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        "quote": "在[第3](../chapter-03/index#section-3)章中我们看到，一个具有$\\mathcal { H } = \\mathbf { C } ^ { 2 }$的一般量子系统可以通过$U ( 2 )$在$\\mathbf { C } ^ { 2 }$上的作用来理解。自伴算符所表示的[<u id=\"concept-7-quantum-observable\" class=\"concept-term\" data-concept-identity=\"urn:uuid:1f30c262-f238-4dfd-acec-55532f758890\" data-concept-route=\"/concept-identities#concept-1f30c262-f238-4dfd-acec-55532f758890\">可观测量(quantum observable)</u>](../../../../../concepts/quantum-mechanics/quantum-observable)对应于相应的[<u id=\"concept-7-lie-algebra-representation\" class=\"concept-term\" data-concept-identity=\"urn:uuid:5bad1df2-281a-4c11-8362-128d54fb523a\" data-concept-route=\"/concept-identities#concept-5bad1df2-281a-4c11-8362-128d54fb523a\">李代数表示(Lie algebra representation)</u>](../../../../../concepts/lie-theory/lie-algebra-representation)（相差一个因子 $i$）。$U ( 1 ) \\subset U ( 2 )$子群与所有其他部分对易，可以单独分析，这里我们只考虑$S U ( 2 )$子群。对于任意这样的系统，群$S U ( 2 )$没有特别的几何意义。当它作为旋转群的双覆盖出现时，称该量子系统携带[<u id=\"concept-7-spin\" class=\"concept-term\" data-concept-identity=\"urn:uuid:3e11a671-c004-44f2-8d6e-bf7933e08bbb\" data-concept-route=\"/concept-identities#concept-3e11a671-c004-44f2-8d6e-bf7933e08bbb\">自旋(spin)</u>](../../../../../concepts/quantum-mechanics/spin)；特别是，二维[<u id=\"concept-7-irreducible-representation\" class=\"concept-term\" data-concept-identity=\"urn:uuid:4e9e2c89-0422-42cf-8762-6b5e59837ef0\" data-concept-route=\"/concept-identities#concept-4e9e2c89-0422-42cf-8762-6b5e59837ef0\">不可约表示(irreducible representation)</u>](../../../../../concepts/representation-theory/irreducible-representation)对应自旋 $1/2$（在[第8](../chapter-08/index#section-8)章中我们将讨论更高自旋值的态空间）。",
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        "quote": "将这一结果用于磁场中的[<u id=\"concept-7-3-spin\" class=\"concept-term\" data-concept-reference=\"concepts/quantum-mechanics/spin\" data-concept-id=\"concept-7-3-spin\" data-concept-identity=\"urn:uuid:3e11a671-c004-44f2-8d6e-bf7933e08bbb\" data-concept-route=\"/concept-identities#concept-3e11a671-c004-44f2-8d6e-bf7933e08bbb\">自旋(spin)</u>](../../../../../concepts/quantum-mechanics/spin) $1/2$ 系统，并取可观测量 $\\mathbf{S}$（即由 $S_j$ 组成的列向量），可得：",
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        "quote": "The sum comes from the tensor-product representation. Here $\\widehat{\\mathbf L}$ comprises two copies of <a href=\"#equation-38-12\" class=\"cross-reference\" id=\"xref-05-spatial-symmetries-6\" data-reference=\"equation-38-12\">equation38.12</a>, induced by spatial rotations of the solutions. The [<u class=\"concept-term\" data-concept-reference=\"concepts/quantum-mechanics/spin-angular-momentum\" data-concept-identity=\"urn:uuid:3e11a671-c004-44f2-8d6e-bf7933e08bbb\" data-concept-route=\"/concept-identities#concept-3e11a671-c004-44f2-8d6e-bf7933e08bbb\">spin</u>](../../../../../concepts/quantum-mechanics/spin-angular-momentum) operator $\\widehat{\\mathbf S}$ comes from the $SU(2)$ action on the $\\mathbb C^2$ factor and is",
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