{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:JCJVUNTWWWRK4BPDEQEUONDMFK","short_pith_number":"pith:JCJVUNTW","canonical_record":{"source":{"id":"2605.14958","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2026-05-14T15:26:44Z","cross_cats_sorted":["astro-ph.SR"],"title_canon_sha256":"2c4d367f4d8d073a5229f41119290aee868922423e71e6fa53b5a7d2ad6ef8cd","abstract_canon_sha256":"31f6ed56dc51edf66b8d251bc935c3b621c7aa1db410b9f353cea50893602c02"},"schema_version":"1.0"},"canonical_sha256":"48935a3676b5a2ae05e3240947346c2a875e9fe6e4a8f354e046ff2d7afac308","source":{"kind":"arxiv","id":"2605.14958","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.14958","created_at":"2026-05-17T23:38:55Z"},{"alias_kind":"arxiv_version","alias_value":"2605.14958v1","created_at":"2026-05-17T23:38:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.14958","created_at":"2026-05-17T23:38:55Z"},{"alias_kind":"pith_short_12","alias_value":"JCJVUNTWWWRK","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_16","alias_value":"JCJVUNTWWWRK4BPD","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_8","alias_value":"JCJVUNTW","created_at":"2026-05-18T12:33:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:JCJVUNTWWWRK4BPDEQEUONDMFK","target":"record","payload":{"canonical_record":{"source":{"id":"2605.14958","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2026-05-14T15:26:44Z","cross_cats_sorted":["astro-ph.SR"],"title_canon_sha256":"2c4d367f4d8d073a5229f41119290aee868922423e71e6fa53b5a7d2ad6ef8cd","abstract_canon_sha256":"31f6ed56dc51edf66b8d251bc935c3b621c7aa1db410b9f353cea50893602c02"},"schema_version":"1.0"},"canonical_sha256":"48935a3676b5a2ae05e3240947346c2a875e9fe6e4a8f354e046ff2d7afac308","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:38:55.313993Z","signature_b64":"znGsqN1K6r1z30hA86aJ4drZgTsH7kfQ8NB0BxrgTxD2yXW//1EDN/coEm6WBj7RlV4zORXXkNjQZEWLMyDBAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"48935a3676b5a2ae05e3240947346c2a875e9fe6e4a8f354e046ff2d7afac308","last_reissued_at":"2026-05-17T23:38:55.313378Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:38:55.313378Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2605.14958","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:38:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LBynRGotzFTlfKiFAJPaxMBdJhgjmZdy/hZHut4iCFhrTtcAtrU2TcO0dD562ExfLi44C0Xdur3YzlHFlc2eCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T23:04:51.244824Z"},"content_sha256":"73e055ae4c54ef0d2b0e1c4df0b33290f430fdbd326a40746ddd1eda611d8d72","schema_version":"1.0","event_id":"sha256:73e055ae4c54ef0d2b0e1c4df0b33290f430fdbd326a40746ddd1eda611d8d72"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:JCJVUNTWWWRK4BPDEQEUONDMFK","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Conservative and dissipative sectors in a nonlinear scalar model for the gravitational self-force problem","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["astro-ph.SR"],"primary_cat":"gr-qc","authors_text":"Abraham I. Harte, Eanna E. Flanagan, Francisco M. Blanco","submitted_at":"2026-05-14T15:26:44Z","abstract_excerpt":"When considering how self-interaction affects an object's motion, it can be convenient to decompose the self-force into conservative and dissipative pieces. As a toy model for understanding such decompositions of the gravitational self-force, we consider objects that do not affect the spacetime, but are instead coupled to a nonlinear scalar field. There is then a standard splitting of the first-order scalar self-force into conservative and dissipative components. Multiple criteria can be used to obtain this splitting, all of which imply the same result. However, the implications of these crite"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2605.14958","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":""},"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":"2026-05-17T23:38:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"chqQazkeuxmQTRX50dJlu6LAgkuiTDaujt8JDkQFNPVA4kp6EpJP1mVHg0OEc/hWE7NBTRGNXAiDmDW1ZHHpAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T23:04:51.245694Z"},"content_sha256":"ae8122e4b6d7c968f574636c3008666d69b992b308dae21c7d039f80b8b41a68","schema_version":"1.0","event_id":"sha256:ae8122e4b6d7c968f574636c3008666d69b992b308dae21c7d039f80b8b41a68"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JCJVUNTWWWRK4BPDEQEUONDMFK/bundle.json","state_url":"https://pith.science/pith/JCJVUNTWWWRK4BPDEQEUONDMFK/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JCJVUNTWWWRK4BPDEQEUONDMFK/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":"2026-05-31T23:04:51Z","links":{"resolver":"https://pith.science/pith/JCJVUNTWWWRK4BPDEQEUONDMFK","bundle":"https://pith.science/pith/JCJVUNTWWWRK4BPDEQEUONDMFK/bundle.json","state":"https://pith.science/pith/JCJVUNTWWWRK4BPDEQEUONDMFK/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JCJVUNTWWWRK4BPDEQEUONDMFK/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:JCJVUNTWWWRK4BPDEQEUONDMFK","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":"31f6ed56dc51edf66b8d251bc935c3b621c7aa1db410b9f353cea50893602c02","cross_cats_sorted":["astro-ph.SR"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2026-05-14T15:26:44Z","title_canon_sha256":"2c4d367f4d8d073a5229f41119290aee868922423e71e6fa53b5a7d2ad6ef8cd"},"schema_version":"1.0","source":{"id":"2605.14958","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.14958","created_at":"2026-05-17T23:38:55Z"},{"alias_kind":"arxiv_version","alias_value":"2605.14958v1","created_at":"2026-05-17T23:38:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.14958","created_at":"2026-05-17T23:38:55Z"},{"alias_kind":"pith_short_12","alias_value":"JCJVUNTWWWRK","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_16","alias_value":"JCJVUNTWWWRK4BPD","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_8","alias_value":"JCJVUNTW","created_at":"2026-05-18T12:33:37Z"}],"graph_snapshots":[{"event_id":"sha256:ae8122e4b6d7c968f574636c3008666d69b992b308dae21c7d039f80b8b41a68","target":"graph","created_at":"2026-05-17T23:38:55Z","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":"When considering how self-interaction affects an object's motion, it can be convenient to decompose the self-force into conservative and dissipative pieces. As a toy model for understanding such decompositions of the gravitational self-force, we consider objects that do not affect the spacetime, but are instead coupled to a nonlinear scalar field. There is then a standard splitting of the first-order scalar self-force into conservative and dissipative components. Multiple criteria can be used to obtain this splitting, all of which imply the same result. However, the implications of these crite","authors_text":"Abraham I. Harte, Eanna E. Flanagan, Francisco M. Blanco","cross_cats":["astro-ph.SR"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2026-05-14T15:26:44Z","title":"Conservative and dissipative sectors in a nonlinear scalar model for the gravitational self-force problem"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2605.14958","kind":"arxiv","version":1},"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":"sha256:73e055ae4c54ef0d2b0e1c4df0b33290f430fdbd326a40746ddd1eda611d8d72","target":"record","created_at":"2026-05-17T23:38:55Z","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":"31f6ed56dc51edf66b8d251bc935c3b621c7aa1db410b9f353cea50893602c02","cross_cats_sorted":["astro-ph.SR"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2026-05-14T15:26:44Z","title_canon_sha256":"2c4d367f4d8d073a5229f41119290aee868922423e71e6fa53b5a7d2ad6ef8cd"},"schema_version":"1.0","source":{"id":"2605.14958","kind":"arxiv","version":1}},"canonical_sha256":"48935a3676b5a2ae05e3240947346c2a875e9fe6e4a8f354e046ff2d7afac308","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"48935a3676b5a2ae05e3240947346c2a875e9fe6e4a8f354e046ff2d7afac308","first_computed_at":"2026-05-17T23:38:55.313378Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:38:55.313378Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"znGsqN1K6r1z30hA86aJ4drZgTsH7kfQ8NB0BxrgTxD2yXW//1EDN/coEm6WBj7RlV4zORXXkNjQZEWLMyDBAw==","signature_status":"signed_v1","signed_at":"2026-05-17T23:38:55.313993Z","signed_message":"canonical_sha256_bytes"},"source_id":"2605.14958","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:73e055ae4c54ef0d2b0e1c4df0b33290f430fdbd326a40746ddd1eda611d8d72","sha256:ae8122e4b6d7c968f574636c3008666d69b992b308dae21c7d039f80b8b41a68"],"state_sha256":"961029666d97247e041a4fdf11d0c98b34cb568a3d97adeaa9c1e2fc46e2c388"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DQNrb9PYHVgGZQWf07LetDyLShtTP846CgqIPtZ6txGtWrNs0o0+JWQsDwb47JpGrogXbDhTTzZnyD6R0bEkCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T23:04:51.250406Z","bundle_sha256":"f14457cdea8ffa21524a8e5e54511514b0ff4ee9020638f13a204c737aaae3e3"}}