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The natural map between Bott-Chern cohomology and Dolbeault cohomology isIt is well-defined: a $d$-closed pure-type form is $\bar{\partial }$-closed, and $\partial \bar{\partial }\beta =-\bar{\partial }(\partial \beta )$ is $\bar{\partial }$-exact.

For surjectivity, choose the unique harmonic differential form $h$ representing a Dolbeault cohomology class using Dolbeault Hodge decomposition. The Kähler Laplacian identity ${\Delta }_d=2{\Delta }_{\bar{\partial }}$ makes $h$ a harmonic differential form for $d$, hence $d$-closed. Sending the Dolbeault class to $[h{]}_{BC}$ consequently gives a right inverse.

For injectivity, the ddbar lemma says directly that a $d$-closed, $\bar{\partial }$-exact pure-type form is $\partial \bar{\partial }$-exact. One can also exhibit its primitive. Let $G_d$ be the Green operator of the Hodge Laplacian, and put $G_{\bar{\partial }}=2G_d$. If $\alpha$ is $d$-closed and $\bar{\partial }$-exact, its harmonic projection vanishes and the Kähler identities giveHere $\partial G_{\bar{\partial }}\alpha =\bar{\partial }{G}_{\bar{\partial }}\alpha =0$ because the Green operator commutes with these differentials, and ${\bar{\partial }}^{\ast }=-i[\Lambda ,\partial ]$. Thus $\alpha$ represents zero in Bott-Chern cohomology. We have constructed the canonical isomorphism and its harmonic inverse: