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        "quote": "我们有时把算符 $Q$ 称为“[<u class=\"concept-term\" data-concept-reference=\"concepts/representation-theory/charge-operator\" data-concept-identity=\"urn:uuid:52a09bf2-6b64-4f64-8d17-cb50a2c294d5\" data-concept-route=\"/concept-identities#concept-52a09bf2-6b64-4f64-8d17-cb50a2c294d5\" id=\"first-bbf4d016dc21069094bf-zh\">电荷算符(charge operator)</u>](../../../../../concepts/representation-theory/charge-operator)”，并赋予“电荷”一词比具体电荷更广的含义。$U ( 1 )$表示在数学中也无处不在，其中$Q$算符的整数特征值常被称为“权”。",
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        "quote": "\n> [!definition] 定义 · <span class=\"definition-name\"><u class=\"concept-term\" data-concept-id=\"concept-2-charge-operator\" data-concept-identity=\"urn:uuid:52a09bf2-6b64-4f64-8d17-cb50a2c294d5\" data-concept-route=\"/concept-identities#concept-52a09bf2-6b64-4f64-8d17-cb50a2c294d5\">电荷算符(charge operator)</u></span>\n> <span id=\"source-block-2089\" class=\"block-anchor\"></span>\n>\n> <span class=\"author-definition-label\" aria-hidden=\"true\">定义。</span>对于 $U(1)$ 在 $\\mathcal H$ 上的表示 $(\\pi,\\mathcal H)$，电荷算符 $Q$ 是作用于 $\\mathcal H$ 的自伴线性算符；在每个不可约子表示 $\\mathcal H_{q_j}$ 上，它等于乘以 $q_j$。若在各 $\\mathcal H_{q_j}$ 中选取基向量，则 $Q$ 在 $\\mathcal H$ 上的矩阵为：\n>\n> <span id=\"source-block-2090\" class=\"block-anchor\"></span>\n>\n> $$\n> Q = \\left( \\begin{array}{c c c c} q _ {1} & 0 & \\dots & 0 \\\\ 0 & q _ {2} & \\dots & 0 \\\\ \\dots & & & \\dots \\\\ 0 & 0 & \\dots & q _ {n} \\end{array} \\right)\n> $$\n",
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