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        "quote": "是从李代数 $\\mathfrak g$ 到 $M$ 上函数所成李代数的李代数同态。若能如此选择常数，就称该作用为哈密顿 $G$-作用。若无法作出这样的选择，则称 $G$ 在经典相空间上的作用存在“[<u class=\"concept-term\" data-concept-reference=\"concepts/symplectic-geometry/moment-map-anomaly\" data-concept-identity=\"urn:uuid:82788b92-e7e2-458d-aa00-d14e5448427a\" data-concept-route=\"/concept-identities#concept-82788b92-e7e2-458d-aa00-d14e5448427a\" id=\"first-47bbbd204887dc38bdee-zh\">反常(moment-map anomaly)</u>](../../../../../concepts/symplectic-geometry/moment-map-anomaly)”。",
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        "quote": "正规序算符延拓到 $\\mathfrak{sp}(2d,\\mathbb R)$ 后，不再给出李代数同态；不过偏差仅是一个常数项。回顾[第15.3节](../chapter-15/03-group-actions-on-m-and-the-moment-map#section-15-3)，即使在经典层面，矩映射也只确定到一个加法常数；这可能造成一种“[<u class=\"concept-term\" data-concept-reference=\"concepts/symplectic-geometry/moment-map-anomaly\" data-concept-identity=\"urn:uuid:82788b92-e7e2-458d-aa00-d14e5448427a\" data-concept-route=\"/concept-identities#concept-82788b92-e7e2-458d-aa00-d14e5448427a\">反常(moment-map anomaly)</u>](../../../../../concepts/symplectic-geometry/moment-map-anomaly)”：矩映射因常数项而不再是李代数同态。这里的潜在反常可以通过平移消除。",
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