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        "quote": "其中 $f _ { 1 }$ 和 $f _ { 2 }$ 是反交换变量 $\\theta _ { j }$ 的各次幂的复线性组合。关于此内积构造的细节，见 [91] 的第 7.2 章或 [110] 的第 7.5 章和<a href=\"../chapter-07/06-for-further-reading#section-7-6\" class=\"cross-reference\" id=\"xref-04-spinors-and-the-bargmann-fock-construction-1\" data-reference=\"section-7-6\">第 7.6</a> 章。我们将把这个态空间记作 $\\mathcal { F } _ { d } ^ { + }$，并称之为[<u class=\"concept-term\" data-concept-reference=\"concepts/quantum-mechanics/fermionic-fock-space\" data-concept-identity=\"urn:uuid:9d30f001-86e0-4e06-9631-c199d9cc5ae4\" data-concept-route=\"/concept-identities#concept-9d30f001-86e0-4e06-9631-c199d9cc5ae4\" id=\"first-1c8d82155046b0e8ad06-zh\">费米子Fock空间(fermionic Fock space)</u>](../../../../../concepts/quantum-mechanics/fermionic-fock-space)。由于它是有限维的，因此不需要像玻色子情形那样进行完备化。",
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        "quote": "where $f _ { 1 }$ and $f _ { 2 }$ are complex linear combinations of the powers of the anticommuting variables $\\theta _ { j }$ . For the details of the construction of this inner product, see chapter 7.2 of [91] or chapters 7.5 and 7.6 of [110]. We will denote this state space as $\\mathcal { F } _ { d } ^ { + }$ and refer to it as the [<u class=\"concept-term\" data-concept-reference=\"concepts/quantum-mechanics/fermionic-fock-space\" data-concept-identity=\"urn:uuid:9d30f001-86e0-4e06-9631-c199d9cc5ae4\" data-concept-route=\"/concept-identities#concept-9d30f001-86e0-4e06-9631-c199d9cc5ae4\" id=\"first-1c8d82155046b0e8ad06-en\">fermionic Fock space</u>](../../../../../concepts/quantum-mechanics/fermionic-fock-space). Since it is finite dimensional, there is no need for a completion as in the bosonic case.",
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