{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:S6ASEK5XVBADSQVHFDCJDWYPH7","short_pith_number":"pith:S6ASEK5X","canonical_record":{"source":{"id":"1205.2579","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2012-05-11T17:03:26Z","cross_cats_sorted":["physics.plasm-ph"],"title_canon_sha256":"cbbcddec4460327c89f31c770fc532bc01865a62503c34a850611927226d6e1a","abstract_canon_sha256":"f1f54f050d37efa65b7538af991414858c164baa6410a8d87ff09eff87afcd76"},"schema_version":"1.0"},"canonical_sha256":"9781222bb7a8403942a728c491db0f3fe0fe99cf3fe9d2c2e18b630e2b747c2f","source":{"kind":"arxiv","id":"1205.2579","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1205.2579","created_at":"2026-05-18T03:27:01Z"},{"alias_kind":"arxiv_version","alias_value":"1205.2579v2","created_at":"2026-05-18T03:27:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1205.2579","created_at":"2026-05-18T03:27:01Z"},{"alias_kind":"pith_short_12","alias_value":"S6ASEK5XVBAD","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_16","alias_value":"S6ASEK5XVBADSQVH","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_8","alias_value":"S6ASEK5X","created_at":"2026-05-18T12:27:20Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:S6ASEK5XVBADSQVHFDCJDWYPH7","target":"record","payload":{"canonical_record":{"source":{"id":"1205.2579","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2012-05-11T17:03:26Z","cross_cats_sorted":["physics.plasm-ph"],"title_canon_sha256":"cbbcddec4460327c89f31c770fc532bc01865a62503c34a850611927226d6e1a","abstract_canon_sha256":"f1f54f050d37efa65b7538af991414858c164baa6410a8d87ff09eff87afcd76"},"schema_version":"1.0"},"canonical_sha256":"9781222bb7a8403942a728c491db0f3fe0fe99cf3fe9d2c2e18b630e2b747c2f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:27:01.717027Z","signature_b64":"wlBQSriiViCK8h2VWC99USHZCkpzdoikCHqA9Weywi+t9QnURirjPKAOczvLd/uhwODv7JSoYke/j0umC9w6AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9781222bb7a8403942a728c491db0f3fe0fe99cf3fe9d2c2e18b630e2b747c2f","last_reissued_at":"2026-05-18T03:27:01.716538Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:27:01.716538Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1205.2579","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":"2026-05-18T03:27:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QEKwSggFiqpdQ0dQTyaNC3teHOvVIzVMxZ8gK4Wc/EdDNbGxIGDYIkstQXGtjIGf4At24W+SfX6WRn4kbveVCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T22:53:05.754120Z"},"content_sha256":"ff1e1442d20e7de48073ec3de19dbdd256f8ae23edb56c98f0ac8fa58713d122","schema_version":"1.0","event_id":"sha256:ff1e1442d20e7de48073ec3de19dbdd256f8ae23edb56c98f0ac8fa58713d122"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:S6ASEK5XVBADSQVHFDCJDWYPH7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dynamics of volumetrically heated matter passing through the liquid-vapor metastable states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.plasm-ph"],"primary_cat":"physics.flu-dyn","authors_text":"2), 2) ((1) ITP, (2) EMMI, 3), (3) ITEP, 4, (4) JIHT-RAS, 5), (5) MIPT, Anna Tauschwitz (1, Darmstadt, Germany, Goethe-Universit\\\"at Frankfurt am Main, GSI GmbH, Igor Iosilevskiy (2, Joachim A. Maruhn (1, Mikhail M. Basko (2, Moscow, Moscow region, Russia, Russia), Steffen Faik (1)","submitted_at":"2012-05-11T17:03:26Z","abstract_excerpt":"Remaining within the pure hydrodynamic approach, we formulate a self-consistent model for simulating the dynamic behavior of matter passing through metastable states in the two-phase liquid-vapor region of the phase diagram. The model is based on the local criterion of explosive boiling, derived by applying the theory of homogeneous bubble nucleation in superheated liquids. Practical application of the proposed model is illustrated with hydrodynamic simulations of a volumetrically uniformly heated planar layer of fused silica SiO2. Implications for experimentally measurable quantities are brie"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1205.2579","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":"2026-05-18T03:27:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"EeA0dY2KjNi9yktJ02gSCvjS92bOhe2M+SG5hibJ/6zQzZtzfO4B9h1zBVJYm7g+xRtI/31hLYFRjoS/RTobAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T22:53:05.754796Z"},"content_sha256":"6532d9a86e1a6a7b487cec10ca0b96afe5f807913631a67d53bf615968daedb7","schema_version":"1.0","event_id":"sha256:6532d9a86e1a6a7b487cec10ca0b96afe5f807913631a67d53bf615968daedb7"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/S6ASEK5XVBADSQVHFDCJDWYPH7/bundle.json","state_url":"https://pith.science/pith/S6ASEK5XVBADSQVHFDCJDWYPH7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/S6ASEK5XVBADSQVHFDCJDWYPH7/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":"2026-05-28T22:53:05Z","links":{"resolver":"https://pith.science/pith/S6ASEK5XVBADSQVHFDCJDWYPH7","bundle":"https://pith.science/pith/S6ASEK5XVBADSQVHFDCJDWYPH7/bundle.json","state":"https://pith.science/pith/S6ASEK5XVBADSQVHFDCJDWYPH7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/S6ASEK5XVBADSQVHFDCJDWYPH7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:S6ASEK5XVBADSQVHFDCJDWYPH7","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":"f1f54f050d37efa65b7538af991414858c164baa6410a8d87ff09eff87afcd76","cross_cats_sorted":["physics.plasm-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2012-05-11T17:03:26Z","title_canon_sha256":"cbbcddec4460327c89f31c770fc532bc01865a62503c34a850611927226d6e1a"},"schema_version":"1.0","source":{"id":"1205.2579","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1205.2579","created_at":"2026-05-18T03:27:01Z"},{"alias_kind":"arxiv_version","alias_value":"1205.2579v2","created_at":"2026-05-18T03:27:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1205.2579","created_at":"2026-05-18T03:27:01Z"},{"alias_kind":"pith_short_12","alias_value":"S6ASEK5XVBAD","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_16","alias_value":"S6ASEK5XVBADSQVH","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_8","alias_value":"S6ASEK5X","created_at":"2026-05-18T12:27:20Z"}],"graph_snapshots":[{"event_id":"sha256:6532d9a86e1a6a7b487cec10ca0b96afe5f807913631a67d53bf615968daedb7","target":"graph","created_at":"2026-05-18T03:27:01Z","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":"Remaining within the pure hydrodynamic approach, we formulate a self-consistent model for simulating the dynamic behavior of matter passing through metastable states in the two-phase liquid-vapor region of the phase diagram. The model is based on the local criterion of explosive boiling, derived by applying the theory of homogeneous bubble nucleation in superheated liquids. Practical application of the proposed model is illustrated with hydrodynamic simulations of a volumetrically uniformly heated planar layer of fused silica SiO2. Implications for experimentally measurable quantities are brie","authors_text":"2), 2) ((1) ITP, (2) EMMI, 3), (3) ITEP, 4, (4) JIHT-RAS, 5), (5) MIPT, Anna Tauschwitz (1, Darmstadt, Germany, Goethe-Universit\\\"at Frankfurt am Main, GSI GmbH, Igor Iosilevskiy (2, Joachim A. Maruhn (1, Mikhail M. Basko (2, Moscow, Moscow region, Russia, Russia), Steffen Faik (1)","cross_cats":["physics.plasm-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2012-05-11T17:03:26Z","title":"Dynamics of volumetrically heated matter passing through the liquid-vapor metastable states"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1205.2579","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:ff1e1442d20e7de48073ec3de19dbdd256f8ae23edb56c98f0ac8fa58713d122","target":"record","created_at":"2026-05-18T03:27:01Z","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":"f1f54f050d37efa65b7538af991414858c164baa6410a8d87ff09eff87afcd76","cross_cats_sorted":["physics.plasm-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2012-05-11T17:03:26Z","title_canon_sha256":"cbbcddec4460327c89f31c770fc532bc01865a62503c34a850611927226d6e1a"},"schema_version":"1.0","source":{"id":"1205.2579","kind":"arxiv","version":2}},"canonical_sha256":"9781222bb7a8403942a728c491db0f3fe0fe99cf3fe9d2c2e18b630e2b747c2f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9781222bb7a8403942a728c491db0f3fe0fe99cf3fe9d2c2e18b630e2b747c2f","first_computed_at":"2026-05-18T03:27:01.716538Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:27:01.716538Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"wlBQSriiViCK8h2VWC99USHZCkpzdoikCHqA9Weywi+t9QnURirjPKAOczvLd/uhwODv7JSoYke/j0umC9w6AQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:27:01.717027Z","signed_message":"canonical_sha256_bytes"},"source_id":"1205.2579","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ff1e1442d20e7de48073ec3de19dbdd256f8ae23edb56c98f0ac8fa58713d122","sha256:6532d9a86e1a6a7b487cec10ca0b96afe5f807913631a67d53bf615968daedb7"],"state_sha256":"450b6142bb3cb026e761e5ecd9ce620757eeba70ad691aa9a969a2768770be80"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oytbpt0Q1kgrsOMO8xDV3TIMN7Nz7i4hSEmTAFGs2TugRxNlkw3cfkIzH1X6/2olQHmHMBomqVJnLWhAq5BQCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T22:53:05.758388Z","bundle_sha256":"85ca43dadbf7cd9eba9803fd7fa656fd70093ded27143fc2cf2190bd8ed1c7ed"}}