{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:4CPL5CX6IFZV7SEOPC72C5NWKF","short_pith_number":"pith:4CPL5CX6","canonical_record":{"source":{"id":"1208.1098","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-08-06T07:15:42Z","cross_cats_sorted":[],"title_canon_sha256":"1643582789a69578b43d6a1d73022bd9a63ed64cefc971d6e906afa68c507545","abstract_canon_sha256":"8b75150f48533a7b4bff5c38db9528af9866e4fe1f5196d26c578af906d48595"},"schema_version":"1.0"},"canonical_sha256":"e09ebe8afe41735fc88e78bfa175b6515b56a213ba83f442c6531e1ff4a82752","source":{"kind":"arxiv","id":"1208.1098","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1208.1098","created_at":"2026-05-18T03:48:25Z"},{"alias_kind":"arxiv_version","alias_value":"1208.1098v1","created_at":"2026-05-18T03:48:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1208.1098","created_at":"2026-05-18T03:48:25Z"},{"alias_kind":"pith_short_12","alias_value":"4CPL5CX6IFZV","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_16","alias_value":"4CPL5CX6IFZV7SEO","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_8","alias_value":"4CPL5CX6","created_at":"2026-05-18T12:26:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:4CPL5CX6IFZV7SEOPC72C5NWKF","target":"record","payload":{"canonical_record":{"source":{"id":"1208.1098","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-08-06T07:15:42Z","cross_cats_sorted":[],"title_canon_sha256":"1643582789a69578b43d6a1d73022bd9a63ed64cefc971d6e906afa68c507545","abstract_canon_sha256":"8b75150f48533a7b4bff5c38db9528af9866e4fe1f5196d26c578af906d48595"},"schema_version":"1.0"},"canonical_sha256":"e09ebe8afe41735fc88e78bfa175b6515b56a213ba83f442c6531e1ff4a82752","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:48:25.011840Z","signature_b64":"HUnqoTPgSJU9r/VqHsPLv2+v4KMrxOwhmWJTKkkyiFAiAsYiCcBon1Tr/APJ3kw/fI4BHt3hI1WkQ45J7LzHAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e09ebe8afe41735fc88e78bfa175b6515b56a213ba83f442c6531e1ff4a82752","last_reissued_at":"2026-05-18T03:48:25.011158Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:48:25.011158Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1208.1098","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":"2026-05-18T03:48:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"B4yrXFqddrwzO9aciFezI7ykvFKleg5Y78VJtawsQj+fpFFAzAzTicpfaiwgOVOQ5maLkeX7giQADbmUou8uDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T08:07:10.732478Z"},"content_sha256":"1733771df64b9bf3643d2ad56847da1a7d42024b82c7f5961f6f705bb0776b63","schema_version":"1.0","event_id":"sha256:1733771df64b9bf3643d2ad56847da1a7d42024b82c7f5961f6f705bb0776b63"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:4CPL5CX6IFZV7SEOPC72C5NWKF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Active-to-absorbing state phase transition in the presence of fluctuating environments: Weak and strong dynamic scaling","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Abhik Basu, Niladri Sarkar","submitted_at":"2012-08-06T07:15:42Z","abstract_excerpt":"We investigate the scaling properties of phase transitions between survival and extinction (active-to-absorbing state phase transition, AAPT) in a model, that by itself belongs to the directed percolation (DP) universality class, interacting with a spatio-temporally fluctuating environment having its own non-trivial dynamics. We model the environment by (i) a randomly stirred fluid, governed by the Navier-Stokes (NS) equation, and (ii) a fluctuating surface, described either by the Kardar-Parisi-Zhang (KPZ) or the Edward-Wilkinson (EW) equations. We show, by using a one-loop perturbative field"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1208.1098","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":"2026-05-18T03:48:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jDJWSjDzQRYVn7AIafo4oWIdTb0Q+kfA5a98EGSP6M77lBAK9pCdG014Bp5o6v6tTcmCTNo5h29RMaVgPr1yAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T08:07:10.733147Z"},"content_sha256":"3fe94d59dd57847bf81dadca6421c3dbcaba5f0382918e12d0db8b9f85ab99ea","schema_version":"1.0","event_id":"sha256:3fe94d59dd57847bf81dadca6421c3dbcaba5f0382918e12d0db8b9f85ab99ea"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4CPL5CX6IFZV7SEOPC72C5NWKF/bundle.json","state_url":"https://pith.science/pith/4CPL5CX6IFZV7SEOPC72C5NWKF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4CPL5CX6IFZV7SEOPC72C5NWKF/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":"2026-05-27T08:07:10Z","links":{"resolver":"https://pith.science/pith/4CPL5CX6IFZV7SEOPC72C5NWKF","bundle":"https://pith.science/pith/4CPL5CX6IFZV7SEOPC72C5NWKF/bundle.json","state":"https://pith.science/pith/4CPL5CX6IFZV7SEOPC72C5NWKF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4CPL5CX6IFZV7SEOPC72C5NWKF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:4CPL5CX6IFZV7SEOPC72C5NWKF","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":"8b75150f48533a7b4bff5c38db9528af9866e4fe1f5196d26c578af906d48595","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-08-06T07:15:42Z","title_canon_sha256":"1643582789a69578b43d6a1d73022bd9a63ed64cefc971d6e906afa68c507545"},"schema_version":"1.0","source":{"id":"1208.1098","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1208.1098","created_at":"2026-05-18T03:48:25Z"},{"alias_kind":"arxiv_version","alias_value":"1208.1098v1","created_at":"2026-05-18T03:48:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1208.1098","created_at":"2026-05-18T03:48:25Z"},{"alias_kind":"pith_short_12","alias_value":"4CPL5CX6IFZV","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_16","alias_value":"4CPL5CX6IFZV7SEO","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_8","alias_value":"4CPL5CX6","created_at":"2026-05-18T12:26:53Z"}],"graph_snapshots":[{"event_id":"sha256:3fe94d59dd57847bf81dadca6421c3dbcaba5f0382918e12d0db8b9f85ab99ea","target":"graph","created_at":"2026-05-18T03:48:25Z","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":"We investigate the scaling properties of phase transitions between survival and extinction (active-to-absorbing state phase transition, AAPT) in a model, that by itself belongs to the directed percolation (DP) universality class, interacting with a spatio-temporally fluctuating environment having its own non-trivial dynamics. We model the environment by (i) a randomly stirred fluid, governed by the Navier-Stokes (NS) equation, and (ii) a fluctuating surface, described either by the Kardar-Parisi-Zhang (KPZ) or the Edward-Wilkinson (EW) equations. We show, by using a one-loop perturbative field","authors_text":"Abhik Basu, Niladri Sarkar","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-08-06T07:15:42Z","title":"Active-to-absorbing state phase transition in the presence of fluctuating environments: Weak and strong dynamic scaling"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1208.1098","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":"sha256:1733771df64b9bf3643d2ad56847da1a7d42024b82c7f5961f6f705bb0776b63","target":"record","created_at":"2026-05-18T03:48:25Z","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":"8b75150f48533a7b4bff5c38db9528af9866e4fe1f5196d26c578af906d48595","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-08-06T07:15:42Z","title_canon_sha256":"1643582789a69578b43d6a1d73022bd9a63ed64cefc971d6e906afa68c507545"},"schema_version":"1.0","source":{"id":"1208.1098","kind":"arxiv","version":1}},"canonical_sha256":"e09ebe8afe41735fc88e78bfa175b6515b56a213ba83f442c6531e1ff4a82752","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e09ebe8afe41735fc88e78bfa175b6515b56a213ba83f442c6531e1ff4a82752","first_computed_at":"2026-05-18T03:48:25.011158Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:48:25.011158Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"HUnqoTPgSJU9r/VqHsPLv2+v4KMrxOwhmWJTKkkyiFAiAsYiCcBon1Tr/APJ3kw/fI4BHt3hI1WkQ45J7LzHAA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:48:25.011840Z","signed_message":"canonical_sha256_bytes"},"source_id":"1208.1098","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1733771df64b9bf3643d2ad56847da1a7d42024b82c7f5961f6f705bb0776b63","sha256:3fe94d59dd57847bf81dadca6421c3dbcaba5f0382918e12d0db8b9f85ab99ea"],"state_sha256":"dbd979f098e1b0ed6a06d09ddd76ce742e0edbc84acb02806fe85d68197d8868"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NTEGMIx20rI3ZMuW/XBcRjI97VHV5otqydxGvFsOqMCFMdY+6gz5eyqaUJdqapWF2Lxfc88NEEd9q/3bVduUCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T08:07:10.736966Z","bundle_sha256":"20c350d875f55937871412683ed47caa43dc15028d6969f81c44726cd8214ad9"}}