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        "quote": "构造量子力学态空间 $\\mathcal{H}$ 的一种方式，是把态表示为“<u id=\"concept-1-wavefunction\" class=\"concept-term\" data-concept-id=\"concept-1-wavefunction\" data-concept-role=\"discussion\" data-concept-identity=\"urn:uuid:928ab6a9-7e9a-4beb-adff-65f984589c86\" data-concept-route=\"/concept-identities#concept-928ab6a9-7e9a-4beb-adff-65f984589c86\">波函数(wavefunction)</u>”，也就是定义在时空上的复值函数。给定时空上的任意群作用，依照[方程 (1.3)](./03-unitary-group-representations#equation-1-3) 的构造，便可在这类波函数组成的态空间 $\\mathcal{H}$ 上得到表示 $\\pi$。然而，我们感兴趣的许多表示并非由这种构造得到。接下来几章将先研究这类更简单的有限维例子；之后再讨论由时空上的群作用诱导的无限维表示。",
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