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        "quote": "因此，任何图册 $\\boldsymbol { A }$ 都可以通过向其中添加所有与 的图卡 $C ^ { \\infty }$ 相容的图卡，从而扩展为一个 <u id=\"concept-15-maximal-atlas\" class=\"concept-term\" data-concept-identity=\"urn:uuid:5297658f-b601-4564-8c96-d8298c08cad7\" data-concept-route=\"/concept-identities#concept-5297658f-b601-4564-8c96-d8298c08cad7\">极大图册(maximal atlas)</u>。这个极大图册称为 $M$ 上的一个 <u id=\"concept-15-differentiable-structure\" class=\"concept-term\" data-concept-identity=\"urn:uuid:5c84e88a-89e3-4262-b2c7-9fe2ef55d012\" data-concept-route=\"/concept-identities#concept-5c84e88a-89e3-4262-b2c7-9fe2ef55d012\">可微结构(differentiable structure)</u>。若 $M$ 是一个 $n$ 维拓扑流形，且 是 $M ,$ 上的一个可微结构，则称有序对 $( M , A )$ 为一个 <u id=\"concept-15-differentiable-manifold\" class=\"concept-term\" data-concept-identity=\"urn:uuid:a0553dab-d811-417e-8a79-67ec620792e7\" data-concept-route=\"/concept-identities#concept-a0553dab-d811-417e-8a79-67ec620792e7\">可微流形(differentiable manifold)</u>；通常就简记为 $M$。",
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        "quote": "Any atlas $\\boldsymbol { A }$ may thus be extended to a <u class=\"concept-term\" data-concept-identity=\"urn:uuid:5297658f-b601-4564-8c96-d8298c08cad7\" data-concept-route=\"/concept-identities#concept-5297658f-b601-4564-8c96-d8298c08cad7\" id=\"first-9d5ce9406e1e672e08ae-en\">maximal atlas</u> by adding to it all charts that are $C ^ { \\infty }$ -compatible with the charts of . This maximal atlas is called a <u class=\"concept-term\" data-concept-identity=\"urn:uuid:5c84e88a-89e3-4262-b2c7-9fe2ef55d012\" data-concept-route=\"/concept-identities#concept-5c84e88a-89e3-4262-b2c7-9fe2ef55d012\" id=\"first-361378f15f49e6a6b5e4-en\">differentiable structure</u> on $M$. A pair $( M , A )$ , where $M$, is an $n$-dimensional topological manifold and is a differentiable structure on $M ,$ , is called a <u class=\"concept-term\" data-concept-identity=\"urn:uuid:a0553dab-d811-417e-8a79-67ec620792e7\" data-concept-route=\"/concept-identities#concept-a0553dab-d811-417e-8a79-67ec620792e7\" id=\"first-00aa8b52b61298eda3c9-en\">differentiable manifold</u>; it is usually just denoted $M$.",
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        "quote": "我们主要关注 $G$ 为李群的情形，此时 $G$ 是某个维数的[<u class=\"concept-term\" data-concept-reference=\"concepts/differential-geometry/differentiable-manifold\" data-concept-identity=\"urn:uuid:a0553dab-d811-417e-8a79-67ec620792e7\" data-concept-route=\"/concept-identities#concept-a0553dab-d811-417e-8a79-67ec620792e7\" id=\"first-85de52b9f66f87345b81-zh\">可微流形(differentiable manifold)</u>](../../../../../concepts/differential-geometry/differentiable-manifold)。在这种情形下，我们只考虑由[<u class=\"concept-term\" data-concept-reference=\"concepts/differential-geometry/differentiable-map\" data-concept-identity=\"urn:uuid:6ed47c88-27f1-4afd-88e9-df76c8500ef4\" data-concept-route=\"/concept-identities#concept-6ed47c88-27f1-4afd-88e9-df76c8500ef4\" id=\"first-1298f053f1001f2db6be-zh\">可微映射(differentiable map)</u>](../../../../../concepts/differential-geometry/differentiable-map) $\\pi$ 给出的表示。作为向量空间，$GL(n,\\mathbf{C})$ 是所有 $n\\times n$ 复矩阵构成的 $\\mathbf{C}^{n^2}$；要得到 $GL(n,\\mathbf{C})$，需去掉行列式为零的矩阵，也就是所有不可逆矩阵。在 $G$ 上选定局部坐标后，映射 $\\pi:G\\to GL(n,\\mathbf{C})$ 可由 $2n^2$ 个实值函数表示；$G$ 为可微流形这一条件保证了 $\\pi$ 的导数定义良好。我们的重点不是一般情形，而是量子力学中具有核心意义的某些特定李群及其表示 $\\pi$。对这些表示，$\\pi$ 的可微性可以直接看出。",
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