{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:2RHS7PYENUWLNQYYH4AG3AD2EX","short_pith_number":"pith:2RHS7PYE","canonical_record":{"source":{"id":"1409.0414","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2014-09-01T13:24:12Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"80d7280295bd7f147d7c71a2064906ed0632c1eec234976e75b72b4c7a952fa0","abstract_canon_sha256":"0e05692739bf26969d3f82b4fa3f749ec97a283320aab625a97ff257df86362f"},"schema_version":"1.0"},"canonical_sha256":"d44f2fbf046d2cb6c3183f006d807a25c9b9e794668c91e2d1b6c23077b653d3","source":{"kind":"arxiv","id":"1409.0414","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.0414","created_at":"2026-05-18T00:44:42Z"},{"alias_kind":"arxiv_version","alias_value":"1409.0414v4","created_at":"2026-05-18T00:44:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.0414","created_at":"2026-05-18T00:44:42Z"},{"alias_kind":"pith_short_12","alias_value":"2RHS7PYENUWL","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_16","alias_value":"2RHS7PYENUWLNQYY","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_8","alias_value":"2RHS7PYE","created_at":"2026-05-18T12:28:11Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:2RHS7PYENUWLNQYYH4AG3AD2EX","target":"record","payload":{"canonical_record":{"source":{"id":"1409.0414","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2014-09-01T13:24:12Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"80d7280295bd7f147d7c71a2064906ed0632c1eec234976e75b72b4c7a952fa0","abstract_canon_sha256":"0e05692739bf26969d3f82b4fa3f749ec97a283320aab625a97ff257df86362f"},"schema_version":"1.0"},"canonical_sha256":"d44f2fbf046d2cb6c3183f006d807a25c9b9e794668c91e2d1b6c23077b653d3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:44:42.750219Z","signature_b64":"M1/zihUJA9R1wqgjGb8za/Rp781T3cOKkfO1GpZdHvQ9oCN8b8eXWLhZ62yJRv3EGDCHjZaMXhddBDV93uIEBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d44f2fbf046d2cb6c3183f006d807a25c9b9e794668c91e2d1b6c23077b653d3","last_reissued_at":"2026-05-18T00:44:42.749782Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:44:42.749782Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1409.0414","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:44:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hpSW2KFUmOcnMvx2yHGRhWsb6FFSaZTva3JRDJdzFz96d5SvxjMMB8X4ATfmeqAZ8gc8jvuRan/rUb1ofkXlCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-20T17:55:48.115702Z"},"content_sha256":"2cc0f420490560dbee2faa542e1e690ecbef57066cb39e3ded42f72cea55347f","schema_version":"1.0","event_id":"sha256:2cc0f420490560dbee2faa542e1e690ecbef57066cb39e3ded42f72cea55347f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:2RHS7PYENUWLNQYYH4AG3AD2EX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"A topological Fermi-liquid theory for interacting Weyl metals with time reversal symmetry breaking","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Jae-Ho Han, Ki-Seok Kim, Yong-Soo Jho","submitted_at":"2014-09-01T13:24:12Z","abstract_excerpt":"Introducing both Berry curvature and chiral anomaly into Landau's Fermi-liquid theory, we construct a topological Fermi-liquid theory, applicable to interacting Weyl metals in the absence of time reversal symmetry. Following the Landau's Fermi-liquid theory, we obtain an effective free-energy functional in terms of the density field of chiral fermions. The density field of chiral fermions is determined by a self-consistent equation, minimizing the effective free-energy functional with respect to the order-parameter field. Beyond these thermodynamic properties, we construct Boltzmann transport "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.0414","kind":"arxiv","version":4},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:44:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"btNKUuDME92rrxEUxLNspN1gq193rg+PtqOhorKg+IN8Zp7aXDWj/ekTvEd9X/kTWnI+fDFD1UORQCIaMK/IAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-20T17:55:48.116092Z"},"content_sha256":"60f2523570a62a81fc97409603bf3e2426dabbb1e55245dba3021cabc265d3bd","schema_version":"1.0","event_id":"sha256:60f2523570a62a81fc97409603bf3e2426dabbb1e55245dba3021cabc265d3bd"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2RHS7PYENUWLNQYYH4AG3AD2EX/bundle.json","state_url":"https://pith.science/pith/2RHS7PYENUWLNQYYH4AG3AD2EX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2RHS7PYENUWLNQYYH4AG3AD2EX/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-20T17:55:48Z","links":{"resolver":"https://pith.science/pith/2RHS7PYENUWLNQYYH4AG3AD2EX","bundle":"https://pith.science/pith/2RHS7PYENUWLNQYYH4AG3AD2EX/bundle.json","state":"https://pith.science/pith/2RHS7PYENUWLNQYYH4AG3AD2EX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2RHS7PYENUWLNQYYH4AG3AD2EX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:2RHS7PYENUWLNQYYH4AG3AD2EX","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"0e05692739bf26969d3f82b4fa3f749ec97a283320aab625a97ff257df86362f","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2014-09-01T13:24:12Z","title_canon_sha256":"80d7280295bd7f147d7c71a2064906ed0632c1eec234976e75b72b4c7a952fa0"},"schema_version":"1.0","source":{"id":"1409.0414","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.0414","created_at":"2026-05-18T00:44:42Z"},{"alias_kind":"arxiv_version","alias_value":"1409.0414v4","created_at":"2026-05-18T00:44:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.0414","created_at":"2026-05-18T00:44:42Z"},{"alias_kind":"pith_short_12","alias_value":"2RHS7PYENUWL","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_16","alias_value":"2RHS7PYENUWLNQYY","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_8","alias_value":"2RHS7PYE","created_at":"2026-05-18T12:28:11Z"}],"graph_snapshots":[{"event_id":"sha256:60f2523570a62a81fc97409603bf3e2426dabbb1e55245dba3021cabc265d3bd","target":"graph","created_at":"2026-05-18T00:44:42Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"Introducing both Berry curvature and chiral anomaly into Landau's Fermi-liquid theory, we construct a topological Fermi-liquid theory, applicable to interacting Weyl metals in the absence of time reversal symmetry. Following the Landau's Fermi-liquid theory, we obtain an effective free-energy functional in terms of the density field of chiral fermions. The density field of chiral fermions is determined by a self-consistent equation, minimizing the effective free-energy functional with respect to the order-parameter field. Beyond these thermodynamic properties, we construct Boltzmann transport ","authors_text":"Jae-Ho Han, Ki-Seok Kim, Yong-Soo Jho","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2014-09-01T13:24:12Z","title":"A topological Fermi-liquid theory for interacting Weyl metals with time reversal symmetry breaking"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.0414","kind":"arxiv","version":4},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:2cc0f420490560dbee2faa542e1e690ecbef57066cb39e3ded42f72cea55347f","target":"record","created_at":"2026-05-18T00:44:42Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"0e05692739bf26969d3f82b4fa3f749ec97a283320aab625a97ff257df86362f","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2014-09-01T13:24:12Z","title_canon_sha256":"80d7280295bd7f147d7c71a2064906ed0632c1eec234976e75b72b4c7a952fa0"},"schema_version":"1.0","source":{"id":"1409.0414","kind":"arxiv","version":4}},"canonical_sha256":"d44f2fbf046d2cb6c3183f006d807a25c9b9e794668c91e2d1b6c23077b653d3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d44f2fbf046d2cb6c3183f006d807a25c9b9e794668c91e2d1b6c23077b653d3","first_computed_at":"2026-05-18T00:44:42.749782Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:44:42.749782Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"M1/zihUJA9R1wqgjGb8za/Rp781T3cOKkfO1GpZdHvQ9oCN8b8eXWLhZ62yJRv3EGDCHjZaMXhddBDV93uIEBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:44:42.750219Z","signed_message":"canonical_sha256_bytes"},"source_id":"1409.0414","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2cc0f420490560dbee2faa542e1e690ecbef57066cb39e3ded42f72cea55347f","sha256:60f2523570a62a81fc97409603bf3e2426dabbb1e55245dba3021cabc265d3bd"],"state_sha256":"4b03655297b4c47c523e815c01d40229e9ac3af97a51ef1eb30a6667460d6bfe"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6PXonVB6mx0qKHT+WsO6WqbqeUcayJze935DgV4az2Z0O4Oc9N3ABFLd5P1DDPtXcqpGScfgjCaKMlhhguMPBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-20T17:55:48.118705Z","bundle_sha256":"70ee9f448a0626123d4f28164b936bf6b1e10b5f0dbe7d9ae1c765a87d9deda8"}}