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        "quote": "在量子力学中，一个系统的态最好被看作另一类数学对象：它是具有[<u class=\"concept-term\" data-concept-reference=\"concept-4-complex-inner-product\" data-concept-identity=\"urn:uuid:2aac3b49-341f-4592-97ad-65a31b630e89\" data-concept-route=\"/concept-identities#concept-2aac3b49-341f-4592-97ad-65a31b630e89\" id=\"first-636eed7b2ce59c34871d-zh\">厄米内积(Hermitian inner product)</u>](../chapter-04/04-inner-products#concept-4-complex-inner-product)的[<u class=\"concept-term\" data-concept-reference=\"concept-4-vector-space\" data-concept-identity=\"urn:uuid:cfc2af7a-6467-42cb-8699-52bf30033870\" data-concept-route=\"/concept-identities#concept-cfc2af7a-6467-42cb-8699-52bf30033870\" id=\"first-f4a8739c294321ab2ef9-zh\">复向量空间(complex vector space)</u>](../chapter-04/01-vector-spaces-and-linear-maps#concept-4-vector-space)中的一个向量；这个复向量空间就是所谓的态空间。这样的态空间有时是一个函数空间，其元素称为波函数。这些波函数也可能像经典场一样满足微分方程；但它们取复值这一点，是其非经典特征之一。量子力学迥异之处在于对可观测量的处理：它们对应于态空间上的[<u class=\"concept-term\" data-concept-reference=\"concept-4-adjoint-operator\" data-concept-identity=\"urn:uuid:a7971b9e-8f7b-49a0-a412-0ae28a65c35b\" data-concept-route=\"/concept-identities#concept-a7971b9e-8f7b-49a0-a412-0ae28a65c35b\" id=\"first-cea3b2fa67351cb42cfb-zh\">自伴线性算符(self-adjoint linear operator)</u>](../chapter-04/05-adjoint-operators#concept-4-adjoint-operator)。若这些算符彼此不对易，我们对物理规律应如何运作的直觉便会受到冲击，因为无法再同时给相应的可观测量赋予数值。",
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