{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:P35TB6VYACWE5DGRFCZ3EQYOBG","short_pith_number":"pith:P35TB6VY","canonical_record":{"source":{"id":"1709.09742","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-09-27T21:43:48Z","cross_cats_sorted":[],"title_canon_sha256":"0765df6e7f1358d46b078b56bc664662d5f0358cc070475d1764a0ec7daa82ed","abstract_canon_sha256":"21ace6f771d6ae21eb4f66b4daf0b46508ae918ea9259622e5fd5eeaba70222f"},"schema_version":"1.0"},"canonical_sha256":"7efb30fab800ac4e8cd128b3b2430e098730d8255d8fbec8614595a3b4d976d6","source":{"kind":"arxiv","id":"1709.09742","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1709.09742","created_at":"2026-05-18T00:24:16Z"},{"alias_kind":"arxiv_version","alias_value":"1709.09742v1","created_at":"2026-05-18T00:24:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.09742","created_at":"2026-05-18T00:24:16Z"},{"alias_kind":"pith_short_12","alias_value":"P35TB6VYACWE","created_at":"2026-05-18T12:31:37Z"},{"alias_kind":"pith_short_16","alias_value":"P35TB6VYACWE5DGR","created_at":"2026-05-18T12:31:37Z"},{"alias_kind":"pith_short_8","alias_value":"P35TB6VY","created_at":"2026-05-18T12:31:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:P35TB6VYACWE5DGRFCZ3EQYOBG","target":"record","payload":{"canonical_record":{"source":{"id":"1709.09742","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-09-27T21:43:48Z","cross_cats_sorted":[],"title_canon_sha256":"0765df6e7f1358d46b078b56bc664662d5f0358cc070475d1764a0ec7daa82ed","abstract_canon_sha256":"21ace6f771d6ae21eb4f66b4daf0b46508ae918ea9259622e5fd5eeaba70222f"},"schema_version":"1.0"},"canonical_sha256":"7efb30fab800ac4e8cd128b3b2430e098730d8255d8fbec8614595a3b4d976d6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:24:16.185138Z","signature_b64":"PUrwxSm2qJj8Zn/yh8fKv0jqpOzSaW0GWMeBeCivsLJEafWCdgbGeMQRiVdKC2tR3iVweT1n70zzm3bGU87cCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7efb30fab800ac4e8cd128b3b2430e098730d8255d8fbec8614595a3b4d976d6","last_reissued_at":"2026-05-18T00:24:16.184631Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:24:16.184631Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1709.09742","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":"2026-05-18T00:24:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DnZRdqUEpBcbfJyWuZ3lCiGHqmf73nCUvTjJZP2T1bN6Udd33BF7623LGJ9b1tZzjaGr0BuJjNtfnnY1ImPoDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T18:30:33.945235Z"},"content_sha256":"2a6777106adf7740232a3a467bcf80c8533b2ff333db30a8d79a46b1bab0c23a","schema_version":"1.0","event_id":"sha256:2a6777106adf7740232a3a467bcf80c8533b2ff333db30a8d79a46b1bab0c23a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:P35TB6VYACWE5DGRFCZ3EQYOBG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Reducing the two-body problem in scalar-tensor theories to the motion of a test particle : a scalar-tensor effective-one-body approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"F\\'elix-Louis Juli\\'e","submitted_at":"2017-09-27T21:43:48Z","abstract_excerpt":"Starting from the second post-Keplerian (2PK) Hamiltonian describing the conservative part of the two-body dynamics in massless scalar-tensor (ST) theories, we build an effective-one-body (EOB) Hamiltonian which is a $\\nu$-deformation (where $\\nu= 0$ is the test mass limit) of the analytically known ST Hamiltonian of a test particle. This ST-EOB Hamiltonian leads to a simple (yet canonically equivalent) formulation of the conservative 2PK two-body problem, but also defines a resummation of the dynamics which is well-suited to ST regimes that depart strongly from general relativity (GR) and whi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.09742","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":"2026-05-18T00:24:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YG7gdFAvQeG3FOuc6XGDx1Riy1A01sARIzmv28w5JBH+2vghbAKhC94+DK3wxZanGYX7ew+XneCJTGNGSUpmAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T18:30:33.945585Z"},"content_sha256":"20052906e065e3c23e1a1731dbf1bd2bae9db0ddcf81890d02176e4f1e698952","schema_version":"1.0","event_id":"sha256:20052906e065e3c23e1a1731dbf1bd2bae9db0ddcf81890d02176e4f1e698952"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/P35TB6VYACWE5DGRFCZ3EQYOBG/bundle.json","state_url":"https://pith.science/pith/P35TB6VYACWE5DGRFCZ3EQYOBG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/P35TB6VYACWE5DGRFCZ3EQYOBG/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":"2026-08-03T18:30:33Z","links":{"resolver":"https://pith.science/pith/P35TB6VYACWE5DGRFCZ3EQYOBG","bundle":"https://pith.science/pith/P35TB6VYACWE5DGRFCZ3EQYOBG/bundle.json","state":"https://pith.science/pith/P35TB6VYACWE5DGRFCZ3EQYOBG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/P35TB6VYACWE5DGRFCZ3EQYOBG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:P35TB6VYACWE5DGRFCZ3EQYOBG","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":"21ace6f771d6ae21eb4f66b4daf0b46508ae918ea9259622e5fd5eeaba70222f","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-09-27T21:43:48Z","title_canon_sha256":"0765df6e7f1358d46b078b56bc664662d5f0358cc070475d1764a0ec7daa82ed"},"schema_version":"1.0","source":{"id":"1709.09742","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1709.09742","created_at":"2026-05-18T00:24:16Z"},{"alias_kind":"arxiv_version","alias_value":"1709.09742v1","created_at":"2026-05-18T00:24:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.09742","created_at":"2026-05-18T00:24:16Z"},{"alias_kind":"pith_short_12","alias_value":"P35TB6VYACWE","created_at":"2026-05-18T12:31:37Z"},{"alias_kind":"pith_short_16","alias_value":"P35TB6VYACWE5DGR","created_at":"2026-05-18T12:31:37Z"},{"alias_kind":"pith_short_8","alias_value":"P35TB6VY","created_at":"2026-05-18T12:31:37Z"}],"graph_snapshots":[{"event_id":"sha256:20052906e065e3c23e1a1731dbf1bd2bae9db0ddcf81890d02176e4f1e698952","target":"graph","created_at":"2026-05-18T00:24:16Z","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":"Starting from the second post-Keplerian (2PK) Hamiltonian describing the conservative part of the two-body dynamics in massless scalar-tensor (ST) theories, we build an effective-one-body (EOB) Hamiltonian which is a $\\nu$-deformation (where $\\nu= 0$ is the test mass limit) of the analytically known ST Hamiltonian of a test particle. This ST-EOB Hamiltonian leads to a simple (yet canonically equivalent) formulation of the conservative 2PK two-body problem, but also defines a resummation of the dynamics which is well-suited to ST regimes that depart strongly from general relativity (GR) and whi","authors_text":"F\\'elix-Louis Juli\\'e","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-09-27T21:43:48Z","title":"Reducing the two-body problem in scalar-tensor theories to the motion of a test particle : a scalar-tensor effective-one-body approach"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.09742","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":"sha256:2a6777106adf7740232a3a467bcf80c8533b2ff333db30a8d79a46b1bab0c23a","target":"record","created_at":"2026-05-18T00:24:16Z","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":"21ace6f771d6ae21eb4f66b4daf0b46508ae918ea9259622e5fd5eeaba70222f","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-09-27T21:43:48Z","title_canon_sha256":"0765df6e7f1358d46b078b56bc664662d5f0358cc070475d1764a0ec7daa82ed"},"schema_version":"1.0","source":{"id":"1709.09742","kind":"arxiv","version":1}},"canonical_sha256":"7efb30fab800ac4e8cd128b3b2430e098730d8255d8fbec8614595a3b4d976d6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7efb30fab800ac4e8cd128b3b2430e098730d8255d8fbec8614595a3b4d976d6","first_computed_at":"2026-05-18T00:24:16.184631Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:24:16.184631Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"PUrwxSm2qJj8Zn/yh8fKv0jqpOzSaW0GWMeBeCivsLJEafWCdgbGeMQRiVdKC2tR3iVweT1n70zzm3bGU87cCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:24:16.185138Z","signed_message":"canonical_sha256_bytes"},"source_id":"1709.09742","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2a6777106adf7740232a3a467bcf80c8533b2ff333db30a8d79a46b1bab0c23a","sha256:20052906e065e3c23e1a1731dbf1bd2bae9db0ddcf81890d02176e4f1e698952"],"state_sha256":"b929469043c31fc66aaa2a971f89953cef91613a4f0694450810de966f495f08"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IiaciooiHqBPG8W67sDjO+DcvSfGmEz+3YBWujN7siV0LEfBAl/ZCSSPgsdWRPGjuGA4ZDBICAtoCiLMdASXBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-03T18:30:33.948235Z","bundle_sha256":"507852292a596bf437ecb7ac8c7ac0b30d7ea9b224ae269d1dd31c03795c322a"}}