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        "quote": "任意三个满足对易关系<a href=\"#equation-14-25\" class=\"cross-reference\" id=\"xref-02-quantum-dynamics-19\" data-reference=\"equation-14-25\">式 (14.25)</a> 的算符 $L _ { 1 } , L _ { 2 } , L _ { 3 }$ 都称为 <u class=\"concept-term\" data-concept-identity=\"urn:uuid:3eb9597a-ad5c-4bc3-96cd-60280ad79388\" data-concept-route=\"/concept-identities#concept-3eb9597a-ad5c-4bc3-96cd-60280ad79388\" id=\"first-65644d184cd68c46bbe1-zh\">角动量算子(angular momentum operator)</u>。若它们具有形式 $L _ { i } = \\epsilon _ { i j k } Q _ { j } P _ { k }$，则称之为 <u class=\"concept-term\" data-concept-identity=\"urn:uuid:d24133d7-c651-4a09-95d9-bcd4dfecc852\" data-concept-route=\"/concept-identities#concept-d24133d7-c651-4a09-95d9-bcd4dfecc852\" id=\"first-c302a6cf2fa6e33ec1df-zh\">轨道角动量(orbital angular momentum)</u>；否则称为 <u class=\"concept-term\" data-concept-identity=\"urn:uuid:14f530a7-cae3-4199-a129-754aeece7b1f\" data-concept-route=\"/concept-identities#concept-14f530a7-cae3-4199-a129-754aeece7b1f\" id=\"first-7d8bfa0700d40e3eaff6-zh\">自旋角动量(spin angular momentum)</u>，或其组合。若令 $J _ { i } = L _ { 1 } / \\hbar$ 和 $J ^ { 2 } = ( J _ { 1 } ) ^ { 2 } + ( J _ { 2 } ) ^ { 2 } + ( J _ { 3 } ) ^ { 2 }$，则",
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