{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1992:5KQQTI2NJRXAPF2Z4D5RJVGW5X","short_pith_number":"pith:5KQQTI2N","schema_version":"1.0","canonical_sha256":"eaa109a34d4c6e079759e0fb14d4d6edc648ac890affbc35f5398e6f476f5364","source":{"kind":"arxiv","id":"hep-ph/9209229","version":1},"attestation_state":"computed","paper":{"title":"Baryon Number Diffusion and Instabilities in the Quark/Hadron Phase Transition","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Fred C. Adams, J. S. Langer, Katherine Freese","submitted_at":"1992-09-11T21:18:00Z","abstract_excerpt":"Hadron bubbles that nucleate with radius $R_{nuc}$ in a quark sea (if the phase transition is first order) are shown to be unstable to the growth of nonspherical structure when the bubble radii exceed a critical size of $20 - 10^3$ $R_{nuc}$. This instability is driven by a very thin layer of slowly diffusing excess baryon number that forms on the surface of the bubble wall and limits its growth. This instability occurs on a shorter length scale than those studied previously and these effects can thus be important for both cosmology and heavy ion collisions."},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"hep-ph/9209229","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1992-09-11T21:18:00Z","cross_cats_sorted":[],"title_canon_sha256":"fdc678fb246ce493a770648ce4301e271c2ffda31d7b2a51746dda365fbf6cd8","abstract_canon_sha256":"0822f56dc99879d0fdee47a7b793a01c8103cf00b32cf72a1a709fab8515ed5f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:29:26.529126Z","signature_b64":"YqLurlcntECLDJmCiudmTIbJqn+2dQlkneRRDxYJbMu4f9GpzFzKuMxOBn4/iItDDxqxXRKQ4iq25wzrcwoUBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"eaa109a34d4c6e079759e0fb14d4d6edc648ac890affbc35f5398e6f476f5364","last_reissued_at":"2026-07-04T14:29:26.528622Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:29:26.528622Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Baryon Number Diffusion and Instabilities in the Quark/Hadron Phase Transition","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Fred C. Adams, J. S. Langer, Katherine Freese","submitted_at":"1992-09-11T21:18:00Z","abstract_excerpt":"Hadron bubbles that nucleate with radius $R_{nuc}$ in a quark sea (if the phase transition is first order) are shown to be unstable to the growth of nonspherical structure when the bubble radii exceed a critical size of $20 - 10^3$ $R_{nuc}$. This instability is driven by a very thin layer of slowly diffusing excess baryon number that forms on the surface of the bubble wall and limits its growth. This instability occurs on a shorter length scale than those studied previously and these effects can thus be important for both cosmology and heavy ion collisions."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9209229","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/9209229/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9209229","created_at":"2026-07-04T14:29:26.528690+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9209229v1","created_at":"2026-07-04T14:29:26.528690+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9209229","created_at":"2026-07-04T14:29:26.528690+00:00"},{"alias_kind":"pith_short_12","alias_value":"5KQQTI2NJRXA","created_at":"2026-07-04T14:29:26.528690+00:00"},{"alias_kind":"pith_short_16","alias_value":"5KQQTI2NJRXAPF2Z","created_at":"2026-07-04T14:29:26.528690+00:00"},{"alias_kind":"pith_short_8","alias_value":"5KQQTI2N","created_at":"2026-07-04T14:29:26.528690+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5KQQTI2NJRXAPF2Z4D5RJVGW5X","json":"https://pith.science/pith/5KQQTI2NJRXAPF2Z4D5RJVGW5X.json","graph_json":"https://pith.science/api/pith-number/5KQQTI2NJRXAPF2Z4D5RJVGW5X/graph.json","events_json":"https://pith.science/api/pith-number/5KQQTI2NJRXAPF2Z4D5RJVGW5X/events.json","paper":"https://pith.science/paper/5KQQTI2N"},"agent_actions":{"view_html":"https://pith.science/pith/5KQQTI2NJRXAPF2Z4D5RJVGW5X","download_json":"https://pith.science/pith/5KQQTI2NJRXAPF2Z4D5RJVGW5X.json","view_paper":"https://pith.science/paper/5KQQTI2N","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9209229&json=true","fetch_graph":"https://pith.science/api/pith-number/5KQQTI2NJRXAPF2Z4D5RJVGW5X/graph.json","fetch_events":"https://pith.science/api/pith-number/5KQQTI2NJRXAPF2Z4D5RJVGW5X/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5KQQTI2NJRXAPF2Z4D5RJVGW5X/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5KQQTI2NJRXAPF2Z4D5RJVGW5X/action/storage_attestation","attest_author":"https://pith.science/pith/5KQQTI2NJRXAPF2Z4D5RJVGW5X/action/author_attestation","sign_citation":"https://pith.science/pith/5KQQTI2NJRXAPF2Z4D5RJVGW5X/action/citation_signature","submit_replication":"https://pith.science/pith/5KQQTI2NJRXAPF2Z4D5RJVGW5X/action/replication_record"}},"created_at":"2026-07-04T14:29:26.528690+00:00","updated_at":"2026-07-04T14:29:26.528690+00:00"}