{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:IK3SRNEN5CD5BKAJNWXOVHBSMF","short_pith_number":"pith:IK3SRNEN","schema_version":"1.0","canonical_sha256":"42b728b48de887d0a8096daeea9c32614f0e8128a4fd1ab6520931a617dbe6f1","source":{"kind":"arxiv","id":"2206.04711","version":2},"attestation_state":"computed","paper":{"title":"Finite-Momentum Instability of Dynamical Axion Insulator","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Ioannis Petrides, Jonathan B. Curtis, Prineha Narang","submitted_at":"2022-06-09T18:02:53Z","abstract_excerpt":"The chiral anomaly is a striking signature of quantum effects which lead to the non-conservation of a classically conserved current, specifically the chiral currents in systems of fermions. In condensed matter systems, the chiral anomaly can be realized in Weyl semimetals, which then exhibit a signature electromagnetic response associated to anomaly due to the separation of the Weyl points in momentum space. In the presence of strong interactions however, a Weyl semimetal phase can give rise to an ordered phase, and spontaneously break the chiral symmetry. This then leads to a Goldstone mode w"},"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":"2206.04711","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2022-06-09T18:02:53Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"53f80d87ed6a22ce6777dea439032c3ac92269709dd9378f60e536125a3ab5fe","abstract_canon_sha256":"5eb8a4a32001fbe12f5c677aa08831852e1f90336a5663628156dd028305a1d5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:09:43.169744Z","signature_b64":"BMPkpC0jdMEBQ8G0cJ9TZoEMSEPZYBHdYgOLLd6AEWeceVofF7mRQBs9ucsmVO/7S8qbZozlECmMvVkQx4zdCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"42b728b48de887d0a8096daeea9c32614f0e8128a4fd1ab6520931a617dbe6f1","last_reissued_at":"2026-07-05T06:09:43.169307Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:09:43.169307Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Finite-Momentum Instability of Dynamical Axion Insulator","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Ioannis Petrides, Jonathan B. Curtis, Prineha Narang","submitted_at":"2022-06-09T18:02:53Z","abstract_excerpt":"The chiral anomaly is a striking signature of quantum effects which lead to the non-conservation of a classically conserved current, specifically the chiral currents in systems of fermions. In condensed matter systems, the chiral anomaly can be realized in Weyl semimetals, which then exhibit a signature electromagnetic response associated to anomaly due to the separation of the Weyl points in momentum space. In the presence of strong interactions however, a Weyl semimetal phase can give rise to an ordered phase, and spontaneously break the chiral symmetry. This then leads to a Goldstone mode w"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2206.04711","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/2206.04711/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":"2206.04711","created_at":"2026-07-05T06:09:43.169387+00:00"},{"alias_kind":"arxiv_version","alias_value":"2206.04711v2","created_at":"2026-07-05T06:09:43.169387+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2206.04711","created_at":"2026-07-05T06:09:43.169387+00:00"},{"alias_kind":"pith_short_12","alias_value":"IK3SRNEN5CD5","created_at":"2026-07-05T06:09:43.169387+00:00"},{"alias_kind":"pith_short_16","alias_value":"IK3SRNEN5CD5BKAJ","created_at":"2026-07-05T06:09:43.169387+00:00"},{"alias_kind":"pith_short_8","alias_value":"IK3SRNEN","created_at":"2026-07-05T06:09:43.169387+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/IK3SRNEN5CD5BKAJNWXOVHBSMF","json":"https://pith.science/pith/IK3SRNEN5CD5BKAJNWXOVHBSMF.json","graph_json":"https://pith.science/api/pith-number/IK3SRNEN5CD5BKAJNWXOVHBSMF/graph.json","events_json":"https://pith.science/api/pith-number/IK3SRNEN5CD5BKAJNWXOVHBSMF/events.json","paper":"https://pith.science/paper/IK3SRNEN"},"agent_actions":{"view_html":"https://pith.science/pith/IK3SRNEN5CD5BKAJNWXOVHBSMF","download_json":"https://pith.science/pith/IK3SRNEN5CD5BKAJNWXOVHBSMF.json","view_paper":"https://pith.science/paper/IK3SRNEN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2206.04711&json=true","fetch_graph":"https://pith.science/api/pith-number/IK3SRNEN5CD5BKAJNWXOVHBSMF/graph.json","fetch_events":"https://pith.science/api/pith-number/IK3SRNEN5CD5BKAJNWXOVHBSMF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IK3SRNEN5CD5BKAJNWXOVHBSMF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IK3SRNEN5CD5BKAJNWXOVHBSMF/action/storage_attestation","attest_author":"https://pith.science/pith/IK3SRNEN5CD5BKAJNWXOVHBSMF/action/author_attestation","sign_citation":"https://pith.science/pith/IK3SRNEN5CD5BKAJNWXOVHBSMF/action/citation_signature","submit_replication":"https://pith.science/pith/IK3SRNEN5CD5BKAJNWXOVHBSMF/action/replication_record"}},"created_at":"2026-07-05T06:09:43.169387+00:00","updated_at":"2026-07-05T06:09:43.169387+00:00"}