{
  "schema_version": 1,
  "kind": "ConceptView",
  "producer": "concept-view-1",
  "concept_id": "urn:uuid:d18ab3a8-acf6-4147-afc2-e59c5c4630dd",
  "labels": {
    "zh-CN": "运动常量",
    "en": "constant of the motion"
  },
  "alternative_labels": [],
  "scope_note": "",
  "identity_status": "active",
  "identity_revision": "a2e6b071c829539c454cbc564e03de7ee2a186a986f991cd795a3bd02affb627",
  "occurrences": [
    {
      "concept_id": "urn:uuid:d18ab3a8-acf6-4147-afc2-e59c5c4630dd",
      "book_id": "szekeres",
      "edition_id": "source-snapshot-bc3404156f6e",
      "lang": "zh-CN",
      "route": "zh/chapter-14/03-symmetry-transformations",
      "anchor": "first-d8af141658dc540dd209-zh",
      "chapter": "14",
      "section": "14.3",
      "offset": 17743,
      "range": [
        25013,
        25260
      ],
      "source_revision": "bd46fa60bca66ad8e9e72bb6b593e0bd7bca1ecd3fedf001a84980e27aa738c9",
      "source_category": "translation",
      "review_status": "unreviewed",
      "role": "occurrence",
      "role_basis": {
        "kind": "explicit-source-uuid-marker"
      },
      "label": "运动常量(constant of the motion)",
      "context": {
        "range": [
          24986,
          25283
        ],
        "quote": "任何满足此方程的厄米算符 $S ( t )$ 都称为 <u class=\"concept-term\" data-concept-identity=\"urn:uuid:d18ab3a8-acf6-4147-afc2-e59c5c4630dd\" data-concept-route=\"/concept-identities#concept-d18ab3a8-acf6-4147-afc2-e59c5c4630dd\" id=\"first-d8af141658dc540dd209-zh\">运动常量(constant of the motion)</u> 或守恒量，因为薛定谔方程意味着其期望值恒定：",
        "quote_sha256": "cf480b4c65e048ee8edf1bd3acf54229206c3be2a0924d44cb10cd505ff7f448",
        "environment": null,
        "excerpt_omitted": false
      },
      "parallel_readings": [
        {
          "route": "en/chapter-14/03-symmetry-transformations",
          "lang": "en",
          "source_category": "original_transcription",
          "basis": "registered-book-edition-section-language-context; not-concept-equivalence"
        }
      ],
      "id": "occ-7e619cba0c95fae6ee9bca2b"
    },
    {
      "concept_id": "urn:uuid:d18ab3a8-acf6-4147-afc2-e59c5c4630dd",
      "book_id": "szekeres",
      "edition_id": "source-snapshot-bc3404156f6e",
      "lang": "en",
      "route": "en/chapter-14/03-symmetry-transformations",
      "anchor": "first-d8af141658dc540dd209-en",
      "chapter": "14",
      "section": "14.3",
      "offset": 22221,
      "range": [
        29020,
        29261
      ],
      "source_revision": "885f6b65616f6ba21a44d214be830aa08bddd11a84ea6bff81aef0b641e094d5",
      "source_category": "original_transcription",
      "review_status": "unreviewed",
      "role": "occurrence",
      "role_basis": {
        "kind": "explicit-source-uuid-marker"
      },
      "label": "constant of the motion",
      "context": {
        "range": [
          28946,
          29359
        ],
        "quote": "Any hermitian operator $S ( t )$ satisfying this equation is said to be a <u class=\"concept-term\" data-concept-identity=\"urn:uuid:d18ab3a8-acf6-4147-afc2-e59c5c4630dd\" data-concept-route=\"/concept-identities#concept-d18ab3a8-acf6-4147-afc2-e59c5c4630dd\" id=\"first-d8af141658dc540dd209-en\">constant of the motion</u> or conserved quantity, for Schrödinger’s equation implies that its expection values are constant:",
        "quote_sha256": "337bb1121df7a2343211c0c7375acd2ad14c381965d351a5178e15672b908113",
        "environment": null,
        "excerpt_omitted": false
      },
      "parallel_readings": [
        {
          "route": "zh/chapter-14/03-symmetry-transformations",
          "lang": "zh-CN",
          "source_category": "translation",
          "basis": "registered-book-edition-section-language-context; not-concept-equivalence"
        }
      ],
      "id": "occ-35a4e6e8ec272056f9651fb9"
    }
  ],
  "registered_positions": [
    {
      "route": "en/chapter-14/03-symmetry-transformations",
      "lang": "en",
      "section": "14.3",
      "signal": "term-mark",
      "label": "constant of the motion",
      "english": "constant of the motion",
      "offset": 21039
    },
    {
      "route": "zh/chapter-14/03-symmetry-transformations",
      "lang": "zh-CN",
      "section": "14.3",
      "signal": "term-mark",
      "label": "运动常量",
      "english": "constant of the motion",
      "offset": 16561
    }
  ],
  "statements": [],
  "resolved_references": [],
  "reading_order": [
    "occ-7e619cba0c95fae6ee9bca2b",
    "occ-35a4e6e8ec272056f9651fb9"
  ],
  "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": "5d9fe76764319203c55fff62467c02bf4a2053c0acd7feaaa2da28b15ccacae3",
  "optional_enrichments": []
}
