{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:BEFFPL674UHRXISGCNPQDCN7GK","short_pith_number":"pith:BEFFPL67","canonical_record":{"source":{"id":"2510.06948","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2025-10-08T12:30:56Z","cross_cats_sorted":["astro-ph.GA"],"title_canon_sha256":"3c55e14a1d519c48d0bea6320ce60f35d10cbc194f8fe7eaf2a7c71e29c5d902","abstract_canon_sha256":"d8d8630b340664ffcacb4f0ea56932be1c16d5718304d294a7d6166b63c57f83"},"schema_version":"1.0"},"canonical_sha256":"090a57afdfe50f1ba246135f0189bf328a19a68b40a4aeea4bf913a33a072135","source":{"kind":"arxiv","id":"2510.06948","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2510.06948","created_at":"2026-07-14T01:20:46Z"},{"alias_kind":"arxiv_version","alias_value":"2510.06948v2","created_at":"2026-07-14T01:20:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2510.06948","created_at":"2026-07-14T01:20:46Z"},{"alias_kind":"pith_short_12","alias_value":"BEFFPL674UHR","created_at":"2026-07-14T01:20:46Z"},{"alias_kind":"pith_short_16","alias_value":"BEFFPL674UHRXISG","created_at":"2026-07-14T01:20:46Z"},{"alias_kind":"pith_short_8","alias_value":"BEFFPL67","created_at":"2026-07-14T01:20:46Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:BEFFPL674UHRXISGCNPQDCN7GK","target":"record","payload":{"canonical_record":{"source":{"id":"2510.06948","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2025-10-08T12:30:56Z","cross_cats_sorted":["astro-ph.GA"],"title_canon_sha256":"3c55e14a1d519c48d0bea6320ce60f35d10cbc194f8fe7eaf2a7c71e29c5d902","abstract_canon_sha256":"d8d8630b340664ffcacb4f0ea56932be1c16d5718304d294a7d6166b63c57f83"},"schema_version":"1.0"},"canonical_sha256":"090a57afdfe50f1ba246135f0189bf328a19a68b40a4aeea4bf913a33a072135","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-14T01:20:46.682879Z","signature_b64":"ATf6FtQCJsjx/LmnUXS8ls4a47d4oZMfY/5fZL+0qo4lQbszV+NB3uktbsORF8ysdfojhVVXtUXOau+LuwSMCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"090a57afdfe50f1ba246135f0189bf328a19a68b40a4aeea4bf913a33a072135","last_reissued_at":"2026-07-14T01:20:46.681909Z","signature_status":"signed_v1","first_computed_at":"2026-07-14T01:20:46.681909Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2510.06948","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":"2026-07-14T01:20:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"epbpauI6QOL9FkIIHz3qUiYqAEsURpQ01xLMZxJQtd2CHA9fzub6O0cD0pKVp+5t4JNW5uQuy8Y0dYkCFrlBCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T20:58:49.624904Z"},"content_sha256":"23b608fbb34a3a35167389e1196b73247a17075da0850e78d452de58a82c26b2","schema_version":"1.0","event_id":"sha256:23b608fbb34a3a35167389e1196b73247a17075da0850e78d452de58a82c26b2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:BEFFPL674UHRXISGCNPQDCN7GK","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"When vacuum breaks: a self-consistency test for astrophysical environments in extreme mass ratio inspirals","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["astro-ph.GA"],"primary_cat":"gr-qc","authors_text":"Enrico Barausse, Lorenzo Copparoni, Rohit S. Chandramouli","submitted_at":"2025-10-08T12:30:56Z","abstract_excerpt":"Gravitational-wave signals are typically interpreted under the vacuum hypothesis, i.e. assuming negligible influence from the astrophysical environment. This assumption is expected to break down for low-frequency sources such as extreme mass ratio inspirals (EMRIs), which are prime targets for the Laser Interferometer Space Antenna (LISA) and are expected to form, at least in part, in dense environments such as Active Galactic Nuclei or dark-matter spikes and cores. Modeling environmental effects parametrically is challenging due to the large uncertainties in their underlying physics. We propo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2510.06948","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/2510.06948/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":"2026-07-14T01:20:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xW7Eldrgch3+PyR2HgH3WJcYJqiTuJrkRxmKnCudrH4xr+YEUW1JT8WE9IJLxhF8vwgAG0yDqUQ4CcMy/TCiAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T20:58:49.625832Z"},"content_sha256":"f8ed6d26cb1b5dc52dd709e2cfd35c012b2b6424d1901c39c4bc2af301b061cd","schema_version":"1.0","event_id":"sha256:f8ed6d26cb1b5dc52dd709e2cfd35c012b2b6424d1901c39c4bc2af301b061cd"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/BEFFPL674UHRXISGCNPQDCN7GK/bundle.json","state_url":"https://pith.science/pith/BEFFPL674UHRXISGCNPQDCN7GK/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/BEFFPL674UHRXISGCNPQDCN7GK/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":"2026-08-04T20:58:49Z","links":{"resolver":"https://pith.science/pith/BEFFPL674UHRXISGCNPQDCN7GK","bundle":"https://pith.science/pith/BEFFPL674UHRXISGCNPQDCN7GK/bundle.json","state":"https://pith.science/pith/BEFFPL674UHRXISGCNPQDCN7GK/state.json","well_known_bundle":"https://pith.science/.well-known/pith/BEFFPL674UHRXISGCNPQDCN7GK/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:BEFFPL674UHRXISGCNPQDCN7GK","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":"d8d8630b340664ffcacb4f0ea56932be1c16d5718304d294a7d6166b63c57f83","cross_cats_sorted":["astro-ph.GA"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2025-10-08T12:30:56Z","title_canon_sha256":"3c55e14a1d519c48d0bea6320ce60f35d10cbc194f8fe7eaf2a7c71e29c5d902"},"schema_version":"1.0","source":{"id":"2510.06948","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2510.06948","created_at":"2026-07-14T01:20:46Z"},{"alias_kind":"arxiv_version","alias_value":"2510.06948v2","created_at":"2026-07-14T01:20:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2510.06948","created_at":"2026-07-14T01:20:46Z"},{"alias_kind":"pith_short_12","alias_value":"BEFFPL674UHR","created_at":"2026-07-14T01:20:46Z"},{"alias_kind":"pith_short_16","alias_value":"BEFFPL674UHRXISG","created_at":"2026-07-14T01:20:46Z"},{"alias_kind":"pith_short_8","alias_value":"BEFFPL67","created_at":"2026-07-14T01:20:46Z"}],"graph_snapshots":[{"event_id":"sha256:f8ed6d26cb1b5dc52dd709e2cfd35c012b2b6424d1901c39c4bc2af301b061cd","target":"graph","created_at":"2026-07-14T01:20:46Z","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/2510.06948/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Gravitational-wave signals are typically interpreted under the vacuum hypothesis, i.e. assuming negligible influence from the astrophysical environment. This assumption is expected to break down for low-frequency sources such as extreme mass ratio inspirals (EMRIs), which are prime targets for the Laser Interferometer Space Antenna (LISA) and are expected to form, at least in part, in dense environments such as Active Galactic Nuclei or dark-matter spikes and cores. Modeling environmental effects parametrically is challenging due to the large uncertainties in their underlying physics. We propo","authors_text":"Enrico Barausse, Lorenzo Copparoni, Rohit S. Chandramouli","cross_cats":["astro-ph.GA"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2025-10-08T12:30:56Z","title":"When vacuum breaks: a self-consistency test for astrophysical environments in extreme mass ratio inspirals"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2510.06948","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":"sha256:23b608fbb34a3a35167389e1196b73247a17075da0850e78d452de58a82c26b2","target":"record","created_at":"2026-07-14T01:20:46Z","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":"d8d8630b340664ffcacb4f0ea56932be1c16d5718304d294a7d6166b63c57f83","cross_cats_sorted":["astro-ph.GA"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2025-10-08T12:30:56Z","title_canon_sha256":"3c55e14a1d519c48d0bea6320ce60f35d10cbc194f8fe7eaf2a7c71e29c5d902"},"schema_version":"1.0","source":{"id":"2510.06948","kind":"arxiv","version":2}},"canonical_sha256":"090a57afdfe50f1ba246135f0189bf328a19a68b40a4aeea4bf913a33a072135","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"090a57afdfe50f1ba246135f0189bf328a19a68b40a4aeea4bf913a33a072135","first_computed_at":"2026-07-14T01:20:46.681909Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-14T01:20:46.681909Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ATf6FtQCJsjx/LmnUXS8ls4a47d4oZMfY/5fZL+0qo4lQbszV+NB3uktbsORF8ysdfojhVVXtUXOau+LuwSMCA==","signature_status":"signed_v1","signed_at":"2026-07-14T01:20:46.682879Z","signed_message":"canonical_sha256_bytes"},"source_id":"2510.06948","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:23b608fbb34a3a35167389e1196b73247a17075da0850e78d452de58a82c26b2","sha256:f8ed6d26cb1b5dc52dd709e2cfd35c012b2b6424d1901c39c4bc2af301b061cd"],"state_sha256":"20131a7b41ab88a76c310944db2d67f2b97612d9ee925ef1a0ce29bd484cff37"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VZBNjotWmxLumNO1XASJbrUDvX7VfKlr3kWoJlV6chBxTvx9m7lhhpiWZe6xl0z5In7rIUQ8YGZldwggJ9pLAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T20:58:49.632649Z","bundle_sha256":"c2c491fcf5b68fc199175d64419a87338d75adfc7e275ca5599c825c7f67c74a"}}