{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:KPO27AN7XKSSNLI4XC7V76MXUP","short_pith_number":"pith:KPO27AN7","canonical_record":{"source":{"id":"2501.00151","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2024-12-30T21:52:43Z","cross_cats_sorted":[],"title_canon_sha256":"a0d471d7cabb660347f3e8151d54fac8a98dc3916c69b55af6a7527a3763dac1","abstract_canon_sha256":"6e66276094d15846ec9ecdbcaa88340256956dff4bef103c055683b663b39537"},"schema_version":"1.0"},"canonical_sha256":"53ddaf81bfbaa526ad1cb8bf5ff997a3c34f018d799eb0d1bf39e9d4cacf270d","source":{"kind":"arxiv","id":"2501.00151","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2501.00151","created_at":"2026-07-05T11:23:21Z"},{"alias_kind":"arxiv_version","alias_value":"2501.00151v4","created_at":"2026-07-05T11:23:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2501.00151","created_at":"2026-07-05T11:23:21Z"},{"alias_kind":"pith_short_12","alias_value":"KPO27AN7XKSS","created_at":"2026-07-05T11:23:21Z"},{"alias_kind":"pith_short_16","alias_value":"KPO27AN7XKSSNLI4","created_at":"2026-07-05T11:23:21Z"},{"alias_kind":"pith_short_8","alias_value":"KPO27AN7","created_at":"2026-07-05T11:23:21Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:KPO27AN7XKSSNLI4XC7V76MXUP","target":"record","payload":{"canonical_record":{"source":{"id":"2501.00151","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2024-12-30T21:52:43Z","cross_cats_sorted":[],"title_canon_sha256":"a0d471d7cabb660347f3e8151d54fac8a98dc3916c69b55af6a7527a3763dac1","abstract_canon_sha256":"6e66276094d15846ec9ecdbcaa88340256956dff4bef103c055683b663b39537"},"schema_version":"1.0"},"canonical_sha256":"53ddaf81bfbaa526ad1cb8bf5ff997a3c34f018d799eb0d1bf39e9d4cacf270d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:23:21.972217Z","signature_b64":"pAOuuUXgUGjF/+ryZ/dMOSFT35MY4+cz7R6ir2AzTkO9aQEz/IF+XCFkrDXmKk02dtU7myei/K+4MVZkXGyjDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"53ddaf81bfbaa526ad1cb8bf5ff997a3c34f018d799eb0d1bf39e9d4cacf270d","last_reissued_at":"2026-07-05T11:23:21.971583Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:23:21.971583Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2501.00151","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":"2026-07-05T11:23:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"InqOezSQlKO4sQ8MPoDhyE/1wmyz7DlPDEEWMq2FE91aBx0hI3I/2sX3Tcp0PaCWAc+TA5Bcjg9VjlxxQ8TgBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T15:46:21.849246Z"},"content_sha256":"f6da94f78b325fa78cf9ba09569841a5f7f24134dbdb7b42a28604b5a9b697c0","schema_version":"1.0","event_id":"sha256:f6da94f78b325fa78cf9ba09569841a5f7f24134dbdb7b42a28604b5a9b697c0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:KPO27AN7XKSSNLI4XC7V76MXUP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Effective Lagrangian for the macroscopic motion of Weyl fermions in $^3$He-A","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"M. A. Zubkov, M. Selch","submitted_at":"2024-12-30T21:52:43Z","abstract_excerpt":"We consider macroscopic motion of the normal component of superfluid $^3$He - A in global thermodynamic equilibrium within the context of the Zubarev statistical operator method. We formulate the corresponding effective theory in the language of the functional integral. The effective Lagrangian comprising macroscopic motion of fermionic excitations is calculated explicitly for the emergent relativistic fermions of the superfluid $^3$He - A phase immersed in a non-trivial bosonic background due to a space and time dependent matrix-valued vierbein featuring nonzero torsion as well as the Nieh-Ya"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2501.00151","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2501.00151/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T11:23:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cg2p1iBN8ftkl0ZxGBeRPrusYMvkXr7DlbQm7X0pbPe+jryfNcUr0f3dEkXy10VdHkABx3CA9ENxbHriDSGmCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T15:46:21.849803Z"},"content_sha256":"a2f9cf6c0d45c34ae7bd88b609f64fd0ea83b239de9ca09120e61fb030f0c2d2","schema_version":"1.0","event_id":"sha256:a2f9cf6c0d45c34ae7bd88b609f64fd0ea83b239de9ca09120e61fb030f0c2d2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KPO27AN7XKSSNLI4XC7V76MXUP/bundle.json","state_url":"https://pith.science/pith/KPO27AN7XKSSNLI4XC7V76MXUP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KPO27AN7XKSSNLI4XC7V76MXUP/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":"2026-08-11T15:46:21Z","links":{"resolver":"https://pith.science/pith/KPO27AN7XKSSNLI4XC7V76MXUP","bundle":"https://pith.science/pith/KPO27AN7XKSSNLI4XC7V76MXUP/bundle.json","state":"https://pith.science/pith/KPO27AN7XKSSNLI4XC7V76MXUP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KPO27AN7XKSSNLI4XC7V76MXUP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:KPO27AN7XKSSNLI4XC7V76MXUP","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":"6e66276094d15846ec9ecdbcaa88340256956dff4bef103c055683b663b39537","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2024-12-30T21:52:43Z","title_canon_sha256":"a0d471d7cabb660347f3e8151d54fac8a98dc3916c69b55af6a7527a3763dac1"},"schema_version":"1.0","source":{"id":"2501.00151","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2501.00151","created_at":"2026-07-05T11:23:21Z"},{"alias_kind":"arxiv_version","alias_value":"2501.00151v4","created_at":"2026-07-05T11:23:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2501.00151","created_at":"2026-07-05T11:23:21Z"},{"alias_kind":"pith_short_12","alias_value":"KPO27AN7XKSS","created_at":"2026-07-05T11:23:21Z"},{"alias_kind":"pith_short_16","alias_value":"KPO27AN7XKSSNLI4","created_at":"2026-07-05T11:23:21Z"},{"alias_kind":"pith_short_8","alias_value":"KPO27AN7","created_at":"2026-07-05T11:23:21Z"}],"graph_snapshots":[{"event_id":"sha256:a2f9cf6c0d45c34ae7bd88b609f64fd0ea83b239de9ca09120e61fb030f0c2d2","target":"graph","created_at":"2026-07-05T11:23:21Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2501.00151/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We consider macroscopic motion of the normal component of superfluid $^3$He - A in global thermodynamic equilibrium within the context of the Zubarev statistical operator method. We formulate the corresponding effective theory in the language of the functional integral. The effective Lagrangian comprising macroscopic motion of fermionic excitations is calculated explicitly for the emergent relativistic fermions of the superfluid $^3$He - A phase immersed in a non-trivial bosonic background due to a space and time dependent matrix-valued vierbein featuring nonzero torsion as well as the Nieh-Ya","authors_text":"M. A. Zubkov, M. Selch","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2024-12-30T21:52:43Z","title":"Effective Lagrangian for the macroscopic motion of Weyl fermions in $^3$He-A"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2501.00151","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:f6da94f78b325fa78cf9ba09569841a5f7f24134dbdb7b42a28604b5a9b697c0","target":"record","created_at":"2026-07-05T11:23:21Z","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":"6e66276094d15846ec9ecdbcaa88340256956dff4bef103c055683b663b39537","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2024-12-30T21:52:43Z","title_canon_sha256":"a0d471d7cabb660347f3e8151d54fac8a98dc3916c69b55af6a7527a3763dac1"},"schema_version":"1.0","source":{"id":"2501.00151","kind":"arxiv","version":4}},"canonical_sha256":"53ddaf81bfbaa526ad1cb8bf5ff997a3c34f018d799eb0d1bf39e9d4cacf270d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"53ddaf81bfbaa526ad1cb8bf5ff997a3c34f018d799eb0d1bf39e9d4cacf270d","first_computed_at":"2026-07-05T11:23:21.971583Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:23:21.971583Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"pAOuuUXgUGjF/+ryZ/dMOSFT35MY4+cz7R6ir2AzTkO9aQEz/IF+XCFkrDXmKk02dtU7myei/K+4MVZkXGyjDQ==","signature_status":"signed_v1","signed_at":"2026-07-05T11:23:21.972217Z","signed_message":"canonical_sha256_bytes"},"source_id":"2501.00151","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f6da94f78b325fa78cf9ba09569841a5f7f24134dbdb7b42a28604b5a9b697c0","sha256:a2f9cf6c0d45c34ae7bd88b609f64fd0ea83b239de9ca09120e61fb030f0c2d2"],"state_sha256":"313757f3b875f0eb98af2200d4e7e417d7087d8255200790bc7e5914991d67ab"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NhcTq7kmH18qA9Py3CCK8Mf84oXbVEFLybOKQRruh7pcABniwi+Kk4rMIyp7hgeZuai15n/QT612exNDPtdLCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-11T15:46:21.856082Z","bundle_sha256":"c3e7f24cb07d347e523b0fc9e4e44ee8dce96aa031f1ed8cac6747c1edf43251"}}