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  "body": "\n## Statement\n\nLet $n \\ge 1$ and give $\\R^{2n}$ the coordinates $(x_1, y_1, \\ldots, x_n, y_n)$ and the standard symplectic form $\\omega_0 = \\sum_{i=1}^n dx_i \\wedge dy_i$.\nFor $r \u003e 0$, let $B^{2n}(r)$ be the open ball of radius $r$ centered at $0$.\nFor $R \u003e 0$, let\n$$Z^{2n}(R) = \\set{(x, y) \\in \\R^{2n} : x_1^2 + y_1^2 \u003c R^2}$$\nbe the open cylinder of radius $R$ over a disc in the $(x_1, y_1)$-plane.\nIf there is a symplectic embedding $\\varphi \\colon B^{2n}(r) \\to Z^{2n}(R)$, that is, a smooth embedding with $\\varphi^* \\omega_0 = \\omega_0$, then $r \\le R$.\n\n## Remarks\n\nGromov proved the theorem in 1985 with [[pseudoholomorphic curves|N469E47V75]].\nAssume $r \u003e R$ and an embedding exists; compactify the cylinder to $S^2 \\times T^{2n-2}$ with $S^2$ of area slightly more than $\\pi R^2$.\nFor a suitable almost complex structure, there is a pseudoholomorphic sphere in the class of $S^2$ through the image of the center of the ball.\nIts area is less than $\\pi R^2 + \\varepsilon$.\nPulled back to the ball, it gives a proper minimal surface through the center with area less than $\\pi r^2$.\nThis contradicts the monotonicity formula, which says that such a surface has area at least $\\pi r^2$.\n\nThe hypothesis that the disc lies in a symplectic plane is needed.\nThe map $(x_1, y_1, x_2, y_2) \\mapsto (\\lambda x_1, \\lambda^{-1} y_1, \\lambda x_2, \\lambda^{-1} y_2)$ with small $\\lambda \u003e 0$ is a linear symplectomorphism that squeezes any ball into the cylinder $\\set{x_1^2 + x_2^2 \u003c R^2}$ over the $(x_1, x_2)$-plane, which is Lagrangian.\nFor $n = 1$ the theorem is just the statement that area-preserving maps preserve area.\n\n## Explanations\n\n### L1 human\n\nA symplectic map preserves volume, but in dimension four and higher it is much more rigid than that.\nA ball cannot be squeezed by a symplectic map through a round hole whose radius is smaller than the ball's, even though the cylinder over the hole has infinite volume.\nThis is sometimes called the principle of the symplectic camel.\n\n### L2 human\n\nThe theorem marks the birth of symplectic topology: it shows that symplectic maps are not just volume-preserving maps.\nIt leads to the notion of a [[symplectic capacity|8KCB5KJKNT]], a size of a symplectic set that is invariant under symplectic embeddings.\nBy Liouville's theorem, Hamiltonian flows preserve volume; non-squeezing gives a finer constraint on them, a classical analogue of the uncertainty principle.\n",
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