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  "body": "\n## Definition\n\nLet $U \\subseteq \\C^n$ be an open set, with coordinates $z_j = x_j + i y_j$.\nConsider complex-valued [[differential forms|0E3G0GRPZ6]] on $U$, and put $dz_j = dx_j + i\\, dy_j$ and $d\\bar z_j = dx_j - i\\, dy_j$.\nFor increasing tuples $I = (i_1 \u003c \\cdots \u003c i_p)$ and $J = (j_1 \u003c \\cdots \u003c j_q)$ of elements of $\\set{1, \\dots, n}$, write $dz_I = dz_{i_1} \\wedge \\cdots \\wedge dz_{i_p}$ and $d\\bar z_J = d\\bar z_{j_1} \\wedge \\cdots \\wedge d\\bar z_{j_q}$.\nLet $p, q \\ge 0$ be integers.\nA *$(p, q)$-form* on $U$ is a differential form\n$$\\omega = \\sum_{\\abs{I} = p, \\ \\abs{J} = q} \\omega_{IJ} \\, dz_I \\wedge d\\bar z_J,$$\nwhere the sum runs over increasing tuples and each $\\omega_{IJ} \\colon U \\to \\C$ is a [[smooth function|0V33BNKZ9S]].\n\n## Remarks\n\nThe forms $dz_I \\wedge d\\bar z_J$ with $\\abs{I} + \\abs{J} = k$ form a basis of the complex $k$-th [[exterior power|0MDMZ965VE]] of the cotangent space at each point.\nSo every complex $k$-form is, in a unique way, a sum of $(p, q)$-forms with $p + q = k$.\nExample: $\\omega = \\bar z_1 \\, dz_1 \\wedge d\\bar z_2$ on $\\C^2$ is a $(1, 1)$-form, with $\\omega_{(1)(2)} = \\bar z_1$ and all other coefficients zero.\nNon-example: $dx_1 = \\tfrac12 dz_1 + \\tfrac12 d\\bar z_1$ is a $1$-form whose $(1, 0)$ and $(0, 1)$ parts are both nonzero, so it is not a $(p, q)$-form for any $(p, q)$.\nA holomorphic change of coordinates $w = F(z)$ gives $dw_k = \\sum_j \\frac{\\partial F_k}{\\partial z_j} dz_j$ with no $d\\bar z_j$ terms, so the type $(p, q)$ is preserved; thus $(p, q)$-forms are defined on complex manifolds.\nThe space of $(p, q)$-forms on $U$ is often written $\\mathcal{E}^{p, q}(U)$.\n",
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