{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:DAXH33UKZEFJ6AQV6GX6PQQZMT","short_pith_number":"pith:DAXH33UK","canonical_record":{"source":{"id":"2406.03457","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2024-06-05T17:01:55Z","cross_cats_sorted":[],"title_canon_sha256":"8b189fc6395ec71901b8601e36cdbafaa713e7fdf226429f3a7fac255b023e2f","abstract_canon_sha256":"b32a8d5522575e04610a1ec932734b6650ab0e9bacf6d404bbdbdfe1abb81807"},"schema_version":"1.0"},"canonical_sha256":"182e7dee8ac90a9f0215f1afe7c21964cc570e5c3fe08b0b6f2d89bf5f1f2367","source":{"kind":"arxiv","id":"2406.03457","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2406.03457","created_at":"2026-07-05T08:58:44Z"},{"alias_kind":"arxiv_version","alias_value":"2406.03457v2","created_at":"2026-07-05T08:58:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2406.03457","created_at":"2026-07-05T08:58:44Z"},{"alias_kind":"pith_short_12","alias_value":"DAXH33UKZEFJ","created_at":"2026-07-05T08:58:44Z"},{"alias_kind":"pith_short_16","alias_value":"DAXH33UKZEFJ6AQV","created_at":"2026-07-05T08:58:44Z"},{"alias_kind":"pith_short_8","alias_value":"DAXH33UK","created_at":"2026-07-05T08:58:44Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:DAXH33UKZEFJ6AQV6GX6PQQZMT","target":"record","payload":{"canonical_record":{"source":{"id":"2406.03457","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2024-06-05T17:01:55Z","cross_cats_sorted":[],"title_canon_sha256":"8b189fc6395ec71901b8601e36cdbafaa713e7fdf226429f3a7fac255b023e2f","abstract_canon_sha256":"b32a8d5522575e04610a1ec932734b6650ab0e9bacf6d404bbdbdfe1abb81807"},"schema_version":"1.0"},"canonical_sha256":"182e7dee8ac90a9f0215f1afe7c21964cc570e5c3fe08b0b6f2d89bf5f1f2367","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:58:44.955239Z","signature_b64":"71OY37lGR8EtJji7FEzeA+M0N0WLfQKg6fNAF4077LVUBofpPErBjxaDr/RcAp4incdZTX1JYh9oz6LZF8HzBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"182e7dee8ac90a9f0215f1afe7c21964cc570e5c3fe08b0b6f2d89bf5f1f2367","last_reissued_at":"2026-07-05T08:58:44.954751Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:58:44.954751Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2406.03457","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T08:58:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/Pd+w8eCe5lQcUbWgVr+SOCLqe6lvM5aW0+JPubVJGKmbVNpuV9q8UDaWip817tx/Qpr6c9VNaIwBOZaPpPnCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-17T23:11:23.257704Z"},"content_sha256":"9ad58b09c0292e533405a040129f563ffd15e45db6f75649bd083234b84e9c69","schema_version":"1.0","event_id":"sha256:9ad58b09c0292e533405a040129f563ffd15e45db6f75649bd083234b84e9c69"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:DAXH33UKZEFJ6AQV6GX6PQQZMT","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Gravitational radiation from inspiralling compact binaries to N$^3$LO in the Effective Field Theory approach","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Loris Amalberti, Rafael A. Porto, Zixin Yang","submitted_at":"2024-06-05T17:01:55Z","abstract_excerpt":"Within the context of the Effective Field Theory (EFT) framework to gravitational dynamics, we compute the Hamiltonian, source quadrupole moment, and gravitational-wave energy flux for (non-spinning) inspiralling compact binaries at next-to-next-to-next-to leading order (N$^3$LO) in the Post-Newtonian (PN) expansion. We use the recently developed $d$-dimensional multipole-expanded effective theory, and explicitly perform the matching to the (pseudo-) stress-energy tensor. The calculation involves Feynman integrals up to three- (conservative) and two-loop (radiative) orders, evaluated within di"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2406.03457","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/2406.03457/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":"2026-07-05T08:58:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yJPXKRv57LkezHM/OxqR3GI6yXl6ge4hrIT2xFHzYpLZ/Q2UgijLY/UlT2PNjjPVosTW/ewMSJGrEGCA/Gd2Aw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-17T23:11:23.258197Z"},"content_sha256":"8021e53d1f956e5f3c8f4b6cd8c64753cf31aea7e537e7387274605249d7d2b2","schema_version":"1.0","event_id":"sha256:8021e53d1f956e5f3c8f4b6cd8c64753cf31aea7e537e7387274605249d7d2b2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DAXH33UKZEFJ6AQV6GX6PQQZMT/bundle.json","state_url":"https://pith.science/pith/DAXH33UKZEFJ6AQV6GX6PQQZMT/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DAXH33UKZEFJ6AQV6GX6PQQZMT/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":"2026-08-17T23:11:23Z","links":{"resolver":"https://pith.science/pith/DAXH33UKZEFJ6AQV6GX6PQQZMT","bundle":"https://pith.science/pith/DAXH33UKZEFJ6AQV6GX6PQQZMT/bundle.json","state":"https://pith.science/pith/DAXH33UKZEFJ6AQV6GX6PQQZMT/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DAXH33UKZEFJ6AQV6GX6PQQZMT/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:DAXH33UKZEFJ6AQV6GX6PQQZMT","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":"b32a8d5522575e04610a1ec932734b6650ab0e9bacf6d404bbdbdfe1abb81807","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2024-06-05T17:01:55Z","title_canon_sha256":"8b189fc6395ec71901b8601e36cdbafaa713e7fdf226429f3a7fac255b023e2f"},"schema_version":"1.0","source":{"id":"2406.03457","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2406.03457","created_at":"2026-07-05T08:58:44Z"},{"alias_kind":"arxiv_version","alias_value":"2406.03457v2","created_at":"2026-07-05T08:58:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2406.03457","created_at":"2026-07-05T08:58:44Z"},{"alias_kind":"pith_short_12","alias_value":"DAXH33UKZEFJ","created_at":"2026-07-05T08:58:44Z"},{"alias_kind":"pith_short_16","alias_value":"DAXH33UKZEFJ6AQV","created_at":"2026-07-05T08:58:44Z"},{"alias_kind":"pith_short_8","alias_value":"DAXH33UK","created_at":"2026-07-05T08:58:44Z"}],"graph_snapshots":[{"event_id":"sha256:8021e53d1f956e5f3c8f4b6cd8c64753cf31aea7e537e7387274605249d7d2b2","target":"graph","created_at":"2026-07-05T08:58:44Z","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/2406.03457/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Within the context of the Effective Field Theory (EFT) framework to gravitational dynamics, we compute the Hamiltonian, source quadrupole moment, and gravitational-wave energy flux for (non-spinning) inspiralling compact binaries at next-to-next-to-next-to leading order (N$^3$LO) in the Post-Newtonian (PN) expansion. We use the recently developed $d$-dimensional multipole-expanded effective theory, and explicitly perform the matching to the (pseudo-) stress-energy tensor. The calculation involves Feynman integrals up to three- (conservative) and two-loop (radiative) orders, evaluated within di","authors_text":"Loris Amalberti, Rafael A. Porto, Zixin Yang","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2024-06-05T17:01:55Z","title":"Gravitational radiation from inspiralling compact binaries to N$^3$LO in the Effective Field Theory approach"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2406.03457","kind":"arxiv","version":2},"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":"sha256:9ad58b09c0292e533405a040129f563ffd15e45db6f75649bd083234b84e9c69","target":"record","created_at":"2026-07-05T08:58:44Z","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":"b32a8d5522575e04610a1ec932734b6650ab0e9bacf6d404bbdbdfe1abb81807","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2024-06-05T17:01:55Z","title_canon_sha256":"8b189fc6395ec71901b8601e36cdbafaa713e7fdf226429f3a7fac255b023e2f"},"schema_version":"1.0","source":{"id":"2406.03457","kind":"arxiv","version":2}},"canonical_sha256":"182e7dee8ac90a9f0215f1afe7c21964cc570e5c3fe08b0b6f2d89bf5f1f2367","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"182e7dee8ac90a9f0215f1afe7c21964cc570e5c3fe08b0b6f2d89bf5f1f2367","first_computed_at":"2026-07-05T08:58:44.954751Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:58:44.954751Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"71OY37lGR8EtJji7FEzeA+M0N0WLfQKg6fNAF4077LVUBofpPErBjxaDr/RcAp4incdZTX1JYh9oz6LZF8HzBg==","signature_status":"signed_v1","signed_at":"2026-07-05T08:58:44.955239Z","signed_message":"canonical_sha256_bytes"},"source_id":"2406.03457","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9ad58b09c0292e533405a040129f563ffd15e45db6f75649bd083234b84e9c69","sha256:8021e53d1f956e5f3c8f4b6cd8c64753cf31aea7e537e7387274605249d7d2b2"],"state_sha256":"85b1bbbc85486631a0a7f0a8754c5cc4f9b89d0c3bbf74f5d7d140d48d0d0191"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YwPUvA9isZBt8v8SyVFvsRdD/1M0eSqWqM7tLhTHIABSi8i9XAhDyKWAUsby1Vn73BO/h7jX4rurUF3T7lpnBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-17T23:11:23.262070Z","bundle_sha256":"70dfa427bcb9914ed5666eff8b4f89af343d7ac813de2a1f8672a04dfd51965a"}}