{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:UDUMWARF6WPGMG2SVI3UD4WMZI","short_pith_number":"pith:UDUMWARF","canonical_record":{"source":{"id":"2409.03914","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-09-05T21:23:44Z","cross_cats_sorted":[],"title_canon_sha256":"d0f992630187f3d6ed1f966593755eb4e6c67a75bac660715779ee1b33a6125f","abstract_canon_sha256":"1b263a5355ebf1ae95485faca04089e025a033b3fd61388eb07daa3b974d1909"},"schema_version":"1.0"},"canonical_sha256":"a0e8cb0225f59e661b52aa3741f2ccca3d05b9229f6552f289a8b72455aa0146","source":{"kind":"arxiv","id":"2409.03914","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2409.03914","created_at":"2026-07-05T11:50:58Z"},{"alias_kind":"arxiv_version","alias_value":"2409.03914v3","created_at":"2026-07-05T11:50:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2409.03914","created_at":"2026-07-05T11:50:58Z"},{"alias_kind":"pith_short_12","alias_value":"UDUMWARF6WPG","created_at":"2026-07-05T11:50:58Z"},{"alias_kind":"pith_short_16","alias_value":"UDUMWARF6WPGMG2S","created_at":"2026-07-05T11:50:58Z"},{"alias_kind":"pith_short_8","alias_value":"UDUMWARF","created_at":"2026-07-05T11:50:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:UDUMWARF6WPGMG2SVI3UD4WMZI","target":"record","payload":{"canonical_record":{"source":{"id":"2409.03914","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-09-05T21:23:44Z","cross_cats_sorted":[],"title_canon_sha256":"d0f992630187f3d6ed1f966593755eb4e6c67a75bac660715779ee1b33a6125f","abstract_canon_sha256":"1b263a5355ebf1ae95485faca04089e025a033b3fd61388eb07daa3b974d1909"},"schema_version":"1.0"},"canonical_sha256":"a0e8cb0225f59e661b52aa3741f2ccca3d05b9229f6552f289a8b72455aa0146","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:50:58.251566Z","signature_b64":"h9XXQ4AeRVyOn38cRyddy+IJ+51/nAbu7liZ6BlmFna/QhrZwPDa8E1v759bRF1D7Iy+Ol6zJoR7JKkaXfAHDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a0e8cb0225f59e661b52aa3741f2ccca3d05b9229f6552f289a8b72455aa0146","last_reissued_at":"2026-07-05T11:50:58.251076Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:50:58.251076Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2409.03914","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T11:50:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fTVCOMHudBclyF7HnjTZURYmlC8CbD0IUe3tqu2d6LW7nOI0SKB8L+0ib+sHDKz2BqnrFZgG30txKFQ0FArcAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-07T15:42:12.952248Z"},"content_sha256":"505abb6bb5b5a844ad423aee84cbd24c4e6a151a653f0f1b7d422f020fdb8d93","schema_version":"1.0","event_id":"sha256:505abb6bb5b5a844ad423aee84cbd24c4e6a151a653f0f1b7d422f020fdb8d93"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:UDUMWARF6WPGMG2SVI3UD4WMZI","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Cosmology with non-conformal holographic matter","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Mark Van Raamsdonk, Rana Zibakhsh","submitted_at":"2024-09-05T21:23:44Z","abstract_excerpt":"We investigate the effect on cosmological evolution of a strongly coupled quantum field that undergoes renormalization group flow from a UV CFT to an IR CFT. The field theory is defined by perturbation of a holographic CFT by a relevant operator associated with a bulk scalar field that evolves from a local maximum of its potential near the boundary to a local minimum of its potential deep in the bulk. By studying the gravity solutions dual to this theory on $\\mathbb{R}^3 \\times S^1$, we find that the equation of state parameter $w$ for the field theory has the conformal behavior $w=1/3$ for hi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2409.03914","kind":"arxiv","version":3},"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/2409.03914/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":"2026-07-05T11:50:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JqR2Pk0Fd0pMDOYGIJGf4ruoAIrxCk49iWN6JN8Hs3y8X3Pn6kBOTvjRgFUuO4MVsHg+u/rAFwPHHFbae777Bw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-07T15:42:12.952626Z"},"content_sha256":"b64cc7053a5b92645d51ff9834b7506971b275fd41a009b0be5eab327d3db845","schema_version":"1.0","event_id":"sha256:b64cc7053a5b92645d51ff9834b7506971b275fd41a009b0be5eab327d3db845"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UDUMWARF6WPGMG2SVI3UD4WMZI/bundle.json","state_url":"https://pith.science/pith/UDUMWARF6WPGMG2SVI3UD4WMZI/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UDUMWARF6WPGMG2SVI3UD4WMZI/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":"2026-08-07T15:42:12Z","links":{"resolver":"https://pith.science/pith/UDUMWARF6WPGMG2SVI3UD4WMZI","bundle":"https://pith.science/pith/UDUMWARF6WPGMG2SVI3UD4WMZI/bundle.json","state":"https://pith.science/pith/UDUMWARF6WPGMG2SVI3UD4WMZI/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UDUMWARF6WPGMG2SVI3UD4WMZI/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:UDUMWARF6WPGMG2SVI3UD4WMZI","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":"1b263a5355ebf1ae95485faca04089e025a033b3fd61388eb07daa3b974d1909","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-09-05T21:23:44Z","title_canon_sha256":"d0f992630187f3d6ed1f966593755eb4e6c67a75bac660715779ee1b33a6125f"},"schema_version":"1.0","source":{"id":"2409.03914","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2409.03914","created_at":"2026-07-05T11:50:58Z"},{"alias_kind":"arxiv_version","alias_value":"2409.03914v3","created_at":"2026-07-05T11:50:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2409.03914","created_at":"2026-07-05T11:50:58Z"},{"alias_kind":"pith_short_12","alias_value":"UDUMWARF6WPG","created_at":"2026-07-05T11:50:58Z"},{"alias_kind":"pith_short_16","alias_value":"UDUMWARF6WPGMG2S","created_at":"2026-07-05T11:50:58Z"},{"alias_kind":"pith_short_8","alias_value":"UDUMWARF","created_at":"2026-07-05T11:50:58Z"}],"graph_snapshots":[{"event_id":"sha256:b64cc7053a5b92645d51ff9834b7506971b275fd41a009b0be5eab327d3db845","target":"graph","created_at":"2026-07-05T11:50:58Z","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/2409.03914/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We investigate the effect on cosmological evolution of a strongly coupled quantum field that undergoes renormalization group flow from a UV CFT to an IR CFT. The field theory is defined by perturbation of a holographic CFT by a relevant operator associated with a bulk scalar field that evolves from a local maximum of its potential near the boundary to a local minimum of its potential deep in the bulk. By studying the gravity solutions dual to this theory on $\\mathbb{R}^3 \\times S^1$, we find that the equation of state parameter $w$ for the field theory has the conformal behavior $w=1/3$ for hi","authors_text":"Mark Van Raamsdonk, Rana Zibakhsh","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-09-05T21:23:44Z","title":"Cosmology with non-conformal holographic matter"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2409.03914","kind":"arxiv","version":3},"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":"sha256:505abb6bb5b5a844ad423aee84cbd24c4e6a151a653f0f1b7d422f020fdb8d93","target":"record","created_at":"2026-07-05T11:50:58Z","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":"1b263a5355ebf1ae95485faca04089e025a033b3fd61388eb07daa3b974d1909","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-09-05T21:23:44Z","title_canon_sha256":"d0f992630187f3d6ed1f966593755eb4e6c67a75bac660715779ee1b33a6125f"},"schema_version":"1.0","source":{"id":"2409.03914","kind":"arxiv","version":3}},"canonical_sha256":"a0e8cb0225f59e661b52aa3741f2ccca3d05b9229f6552f289a8b72455aa0146","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a0e8cb0225f59e661b52aa3741f2ccca3d05b9229f6552f289a8b72455aa0146","first_computed_at":"2026-07-05T11:50:58.251076Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:50:58.251076Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"h9XXQ4AeRVyOn38cRyddy+IJ+51/nAbu7liZ6BlmFna/QhrZwPDa8E1v759bRF1D7Iy+Ol6zJoR7JKkaXfAHDg==","signature_status":"signed_v1","signed_at":"2026-07-05T11:50:58.251566Z","signed_message":"canonical_sha256_bytes"},"source_id":"2409.03914","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:505abb6bb5b5a844ad423aee84cbd24c4e6a151a653f0f1b7d422f020fdb8d93","sha256:b64cc7053a5b92645d51ff9834b7506971b275fd41a009b0be5eab327d3db845"],"state_sha256":"87eddf2aadb4ed2306a1002ae87208a76d819d3b76178422d07786ccbbec4fa6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QOgdBgss9kQpINPsPk4MWGMoKU5ilFQk5l81WEz6LZoMbEwT1SyWx+ED5Oxd/C3sWDNVftUkCjww77RYsuacCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-07T15:42:12.955411Z","bundle_sha256":"c85acd1bebc7ac2fa74b74ac1ecc9c0d6609a628c88233e18599a016a616b050"}}