{
  "schema_version": 1,
  "kind": "ConceptView",
  "producer": "concept-view-1",
  "concept_id": "urn:uuid:ca209073-6b0b-4faa-b78f-0d00d3d11d24",
  "labels": {
    "zh-CN": "自发对称破缺",
    "en": "spontaneous symmetry breaking"
  },
  "alternative_labels": [],
  "scope_note": "",
  "identity_status": "active",
  "identity_revision": "341d8dd7acb3b44acf509f1d0394e0096c043bd9c5c6aee794c6ec5e357e6360",
  "occurrences": [
    {
      "concept_id": "urn:uuid:ca209073-6b0b-4faa-b78f-0d00d3d11d24",
      "book_id": "woit-qtgr",
      "edition_id": "2025-10-20",
      "lang": "zh-CN",
      "route": "books/woit-qtgr/2025-10-20/zh/chapter-39/04-spontaneous-symmetry-breaking",
      "anchor": "first-604a9d7ff08d53f734ab-zh",
      "chapter": "39",
      "section": "39.4",
      "offset": 802,
      "range": [
        7558,
        7896
      ],
      "source_revision": "7e850ad67d56f518cfcaff5307b2ebac542ae009c0fdbe493ad48700c78788f4",
      "source_category": "machine_draft",
      "review_status": "machine-draft-not-reviewed",
      "role": "occurrence",
      "role_basis": {
        "kind": "explicit-source-uuid-marker"
      },
      "label": "自发对称破缺(spontaneous symmetry breaking)",
      "context": {
        "range": [
          7417,
          8015
        ],
        "quote": "此时真空不是 $\\widehat N$ 的本征态，没有确定的粒子数。若 $[\\widehat N,\\widehat H]=0$，则 $|\\theta\\rangle$ 都具有与 $|0\\rangle$ 相同的能量，形成由 $\\theta$ 标记的不同真空。此时称 $U(1)$ 发生[<u class=\"concept-term\" data-concept-reference=\"concepts/quantum-mechanics/spontaneous-symmetry-breaking\" data-concept-identity=\"urn:uuid:ca209073-6b0b-4faa-b78f-0d00d3d11d24\" data-concept-route=\"/concept-identities#concept-ca209073-6b0b-4faa-b78f-0d00d3d11d24\" id=\"first-604a9d7ff08d53f734ab-zh\">自发对称破缺(spontaneous symmetry breaking)</u>](../../../../../concepts/quantum-mechanics/spontaneous-symmetry-breaking)。在超导体的非相对论场论描述中，电子配对降低能量并凝聚到最低能量态，该态没有确定的粒子数。",
        "quote_sha256": "babd8b8ebfc03b540e22a7e0eec22cfa9a3394fa97db7b84086dd9748a54377a",
        "environment": null,
        "excerpt_omitted": false
      },
      "parallel_readings": [
        {
          "route": "books/woit-qtgr/2025-10-20/en/chapter-39/04-spontaneous-symmetry-breaking",
          "lang": "en",
          "source_category": "machine_draft",
          "basis": "registered-book-edition-section-language-context; not-concept-equivalence"
        }
      ],
      "id": "occ-ce609113ade3c6905ff00b1c"
    },
    {
      "concept_id": "urn:uuid:ca209073-6b0b-4faa-b78f-0d00d3d11d24",
      "book_id": "woit-qtgr",
      "edition_id": "2025-10-20",
      "lang": "en",
      "route": "books/woit-qtgr/2025-10-20/en/chapter-39/04-spontaneous-symmetry-breaking",
      "anchor": "first-604a9d7ff08d53f734ab-en",
      "chapter": "39",
      "section": "39.4",
      "offset": 1262,
      "range": [
        7180,
        7510
      ],
      "source_revision": "371caea7902ae61115f6a48877b901c32e51f1fede2952ddd5e03374ad0e39cf",
      "source_category": "machine_draft",
      "review_status": "machine-draft-not-reviewed",
      "role": "occurrence",
      "role_basis": {
        "kind": "explicit-source-uuid-marker"
      },
      "label": "spontaneous symmetry breaking",
      "context": {
        "range": [
          6967,
          7733
        ],
        "quote": "The vacuum is not an eigenstate of $\\widehat N$ and has no definite particle number. If $[\\widehat N,\\widehat H]=0$, all $|\\theta\\rangle$ have the same energy. This vacuum degeneracy with non-invariant vacua is “[<u class=\"concept-term\" data-concept-reference=\"concepts/quantum-mechanics/spontaneous-symmetry-breaking\" data-concept-identity=\"urn:uuid:ca209073-6b0b-4faa-b78f-0d00d3d11d24\" data-concept-route=\"/concept-identities#concept-ca209073-6b0b-4faa-b78f-0d00d3d11d24\" id=\"first-604a9d7ff08d53f734ab-en\">spontaneous symmetry breaking</u>](../../../../../concepts/quantum-mechanics/spontaneous-symmetry-breaking)” of $U(1)$. In superconductivity, electrons pair in an energetically favorable way, condensing into a ground state without definite particle number.",
        "quote_sha256": "6089cf8e3bbed80b79c138cbe3039e62776557efe655530b76f00079e7188906",
        "environment": null,
        "excerpt_omitted": false
      },
      "parallel_readings": [
        {
          "route": "books/woit-qtgr/2025-10-20/zh/chapter-39/04-spontaneous-symmetry-breaking",
          "lang": "zh-CN",
          "source_category": "machine_draft",
          "basis": "registered-book-edition-section-language-context; not-concept-equivalence"
        }
      ],
      "id": "occ-a2892107ff1e00a1889c85fb"
    }
  ],
  "registered_positions": [
    {
      "route": "books/woit-qtgr/2025-10-20/en/chapter-39/04-spontaneous-symmetry-breaking",
      "lang": "en",
      "section": "39.4",
      "signal": "term-mark",
      "label": "spontaneous symmetry breaking",
      "english": "spontaneous symmetry breaking",
      "offset": 1262
    },
    {
      "route": "books/woit-qtgr/2025-10-20/zh/chapter-39/04-spontaneous-symmetry-breaking",
      "lang": "zh-CN",
      "section": "39.4",
      "signal": "term-mark",
      "label": "自发对称破缺",
      "english": "spontaneous symmetry breaking",
      "offset": 802
    }
  ],
  "statements": [],
  "resolved_references": [],
  "reading_order": [
    "occ-ce609113ade3c6905ff00b1c",
    "occ-a2892107ff1e00a1889c85fb"
  ],
  "recorded_dependencies": [],
  "reading_paths": [],
  "coverage": {
    "registered_positions": 2,
    "located_occurrences": 2,
    "whole_book_search_complete": false,
    "registered_positions_truncated": false,
    "independent_human_review_implied": false
  },
  "unresolved": [],
  "base_revision": "02a80c3ae51f3f687f696b77f50600ad35a689931573cfadac69618e85b85ca3",
  "optional_enrichments": []
}
