{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1995:LVBR4I4AFOBYFFILFBWPXVANKL","short_pith_number":"pith:LVBR4I4A","canonical_record":{"source":{"id":"hep-ph/9512202","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1995-12-01T09:07:22Z","cross_cats_sorted":["astro-ph"],"title_canon_sha256":"f37b136a221197414462145d686887f7ce45e530c496a5226839486a1d13e8e5","abstract_canon_sha256":"7d20ea47cb129a1748a18cc359f8c922b736c67a746f3d258025c66aa09dadf2"},"schema_version":"1.0"},"canonical_sha256":"5d431e23802b8382950b286cfbd40d52fed1600dfa736819858c220686d1dba4","source":{"kind":"arxiv","id":"hep-ph/9512202","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9512202","created_at":"2026-07-04T15:59:17Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9512202v1","created_at":"2026-07-04T15:59:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9512202","created_at":"2026-07-04T15:59:17Z"},{"alias_kind":"pith_short_12","alias_value":"LVBR4I4AFOBY","created_at":"2026-07-04T15:59:17Z"},{"alias_kind":"pith_short_16","alias_value":"LVBR4I4AFOBYFFIL","created_at":"2026-07-04T15:59:17Z"},{"alias_kind":"pith_short_8","alias_value":"LVBR4I4A","created_at":"2026-07-04T15:59:17Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1995:LVBR4I4AFOBYFFILFBWPXVANKL","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9512202","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1995-12-01T09:07:22Z","cross_cats_sorted":["astro-ph"],"title_canon_sha256":"f37b136a221197414462145d686887f7ce45e530c496a5226839486a1d13e8e5","abstract_canon_sha256":"7d20ea47cb129a1748a18cc359f8c922b736c67a746f3d258025c66aa09dadf2"},"schema_version":"1.0"},"canonical_sha256":"5d431e23802b8382950b286cfbd40d52fed1600dfa736819858c220686d1dba4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:59:17.465262Z","signature_b64":"w5IYzcU8lBFp+QlnfBB/tQFDu9RzWBJ3ZWy220IXErbnz5gas1QJkUIZo7S31yd4j8GMcf2NeJ6o7Ct9+RtICA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5d431e23802b8382950b286cfbd40d52fed1600dfa736819858c220686d1dba4","last_reissued_at":"2026-07-04T15:59:17.464925Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:59:17.464925Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9512202","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":"2026-07-04T15:59:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5nPRIyETX9qwTFpvqm4K4+2ZoCRSVN3bAmynYq/Q5kTlK+D45PkTn41gTmlxFd0u+tWx44m9rhCQWXJLZkJgCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-13T17:06:51.189734Z"},"content_sha256":"51fa779c9fe7351d97fcea7bcd6070f54ece5855cda011ec4f14c516ec7858ef","schema_version":"1.0","event_id":"sha256:51fa779c9fe7351d97fcea7bcd6070f54ece5855cda011ec4f14c516ec7858ef"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1995:LVBR4I4AFOBYFFILFBWPXVANKL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"On Bubble Growth and Droplet Decay in Cosmological Phase Transitions","license":"","headline":"","cross_cats":["astro-ph"],"primary_cat":"hep-ph","authors_text":"H.Kurki-Suonio, M.Laine","submitted_at":"1995-12-01T09:07:22Z","abstract_excerpt":"We study spherically symmetric bubble growth and droplet decay in first order cosmological phase transitions, using a numerical code including both the complete hydrodynamics of the problem and a phenomenological model for the microscopic entropy producing mechanism at the phase transition surface. The small-scale effects of finite wall width and surface tension are thus consistently incorporated. We verify the existence of the different hydrodynamical growth modes proposed recently and investigate the problem of a decaying quark droplet in the QCD phase transition. We find that the decaying d"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9512202","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/9512202/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":"2026-07-04T15:59:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cjsGfBGoJ9BB0KwVUH/4Oaf4E/JormTtsaD14fegfnuTU9ZRkffjJpWUSKa2FwVH+j555x29tjHFv1nqvmKABg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-13T17:06:51.190702Z"},"content_sha256":"b74229f62bfd6675405c84a582465c8812ba5c3c8a0088bf60117fc9bae26370","schema_version":"1.0","event_id":"sha256:b74229f62bfd6675405c84a582465c8812ba5c3c8a0088bf60117fc9bae26370"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LVBR4I4AFOBYFFILFBWPXVANKL/bundle.json","state_url":"https://pith.science/pith/LVBR4I4AFOBYFFILFBWPXVANKL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LVBR4I4AFOBYFFILFBWPXVANKL/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":"2026-08-13T17:06:51Z","links":{"resolver":"https://pith.science/pith/LVBR4I4AFOBYFFILFBWPXVANKL","bundle":"https://pith.science/pith/LVBR4I4AFOBYFFILFBWPXVANKL/bundle.json","state":"https://pith.science/pith/LVBR4I4AFOBYFFILFBWPXVANKL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LVBR4I4AFOBYFFILFBWPXVANKL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1995:LVBR4I4AFOBYFFILFBWPXVANKL","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":"7d20ea47cb129a1748a18cc359f8c922b736c67a746f3d258025c66aa09dadf2","cross_cats_sorted":["astro-ph"],"license":"","primary_cat":"hep-ph","submitted_at":"1995-12-01T09:07:22Z","title_canon_sha256":"f37b136a221197414462145d686887f7ce45e530c496a5226839486a1d13e8e5"},"schema_version":"1.0","source":{"id":"hep-ph/9512202","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9512202","created_at":"2026-07-04T15:59:17Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9512202v1","created_at":"2026-07-04T15:59:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9512202","created_at":"2026-07-04T15:59:17Z"},{"alias_kind":"pith_short_12","alias_value":"LVBR4I4AFOBY","created_at":"2026-07-04T15:59:17Z"},{"alias_kind":"pith_short_16","alias_value":"LVBR4I4AFOBYFFIL","created_at":"2026-07-04T15:59:17Z"},{"alias_kind":"pith_short_8","alias_value":"LVBR4I4A","created_at":"2026-07-04T15:59:17Z"}],"graph_snapshots":[{"event_id":"sha256:b74229f62bfd6675405c84a582465c8812ba5c3c8a0088bf60117fc9bae26370","target":"graph","created_at":"2026-07-04T15:59:17Z","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/hep-ph/9512202/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study spherically symmetric bubble growth and droplet decay in first order cosmological phase transitions, using a numerical code including both the complete hydrodynamics of the problem and a phenomenological model for the microscopic entropy producing mechanism at the phase transition surface. The small-scale effects of finite wall width and surface tension are thus consistently incorporated. We verify the existence of the different hydrodynamical growth modes proposed recently and investigate the problem of a decaying quark droplet in the QCD phase transition. We find that the decaying d","authors_text":"H.Kurki-Suonio, M.Laine","cross_cats":["astro-ph"],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1995-12-01T09:07:22Z","title":"On Bubble Growth and Droplet Decay in Cosmological Phase Transitions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9512202","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":"sha256:51fa779c9fe7351d97fcea7bcd6070f54ece5855cda011ec4f14c516ec7858ef","target":"record","created_at":"2026-07-04T15:59:17Z","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":"7d20ea47cb129a1748a18cc359f8c922b736c67a746f3d258025c66aa09dadf2","cross_cats_sorted":["astro-ph"],"license":"","primary_cat":"hep-ph","submitted_at":"1995-12-01T09:07:22Z","title_canon_sha256":"f37b136a221197414462145d686887f7ce45e530c496a5226839486a1d13e8e5"},"schema_version":"1.0","source":{"id":"hep-ph/9512202","kind":"arxiv","version":1}},"canonical_sha256":"5d431e23802b8382950b286cfbd40d52fed1600dfa736819858c220686d1dba4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5d431e23802b8382950b286cfbd40d52fed1600dfa736819858c220686d1dba4","first_computed_at":"2026-07-04T15:59:17.464925Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:59:17.464925Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"w5IYzcU8lBFp+QlnfBB/tQFDu9RzWBJ3ZWy220IXErbnz5gas1QJkUIZo7S31yd4j8GMcf2NeJ6o7Ct9+RtICA==","signature_status":"signed_v1","signed_at":"2026-07-04T15:59:17.465262Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9512202","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:51fa779c9fe7351d97fcea7bcd6070f54ece5855cda011ec4f14c516ec7858ef","sha256:b74229f62bfd6675405c84a582465c8812ba5c3c8a0088bf60117fc9bae26370"],"state_sha256":"9c8046a0f45fef8fb9eaeaefba48030445a5d84398642b59a442ca58471089b6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"MLeQgjAulHpDr2QoIVmhfyRO01AVFJMTf3Zxo7fnDdEBV+NaEhz/6sQltYyEFBKh2ofZTqEXG7yX5QY1FUMSAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-13T17:06:51.234871Z","bundle_sha256":"154aee9dd135044aabf20290799cdfafc6f5849c1963b1a7b09ffffb9f3d828b"}}