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      "label": "莫比乌斯变换(Möbius transformation)",
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        "quote": "> [!exercise] <a class=\"object-permalink\" href=\"#problem-2-16\">习题 2.16</a> \n>\n> <u id=\"concept-2-mobius-transformation\" class=\"concept-term\" data-concept-identity=\"urn:uuid:6328536c-e4a4-4277-b275-0a8a7146d152\" data-concept-route=\"/concept-identities#concept-6328536c-e4a4-4277-b275-0a8a7146d152\">莫比乌斯变换(Möbius transformation)</u>是复映射\n>\n> $$\n> z\\mapsto z'=\\frac{az+b}{cz+d},\\qquad a,b,c,d\\in\\mathbb{C},\\quad ad-bc=1.\n> $$\n>\n> (a) 证明这些映射是扩充复平面（包含点 $z=\\infty$）上的一一到上变换，并写出分别由常数 $(a,b,c,d)$ 和 $(a',b',c',d')$ 确定的任意两个变换的复合。\n>\n> (b) 证明它们组成一个群，称为<u id=\"concept-2-mobius-group\" class=\"concept-term\" data-concept-identity=\"urn:uuid:861e1ce9-8826-4d7f-b756-fead75d051ac\" data-concept-route=\"/concept-identities#concept-861e1ce9-8826-4d7f-b756-fead75d051ac\">莫比乌斯群(Möbius group)</u>。\n>\n> (c) 证明把幺模矩阵 $\\begin{pmatrix}a&b\\\\c&d\\end{pmatrix}$ 映到上述莫比乌斯变换的映射 $\\mu$，是从 $SL(2,\\mathbb{C})$ 到莫比乌斯群的同态，其核为 $\\{\\mathsf{I},-\\mathsf{I}\\}$。也就是说，莫比乌斯群同构于 $SL(2,\\mathbb{C})/\\mathbb{Z}_2$。",
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        "quote": "若矩阵行列式非零，相应变换便可逆。这些保角变换称为[<u class=\"concept-term\" data-concept-reference=\"concepts/geometry/mobius-transformation\" data-concept-identity=\"urn:uuid:6328536c-e4a4-4277-b275-0a8a7146d152\" data-concept-route=\"/concept-identities#concept-6328536c-e4a4-4277-b275-0a8a7146d152\" id=\"first-5ac38295dc438d0557a8-zh\">莫比乌斯变换(Möbius transformation)</u>](../../../../../concepts/geometry/mobius-transformation.md)。在[第 40 章](../chapter-40/index#section-40)中，我们会看到这种[<u class=\"concept-term\" data-concept-reference=\"concepts/group-theory/group-action\" data-concept-identity=\"urn:uuid:9bd75d12-0eb0-4d97-ab55-23361589bdab\" data-concept-route=\"/concept-identities#concept-9bd75d12-0eb0-4d97-ab55-23361589bdab\" id=\"first-2114245f91c19109af2f-zh\">群作用(group action)</u>](../../../../../concepts/group-theory/group-action.md)出现在狭义相对论中；它对球面的作用可以理解为对光线空间的变换。当矩阵属于 $SU(2)$ 时，其元素满足 $\\gamma=-\\overline\\beta$、$\\delta=\\overline\\alpha$ 以及 $|\\alpha|^2+|\\beta|^2=1$。此时球面上的对应变换就是 $\\mathbf R^3$ 中球面的旋转。这也从另一角度说明 $SU(2)=\\operatorname{Spin}(3)$ 是旋转群 $SO(3)$ 的双覆盖。",
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        "quote": "If the matrix has nonzero determinant, the transformation is invertible. These are conformal (angle-preserving) transformations of the complex plane called [<u class=\"concept-term\" data-concept-reference=\"concepts/geometry/mobius-transformation\" data-concept-identity=\"urn:uuid:6328536c-e4a4-4277-b275-0a8a7146d152\" data-concept-route=\"/concept-identities#concept-6328536c-e4a4-4277-b275-0a8a7146d152\" id=\"first-e2a6486a1efc2e914542-en\">Möbius transformations</u>](../../../../../concepts/geometry/mobius-transformation.md). In [Chapter 40](../chapter-40/index#section-40), we will see this [<u class=\"concept-term\" data-concept-reference=\"concepts/group-theory/group-action\" data-concept-identity=\"urn:uuid:9bd75d12-0eb0-4d97-ab55-23361589bdab\" data-concept-route=\"/concept-identities#concept-9bd75d12-0eb0-4d97-ab55-23361589bdab\" id=\"first-2114245f91c19109af2f-en\">group action</u>](../../../../../concepts/group-theory/group-action.md) in special relativity, where its action on the sphere can be understood as a transformation of the space of light rays. For a matrix in $SU(2)$, the entries satisfy $\\gamma=-\\overline\\beta$, $\\delta=\\overline\\alpha$, and $|\\alpha|^2+|\\beta|^2=1$. The corresponding transformation rotates the sphere in $\\mathbf R^3$, giving another way to understand $SU(2)=\\operatorname{Spin}(3)$ as the double cover of $SO(3)$.",
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