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  "body": "\n## Definition\n\nA *De Morgan algebra* is a structure $(A, \\vee, \\wedge, 0, 1, \\sim)$ such that:\n\n1. $(A, \\vee, \\wedge, 0, 1)$ is a [[bounded lattice|72V1Z82M5F]] that is a [[distributive lattice|0HM0HQCK6N]].\n2. ${\\sim} \\colon A \\to A$ satisfies ${\\sim}{\\sim} a = a$ for every $a \\in A$.\n3. ${\\sim}(a \\vee b) = {\\sim} a \\wedge {\\sim} b$ for all $a, b \\in A$.\n\n## Remarks\n\nFrom clauses 2 and 3 one gets ${\\sim}(a \\wedge b) = {\\sim} a \\vee {\\sim} b$, ${\\sim} 0 = 1$ and ${\\sim} 1 = 0$.\nSo ${\\sim}$ is an order-reversing bijection of $A$ onto itself.\n\nExample: the interval $[0, 1]$ with $a \\vee b = \\max(a, b)$, $a \\wedge b = \\min(a, b)$ and ${\\sim} a = 1 - a$.\nA chain is a distributive lattice, $1 - (1 - a) = a$, and $1 - \\max(a, b) = \\min(1 - a, 1 - b)$.\nIt is not a Boolean algebra, since $\\tfrac12 \\wedge {\\sim} \\tfrac12 = \\tfrac12 \\ne 0$.\n\nNon-example: the chain $0 \u003c m \u003c 1$ with ${\\sim}$ the [[pseudocomplement|WMR73J0S26]], so ${\\sim} 0 = 1$, ${\\sim} m = 0$, ${\\sim} 1 = 0$.\nClause 2 fails, since ${\\sim}{\\sim} m = 1 \\ne m$.\n",
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