{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:74AMYHTUYZVAIA7F6UNPTGZR3R","short_pith_number":"pith:74AMYHTU","schema_version":"1.0","canonical_sha256":"ff00cc1e74c66a0403e5f51af99b31dc5eec512a25207e78f27173996050b852","source":{"kind":"arxiv","id":"2203.05004","version":2},"attestation_state":"computed","paper":{"title":"Nonlinear Bosonization of Fermi Surfaces: The Method of Coadjoint Orbits","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Dam Thanh Son, Luca V. Delacretaz, Umang Mehta, Yi-Hsien Du","submitted_at":"2022-03-09T19:02:40Z","abstract_excerpt":"We develop a new method for bosonizing the Fermi surface based on the formalism of the coadjoint orbits. This allows one to parametrize the Fermi surface by a bosonic field that depends on the spacetime coordinates and on the position on the Fermi surface. The Wess-Zumino-Witten term in the effective action, governing the adiabatic phase acquired when the Fermi surface changes its shape, is completely fixed. As an effective field theory the action also involves a Hamiltonian which contains, beside the kinetic energy and the Landau interaction, terms with arbitrary number of derivatives and fie"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2203.05004","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2022-03-09T19:02:40Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"f9d1d70d21f3a06e88fd756a40cbb3f962c86bd7f5b8fd3340a48c79305e779c","abstract_canon_sha256":"2992e5fe10346c296dc8fc5f3c07b6f023920f8b99c14c44797a8aa500377a6b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:52:49.689275Z","signature_b64":"bSpFQMYSeE1lppQ8Z/egQzNIZK61wQ2bA4Q9U4En5GY8NMGRBuOFGfKGtxg7v1KBZugdvWqoEciJrbBfl/q4Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ff00cc1e74c66a0403e5f51af99b31dc5eec512a25207e78f27173996050b852","last_reissued_at":"2026-07-05T04:52:49.688802Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:52:49.688802Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nonlinear Bosonization of Fermi Surfaces: The Method of Coadjoint Orbits","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Dam Thanh Son, Luca V. Delacretaz, Umang Mehta, Yi-Hsien Du","submitted_at":"2022-03-09T19:02:40Z","abstract_excerpt":"We develop a new method for bosonizing the Fermi surface based on the formalism of the coadjoint orbits. This allows one to parametrize the Fermi surface by a bosonic field that depends on the spacetime coordinates and on the position on the Fermi surface. The Wess-Zumino-Witten term in the effective action, governing the adiabatic phase acquired when the Fermi surface changes its shape, is completely fixed. As an effective field theory the action also involves a Hamiltonian which contains, beside the kinetic energy and the Landau interaction, terms with arbitrary number of derivatives and fie"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2203.05004","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2203.05004/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2203.05004","created_at":"2026-07-05T04:52:49.688861+00:00"},{"alias_kind":"arxiv_version","alias_value":"2203.05004v2","created_at":"2026-07-05T04:52:49.688861+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2203.05004","created_at":"2026-07-05T04:52:49.688861+00:00"},{"alias_kind":"pith_short_12","alias_value":"74AMYHTUYZVA","created_at":"2026-07-05T04:52:49.688861+00:00"},{"alias_kind":"pith_short_16","alias_value":"74AMYHTUYZVAIA7F","created_at":"2026-07-05T04:52:49.688861+00:00"},{"alias_kind":"pith_short_8","alias_value":"74AMYHTU","created_at":"2026-07-05T04:52:49.688861+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2512.04150","citing_title":"Symmetry-Enforced Fermi Surfaces","ref_index":28,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/74AMYHTUYZVAIA7F6UNPTGZR3R","json":"https://pith.science/pith/74AMYHTUYZVAIA7F6UNPTGZR3R.json","graph_json":"https://pith.science/api/pith-number/74AMYHTUYZVAIA7F6UNPTGZR3R/graph.json","events_json":"https://pith.science/api/pith-number/74AMYHTUYZVAIA7F6UNPTGZR3R/events.json","paper":"https://pith.science/paper/74AMYHTU"},"agent_actions":{"view_html":"https://pith.science/pith/74AMYHTUYZVAIA7F6UNPTGZR3R","download_json":"https://pith.science/pith/74AMYHTUYZVAIA7F6UNPTGZR3R.json","view_paper":"https://pith.science/paper/74AMYHTU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2203.05004&json=true","fetch_graph":"https://pith.science/api/pith-number/74AMYHTUYZVAIA7F6UNPTGZR3R/graph.json","fetch_events":"https://pith.science/api/pith-number/74AMYHTUYZVAIA7F6UNPTGZR3R/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/74AMYHTUYZVAIA7F6UNPTGZR3R/action/timestamp_anchor","attest_storage":"https://pith.science/pith/74AMYHTUYZVAIA7F6UNPTGZR3R/action/storage_attestation","attest_author":"https://pith.science/pith/74AMYHTUYZVAIA7F6UNPTGZR3R/action/author_attestation","sign_citation":"https://pith.science/pith/74AMYHTUYZVAIA7F6UNPTGZR3R/action/citation_signature","submit_replication":"https://pith.science/pith/74AMYHTUYZVAIA7F6UNPTGZR3R/action/replication_record"}},"created_at":"2026-07-05T04:52:49.688861+00:00","updated_at":"2026-07-05T04:52:49.688861+00:00"}