{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:KVXK6FKCYBYLMD5J7Q4WPF5WMY","short_pith_number":"pith:KVXK6FKC","canonical_record":{"source":{"id":"1802.10201","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2018-02-27T22:56:43Z","cross_cats_sorted":[],"title_canon_sha256":"e5af36ca123eac8613b8affefa12151a649b878cca9206b538780731cf32477d","abstract_canon_sha256":"63096d2af8909e3a519b609991c581525a26683596309cc6ff4113da1870028c"},"schema_version":"1.0"},"canonical_sha256":"556eaf1542c070b60fa9fc396797b66614963890a93be8db7649812478062ab0","source":{"kind":"arxiv","id":"1802.10201","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1802.10201","created_at":"2026-07-05T05:47:00Z"},{"alias_kind":"arxiv_version","alias_value":"1802.10201v4","created_at":"2026-07-05T05:47:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1802.10201","created_at":"2026-07-05T05:47:00Z"},{"alias_kind":"pith_short_12","alias_value":"KVXK6FKCYBYL","created_at":"2026-07-05T05:47:00Z"},{"alias_kind":"pith_short_16","alias_value":"KVXK6FKCYBYLMD5J","created_at":"2026-07-05T05:47:00Z"},{"alias_kind":"pith_short_8","alias_value":"KVXK6FKC","created_at":"2026-07-05T05:47:00Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:KVXK6FKCYBYLMD5J7Q4WPF5WMY","target":"record","payload":{"canonical_record":{"source":{"id":"1802.10201","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2018-02-27T22:56:43Z","cross_cats_sorted":[],"title_canon_sha256":"e5af36ca123eac8613b8affefa12151a649b878cca9206b538780731cf32477d","abstract_canon_sha256":"63096d2af8909e3a519b609991c581525a26683596309cc6ff4113da1870028c"},"schema_version":"1.0"},"canonical_sha256":"556eaf1542c070b60fa9fc396797b66614963890a93be8db7649812478062ab0","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:47:00.421421Z","signature_b64":"0PUDgJj5TlQ1xAj/oFvxC/+NEXOLhfkHHWJAzUP8qSkmR69Q3AuEPXwrKUlm3/vFrCRFrmp31rYUbrSLs/AVBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"556eaf1542c070b60fa9fc396797b66614963890a93be8db7649812478062ab0","last_reissued_at":"2026-07-05T05:47:00.420933Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:47:00.420933Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1802.10201","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":"2026-07-05T05:47:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kkf3yJouK7m/NvDhS4Gy8YgAEphyLLOE/mBT/CWBchqOocJkbU1ecPFb+gAc3Wlp1pBbFPnrgJsAZYag03dLAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-09T12:15:14.090998Z"},"content_sha256":"35679a94ae5951b6ae5513b9d163053b86064e6f5c3e0f9044a74cee05135517","schema_version":"1.0","event_id":"sha256:35679a94ae5951b6ae5513b9d163053b86064e6f5c3e0f9044a74cee05135517"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:KVXK6FKCYBYLMD5J7Q4WPF5WMY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dynamics of compact binary systems in scalar-tensor theories: I. Equations of motion to the third post-Newtonian order","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Laura Bernard","submitted_at":"2018-02-27T22:56:43Z","abstract_excerpt":"Scalar-tensor theories are one of the most natural and well-constrained alternative theories of gravity, while still allowing for significant deviations from general relativity. We present the equations of motion of nonspinning compact binary systems at the third post-Newtonian (PN) order in massless scalar-tensor theories. We adapt the Fokker action of point particles in harmonic coordinates in general relativity to the specificities of scalar-tensor theories. We use dimensional regularisation to treat both the infrared and ultraviolet divergences, and we consistently include the tail effects"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1802.10201","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/1802.10201/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":"2026-07-05T05:47:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZeQJSryTVfLuKFwP2d4AJuyH38xEvofosD/VA4+mCHy5QnZFGekta861963XfGS6SIYnUYQOjWWkb9QXVLe7Aw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-09T12:15:14.091498Z"},"content_sha256":"e1e7c8104947fe45f531018652a3350cd563b25290e70717ab004718f7168487","schema_version":"1.0","event_id":"sha256:e1e7c8104947fe45f531018652a3350cd563b25290e70717ab004718f7168487"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KVXK6FKCYBYLMD5J7Q4WPF5WMY/bundle.json","state_url":"https://pith.science/pith/KVXK6FKCYBYLMD5J7Q4WPF5WMY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KVXK6FKCYBYLMD5J7Q4WPF5WMY/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":"2026-08-09T12:15:14Z","links":{"resolver":"https://pith.science/pith/KVXK6FKCYBYLMD5J7Q4WPF5WMY","bundle":"https://pith.science/pith/KVXK6FKCYBYLMD5J7Q4WPF5WMY/bundle.json","state":"https://pith.science/pith/KVXK6FKCYBYLMD5J7Q4WPF5WMY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KVXK6FKCYBYLMD5J7Q4WPF5WMY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:KVXK6FKCYBYLMD5J7Q4WPF5WMY","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":"63096d2af8909e3a519b609991c581525a26683596309cc6ff4113da1870028c","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2018-02-27T22:56:43Z","title_canon_sha256":"e5af36ca123eac8613b8affefa12151a649b878cca9206b538780731cf32477d"},"schema_version":"1.0","source":{"id":"1802.10201","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1802.10201","created_at":"2026-07-05T05:47:00Z"},{"alias_kind":"arxiv_version","alias_value":"1802.10201v4","created_at":"2026-07-05T05:47:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1802.10201","created_at":"2026-07-05T05:47:00Z"},{"alias_kind":"pith_short_12","alias_value":"KVXK6FKCYBYL","created_at":"2026-07-05T05:47:00Z"},{"alias_kind":"pith_short_16","alias_value":"KVXK6FKCYBYLMD5J","created_at":"2026-07-05T05:47:00Z"},{"alias_kind":"pith_short_8","alias_value":"KVXK6FKC","created_at":"2026-07-05T05:47:00Z"}],"graph_snapshots":[{"event_id":"sha256:e1e7c8104947fe45f531018652a3350cd563b25290e70717ab004718f7168487","target":"graph","created_at":"2026-07-05T05:47:00Z","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/1802.10201/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Scalar-tensor theories are one of the most natural and well-constrained alternative theories of gravity, while still allowing for significant deviations from general relativity. We present the equations of motion of nonspinning compact binary systems at the third post-Newtonian (PN) order in massless scalar-tensor theories. We adapt the Fokker action of point particles in harmonic coordinates in general relativity to the specificities of scalar-tensor theories. We use dimensional regularisation to treat both the infrared and ultraviolet divergences, and we consistently include the tail effects","authors_text":"Laura Bernard","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2018-02-27T22:56:43Z","title":"Dynamics of compact binary systems in scalar-tensor theories: I. Equations of motion to the third post-Newtonian order"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1802.10201","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":"sha256:35679a94ae5951b6ae5513b9d163053b86064e6f5c3e0f9044a74cee05135517","target":"record","created_at":"2026-07-05T05:47:00Z","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":"63096d2af8909e3a519b609991c581525a26683596309cc6ff4113da1870028c","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2018-02-27T22:56:43Z","title_canon_sha256":"e5af36ca123eac8613b8affefa12151a649b878cca9206b538780731cf32477d"},"schema_version":"1.0","source":{"id":"1802.10201","kind":"arxiv","version":4}},"canonical_sha256":"556eaf1542c070b60fa9fc396797b66614963890a93be8db7649812478062ab0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"556eaf1542c070b60fa9fc396797b66614963890a93be8db7649812478062ab0","first_computed_at":"2026-07-05T05:47:00.420933Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:47:00.420933Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"0PUDgJj5TlQ1xAj/oFvxC/+NEXOLhfkHHWJAzUP8qSkmR69Q3AuEPXwrKUlm3/vFrCRFrmp31rYUbrSLs/AVBA==","signature_status":"signed_v1","signed_at":"2026-07-05T05:47:00.421421Z","signed_message":"canonical_sha256_bytes"},"source_id":"1802.10201","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:35679a94ae5951b6ae5513b9d163053b86064e6f5c3e0f9044a74cee05135517","sha256:e1e7c8104947fe45f531018652a3350cd563b25290e70717ab004718f7168487"],"state_sha256":"30bd0125d8ec65fd7ee4384de27733863f8101eab2c87e81e4f042c48914870f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"syzRm6bkD9rH4vbmT2v/mSbaGG5euVeMqDHBKWkqtQ5olFl66daO9tggMtgMzeGdk46bQxe1bFYgQ4JB6CmSCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-09T12:15:14.095672Z","bundle_sha256":"9f610caa2cc5d1b79174731e2482a5789dd996e430b642e0cb70d5bbb84a95af"}}