{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:2RDWKK6ETDHKI4TB7LLDWA34LT","short_pith_number":"pith:2RDWKK6E","canonical_record":{"source":{"id":"1711.04704","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-11-13T17:01:29Z","cross_cats_sorted":[],"title_canon_sha256":"ee5397683fe96815877f4f64aa74f5ca4aa58eff0038b124fabec5f0958123fe","abstract_canon_sha256":"2e62792702d0483e6464ac6e082737e05cb81449ae8bc86ad312ad13bb909864"},"schema_version":"1.0"},"canonical_sha256":"d447652bc498cea47261fad63b037c5cf2f1a52544fa39979dc534d11de3cd16","source":{"kind":"arxiv","id":"1711.04704","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.04704","created_at":"2026-05-18T00:01:49Z"},{"alias_kind":"arxiv_version","alias_value":"1711.04704v2","created_at":"2026-05-18T00:01:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.04704","created_at":"2026-05-18T00:01:49Z"},{"alias_kind":"pith_short_12","alias_value":"2RDWKK6ETDHK","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_16","alias_value":"2RDWKK6ETDHKI4TB","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_8","alias_value":"2RDWKK6E","created_at":"2026-05-18T12:30:55Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:2RDWKK6ETDHKI4TB7LLDWA34LT","target":"record","payload":{"canonical_record":{"source":{"id":"1711.04704","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-11-13T17:01:29Z","cross_cats_sorted":[],"title_canon_sha256":"ee5397683fe96815877f4f64aa74f5ca4aa58eff0038b124fabec5f0958123fe","abstract_canon_sha256":"2e62792702d0483e6464ac6e082737e05cb81449ae8bc86ad312ad13bb909864"},"schema_version":"1.0"},"canonical_sha256":"d447652bc498cea47261fad63b037c5cf2f1a52544fa39979dc534d11de3cd16","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:01:49.102041Z","signature_b64":"m+usjmxLAWhX5/EzRZ66yqA2DocDUtNCbFohdSPz7wssT3MCrCT0UUwqj/fZj384d8Awrl4VSGXBEN+ruRzZBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d447652bc498cea47261fad63b037c5cf2f1a52544fa39979dc534d11de3cd16","last_reissued_at":"2026-05-18T00:01:49.101312Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:01:49.101312Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1711.04704","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":"2026-05-18T00:01:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6c6wWN+WoR20UzeNap9ruFn7U++i6xgidK4XcAZWHhEiVE44d1FPUb+jIyx0Pm76BtDI+4w2QmUFj8dqO+ozAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T18:11:48.155121Z"},"content_sha256":"cf7ac6fbeead560bb93a135a66f5730f2aafe34b365932b18637309761d106f0","schema_version":"1.0","event_id":"sha256:cf7ac6fbeead560bb93a135a66f5730f2aafe34b365932b18637309761d106f0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:2RDWKK6ETDHKI4TB7LLDWA34LT","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Evolution of thick domain walls in inflationary and $p=w\\rho$ universe","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"A.D. Dolgov, A.S. Rudenko, S.I. Godunov","submitted_at":"2017-11-13T17:01:29Z","abstract_excerpt":"We study the evolution of thick domain walls in the different models of cosmological inflation, in the matter-dominated and radiation-dominated universe, or more generally in the universe with the equation of state $p=w\\rho$. We have found that the domain wall evolution crucially depends on the time-dependent parameter $C(t)=1/(H(t)\\delta_0)^2$, where $H(t)$ is the Hubble parameter and $\\delta_0$ is the thickness of the wall in flat space-time. For $C(t)>2$ the physical thickness of the wall, $a(t)\\delta(t)$, tends with time to $\\delta_0$, which is microscopically small. Otherwise, when $C(t) "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.04704","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":""},"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":"2026-05-18T00:01:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YkmkzLvQ/Os+dcg6gztKmm7fID1eV8U/WMXGUGNlm3VCUDhhvSp8jrqJ11YseUtaUwmoMdn2teuMQaHZYx13Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T18:11:48.155481Z"},"content_sha256":"ed9831357f4a91a7dc3466d2e017d19d8d8c6c01f52475a09389e06c4b8595e5","schema_version":"1.0","event_id":"sha256:ed9831357f4a91a7dc3466d2e017d19d8d8c6c01f52475a09389e06c4b8595e5"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2RDWKK6ETDHKI4TB7LLDWA34LT/bundle.json","state_url":"https://pith.science/pith/2RDWKK6ETDHKI4TB7LLDWA34LT/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2RDWKK6ETDHKI4TB7LLDWA34LT/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":"2026-06-02T18:11:48Z","links":{"resolver":"https://pith.science/pith/2RDWKK6ETDHKI4TB7LLDWA34LT","bundle":"https://pith.science/pith/2RDWKK6ETDHKI4TB7LLDWA34LT/bundle.json","state":"https://pith.science/pith/2RDWKK6ETDHKI4TB7LLDWA34LT/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2RDWKK6ETDHKI4TB7LLDWA34LT/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:2RDWKK6ETDHKI4TB7LLDWA34LT","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":"2e62792702d0483e6464ac6e082737e05cb81449ae8bc86ad312ad13bb909864","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-11-13T17:01:29Z","title_canon_sha256":"ee5397683fe96815877f4f64aa74f5ca4aa58eff0038b124fabec5f0958123fe"},"schema_version":"1.0","source":{"id":"1711.04704","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.04704","created_at":"2026-05-18T00:01:49Z"},{"alias_kind":"arxiv_version","alias_value":"1711.04704v2","created_at":"2026-05-18T00:01:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.04704","created_at":"2026-05-18T00:01:49Z"},{"alias_kind":"pith_short_12","alias_value":"2RDWKK6ETDHK","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_16","alias_value":"2RDWKK6ETDHKI4TB","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_8","alias_value":"2RDWKK6E","created_at":"2026-05-18T12:30:55Z"}],"graph_snapshots":[{"event_id":"sha256:ed9831357f4a91a7dc3466d2e017d19d8d8c6c01f52475a09389e06c4b8595e5","target":"graph","created_at":"2026-05-18T00:01:49Z","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 study the evolution of thick domain walls in the different models of cosmological inflation, in the matter-dominated and radiation-dominated universe, or more generally in the universe with the equation of state $p=w\\rho$. We have found that the domain wall evolution crucially depends on the time-dependent parameter $C(t)=1/(H(t)\\delta_0)^2$, where $H(t)$ is the Hubble parameter and $\\delta_0$ is the thickness of the wall in flat space-time. For $C(t)>2$ the physical thickness of the wall, $a(t)\\delta(t)$, tends with time to $\\delta_0$, which is microscopically small. Otherwise, when $C(t) ","authors_text":"A.D. Dolgov, A.S. Rudenko, S.I. Godunov","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-11-13T17:01:29Z","title":"Evolution of thick domain walls in inflationary and $p=w\\rho$ universe"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.04704","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:cf7ac6fbeead560bb93a135a66f5730f2aafe34b365932b18637309761d106f0","target":"record","created_at":"2026-05-18T00:01:49Z","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":"2e62792702d0483e6464ac6e082737e05cb81449ae8bc86ad312ad13bb909864","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2017-11-13T17:01:29Z","title_canon_sha256":"ee5397683fe96815877f4f64aa74f5ca4aa58eff0038b124fabec5f0958123fe"},"schema_version":"1.0","source":{"id":"1711.04704","kind":"arxiv","version":2}},"canonical_sha256":"d447652bc498cea47261fad63b037c5cf2f1a52544fa39979dc534d11de3cd16","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d447652bc498cea47261fad63b037c5cf2f1a52544fa39979dc534d11de3cd16","first_computed_at":"2026-05-18T00:01:49.101312Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:01:49.101312Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"m+usjmxLAWhX5/EzRZ66yqA2DocDUtNCbFohdSPz7wssT3MCrCT0UUwqj/fZj384d8Awrl4VSGXBEN+ruRzZBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:01:49.102041Z","signed_message":"canonical_sha256_bytes"},"source_id":"1711.04704","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cf7ac6fbeead560bb93a135a66f5730f2aafe34b365932b18637309761d106f0","sha256:ed9831357f4a91a7dc3466d2e017d19d8d8c6c01f52475a09389e06c4b8595e5"],"state_sha256":"ed00865bbd4a4578e51a6d2040d7d0812045e1159656c45c8a69aa39bed47277"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Kh3vgpeQ/ySbJotv46hAKWyccyCv1KEhQ08kMZQ1ssPnP1Ix2W4mviw9nPP7WaGacZcscTnOQr/m2q85T1i5Dg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T18:11:48.157355Z","bundle_sha256":"9623397c0d76562d959c262fb9440f7988c1c2a6a31a226c543c09d16508a68d"}}