii)$, and $(iii)$, determine all the Hodge maps, but without ever explicitly mentioning metrics.

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I'm not sure what you're really looking for, but aside from (i)-(iii), what is essential is that $(const.)\int \alpha\wedge*\beta$ determines an inner product on the space of forms. –  Donu Arapura Feb 2 '13 at 15:23
... with compact support. –  Donu Arapura Feb 2 '13 at 15:35
John, I'm just trying to understand the question. When you say "Hodge map" are you explicitly referring to the hodge star operator? I'm a little confused, since you say the plural "Hodge maps" later (which makes sense in this context). I'm just being a little careful. Is this standard terminology? –  LMN Feb 3 '13 at 0:47
1. In (i), you need $*$ to be linear over functions otherwise it is not algebraic (tensorial) at all.
2. There are clearly necessary conditions for $*$ to be a Hodge map for some Hermitian metric. We fix a volume form as $*1$ and then the metric on $1$-forms is defined by $(\omega_1,\omega_2)*1=\omega_1\wedge *\omega_2$. At this point, we get two conditions: the metric so defined had better be non-degenerate and positive definite. This is an open condition. Moreover, $\star 1$ must now be the wedge of an orthonormal basis of $1$-forms and that is an algebraic condition relating $\star$ on $0$-forms with $\star$ on $1$-forms. For $N=1$, this condition is vacuous: $\star$ on $1$-forms defines a conformal structure and then $\star$ on $0$-forms simply fixes a scale to get a metric. However, when $N>1$, $\star$ on $k$-forms for $2\leq k\leq N$ is already determined by the metric we have found and so there must be compatibility conditions.