{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2004:EAFDRGCEYMAYUGVAWR5AM5QGNP","short_pith_number":"pith:EAFDRGCE","schema_version":"1.0","canonical_sha256":"200a389844c3018a1aa0b47a0676066be895fc925c8f4a926156eb669d4b1260","source":{"kind":"arxiv","id":"hep-th/0406052","version":1},"attestation_state":"computed","paper":{"title":"Conserved gravitational charges from Yano tensors","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"David Kastor, Jennie Traschen","submitted_at":"2004-06-04T18:06:53Z","abstract_excerpt":"The defining properties of Yano tensors naturally generalize those of Killing vectors to anti-symmetric tensor fields of arbitrary rank. We show how the Yano tensors of flat spacetime can be used to construct new, conserved gravitational charges for transverse asymptotically flat spacetimes. The relationship of these new charges to Yano tensors parallels that of ordinary ADM conserved charges to Killing vectors. Hence, we call them Y-ADM charges. A rank n Y-ADM charge is given by an integral over a co-dimension $n$ slice of spatial infinity. In particular, a rank (p+1) Y-ADM charge in a p-bran"},"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":"hep-th/0406052","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2004-06-04T18:06:53Z","cross_cats_sorted":[],"title_canon_sha256":"5ee217ff34cdb4540ff8bdf4130239c9746bbab76b581cdb5eb86254590d4a9a","abstract_canon_sha256":"db7ee0d334a663144642a8a8b2add31c0cc204b1fa3cdb84b29e831e61fed6b2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:21:09.858685Z","signature_b64":"OKkYm95dMnOeNh7i2ZP6X35xiCjwGJP9q5o15KH0I33xeIwB6cWG5oMJTWQKytLOmw61QuzrV4sCywVAuBagBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"200a389844c3018a1aa0b47a0676066be895fc925c8f4a926156eb669d4b1260","last_reissued_at":"2026-07-04T17:21:09.858259Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:21:09.858259Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Conserved gravitational charges from Yano tensors","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"David Kastor, Jennie Traschen","submitted_at":"2004-06-04T18:06:53Z","abstract_excerpt":"The defining properties of Yano tensors naturally generalize those of Killing vectors to anti-symmetric tensor fields of arbitrary rank. We show how the Yano tensors of flat spacetime can be used to construct new, conserved gravitational charges for transverse asymptotically flat spacetimes. The relationship of these new charges to Yano tensors parallels that of ordinary ADM conserved charges to Killing vectors. Hence, we call them Y-ADM charges. A rank n Y-ADM charge is given by an integral over a co-dimension $n$ slice of spatial infinity. In particular, a rank (p+1) Y-ADM charge in a p-bran"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0406052","kind":"arxiv","version":1},"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/hep-th/0406052/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":"hep-th/0406052","created_at":"2026-07-04T17:21:09.858322+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0406052v1","created_at":"2026-07-04T17:21:09.858322+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0406052","created_at":"2026-07-04T17:21:09.858322+00:00"},{"alias_kind":"pith_short_12","alias_value":"EAFDRGCEYMAY","created_at":"2026-07-04T17:21:09.858322+00:00"},{"alias_kind":"pith_short_16","alias_value":"EAFDRGCEYMAYUGVA","created_at":"2026-07-04T17:21:09.858322+00:00"},{"alias_kind":"pith_short_8","alias_value":"EAFDRGCE","created_at":"2026-07-04T17:21:09.858322+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.10503","citing_title":"Gauge-invariant charges of the dual graviton","ref_index":21,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/EAFDRGCEYMAYUGVAWR5AM5QGNP","json":"https://pith.science/pith/EAFDRGCEYMAYUGVAWR5AM5QGNP.json","graph_json":"https://pith.science/api/pith-number/EAFDRGCEYMAYUGVAWR5AM5QGNP/graph.json","events_json":"https://pith.science/api/pith-number/EAFDRGCEYMAYUGVAWR5AM5QGNP/events.json","paper":"https://pith.science/paper/EAFDRGCE"},"agent_actions":{"view_html":"https://pith.science/pith/EAFDRGCEYMAYUGVAWR5AM5QGNP","download_json":"https://pith.science/pith/EAFDRGCEYMAYUGVAWR5AM5QGNP.json","view_paper":"https://pith.science/paper/EAFDRGCE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0406052&json=true","fetch_graph":"https://pith.science/api/pith-number/EAFDRGCEYMAYUGVAWR5AM5QGNP/graph.json","fetch_events":"https://pith.science/api/pith-number/EAFDRGCEYMAYUGVAWR5AM5QGNP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EAFDRGCEYMAYUGVAWR5AM5QGNP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EAFDRGCEYMAYUGVAWR5AM5QGNP/action/storage_attestation","attest_author":"https://pith.science/pith/EAFDRGCEYMAYUGVAWR5AM5QGNP/action/author_attestation","sign_citation":"https://pith.science/pith/EAFDRGCEYMAYUGVAWR5AM5QGNP/action/citation_signature","submit_replication":"https://pith.science/pith/EAFDRGCEYMAYUGVAWR5AM5QGNP/action/replication_record"}},"created_at":"2026-07-04T17:21:09.858322+00:00","updated_at":"2026-07-04T17:21:09.858322+00:00"}