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  "body": "\n## Summary\n\nGeometric group theory studies [[finitely generated groups|082DWWXMRJ]] through the geometry of spaces on which they act, such as their [[Cayley graphs|0GYQK9NDJF]] with the [[word metric|VCHJVR9NGH]].\nIts basic principle is to study groups up to [[quasi-isometry|6FKYSH729T]], which ignores small-scale details and distortions by bounded factors.\nThe [[Švarc–Milnor lemma|NTK1TVA50A]] links this view to group actions on metric spaces.\nCentral results include [[Gromov's theorem on groups of polynomial growth|RSBFHHPTWX]] and [[Stallings's theorem on ends of groups|GWZN3EKEWD]].\nCentral classes include [[hyperbolic groups|JWJ8YPR7EB]] and [[amenable groups|CEAT9BESKK]].\nThe field grew from combinatorial group theory and low-dimensional topology.\nIt took its modern form in the 1980s and 1990s, largely through the work of Gromov.\n\n## Explanations\n\n### L1 human\n\nA group given by generators can be drawn as a graph: one dot for each element, and a line from $g$ to $gs$ for each generator $s$.\nSeen from far away, this graph has a shape.\nThe Cayley graph of $\\Z^2$ with its two standard generators looks like a grid and, from far away, like a plane.\nThe Cayley graph of a free group on two generators is an infinite tree, which looks nothing like a plane.\nGeometric group theory reads algebraic properties of the group from such large-scale shapes, and the other way around.\n",
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