{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:DD6G2E5Q6RYAZ7NAERC7IL6A7Q","short_pith_number":"pith:DD6G2E5Q","schema_version":"1.0","canonical_sha256":"18fc6d13b0f4700cfda02445f42fc0fc3892d26f758243e4bc75ffedf079cd06","source":{"kind":"arxiv","id":"1011.5140","version":5},"attestation_state":"computed","paper":{"title":"Diffusive counter dispersion of mass in bubbly media","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.chem-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Denis S. Goldobin, Nikolai V. Brilliantov","submitted_at":"2010-11-23T15:58:22Z","abstract_excerpt":"We consider a liquid bearing gas bubbles in a porous medium. When gas bubbles are immovably trapped in a porous matrix by surface-tension forces, the dominant mechanism of transfer of gas mass becomes the diffusion of gas molecules through the liquid. Essentially, the gas solution is in local thermodynamic equilibrium with vapor phase all over the system, i.e., the solute concentration equals the solubility. When temperature and/or pressure gradients are applied, diffusion fluxes appear and these fluxes are faithfully determined by the temperature and pressure fields, not by the local solute c"},"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":"1011.5140","kind":"arxiv","version":5},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2010-11-23T15:58:22Z","cross_cats_sorted":["physics.chem-ph"],"title_canon_sha256":"fb126473514e0430813245c6d76fa41a5a00199cae4abe6639c8c1362c5b9383","abstract_canon_sha256":"7303a580bcfe24675a55eadb77728deb3ff3212452b5ca6b82ea8c551370a83c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:23:23.869094Z","signature_b64":"f7DkGA8gzjiHikeyeOPyUky1ydTK8r4USMrRofcqLtG3vgIgxsri+GIVxp3LUPkNnzP0lUf2bCkdsnTPpRNJBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"18fc6d13b0f4700cfda02445f42fc0fc3892d26f758243e4bc75ffedf079cd06","last_reissued_at":"2026-05-18T02:23:23.868498Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:23:23.868498Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Diffusive counter dispersion of mass in bubbly media","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.chem-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Denis S. Goldobin, Nikolai V. Brilliantov","submitted_at":"2010-11-23T15:58:22Z","abstract_excerpt":"We consider a liquid bearing gas bubbles in a porous medium. When gas bubbles are immovably trapped in a porous matrix by surface-tension forces, the dominant mechanism of transfer of gas mass becomes the diffusion of gas molecules through the liquid. Essentially, the gas solution is in local thermodynamic equilibrium with vapor phase all over the system, i.e., the solute concentration equals the solubility. When temperature and/or pressure gradients are applied, diffusion fluxes appear and these fluxes are faithfully determined by the temperature and pressure fields, not by the local solute c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1011.5140","kind":"arxiv","version":5},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1011.5140","created_at":"2026-05-18T02:23:23.868578+00:00"},{"alias_kind":"arxiv_version","alias_value":"1011.5140v5","created_at":"2026-05-18T02:23:23.868578+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1011.5140","created_at":"2026-05-18T02:23:23.868578+00:00"},{"alias_kind":"pith_short_12","alias_value":"DD6G2E5Q6RYA","created_at":"2026-05-18T12:26:06.534383+00:00"},{"alias_kind":"pith_short_16","alias_value":"DD6G2E5Q6RYAZ7NA","created_at":"2026-05-18T12:26:06.534383+00:00"},{"alias_kind":"pith_short_8","alias_value":"DD6G2E5Q","created_at":"2026-05-18T12:26:06.534383+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/DD6G2E5Q6RYAZ7NAERC7IL6A7Q","json":"https://pith.science/pith/DD6G2E5Q6RYAZ7NAERC7IL6A7Q.json","graph_json":"https://pith.science/api/pith-number/DD6G2E5Q6RYAZ7NAERC7IL6A7Q/graph.json","events_json":"https://pith.science/api/pith-number/DD6G2E5Q6RYAZ7NAERC7IL6A7Q/events.json","paper":"https://pith.science/paper/DD6G2E5Q"},"agent_actions":{"view_html":"https://pith.science/pith/DD6G2E5Q6RYAZ7NAERC7IL6A7Q","download_json":"https://pith.science/pith/DD6G2E5Q6RYAZ7NAERC7IL6A7Q.json","view_paper":"https://pith.science/paper/DD6G2E5Q","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1011.5140&json=true","fetch_graph":"https://pith.science/api/pith-number/DD6G2E5Q6RYAZ7NAERC7IL6A7Q/graph.json","fetch_events":"https://pith.science/api/pith-number/DD6G2E5Q6RYAZ7NAERC7IL6A7Q/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DD6G2E5Q6RYAZ7NAERC7IL6A7Q/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DD6G2E5Q6RYAZ7NAERC7IL6A7Q/action/storage_attestation","attest_author":"https://pith.science/pith/DD6G2E5Q6RYAZ7NAERC7IL6A7Q/action/author_attestation","sign_citation":"https://pith.science/pith/DD6G2E5Q6RYAZ7NAERC7IL6A7Q/action/citation_signature","submit_replication":"https://pith.science/pith/DD6G2E5Q6RYAZ7NAERC7IL6A7Q/action/replication_record"}},"created_at":"2026-05-18T02:23:23.868578+00:00","updated_at":"2026-05-18T02:23:23.868578+00:00"}