{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:37D6AWCZ3PYNXAS24TIQNWBJNC","short_pith_number":"pith:37D6AWCZ","schema_version":"1.0","canonical_sha256":"dfc7e05859dbf0db825ae4d106d82968b43100afdd2326e87aad9f6972898d1c","source":{"kind":"arxiv","id":"1404.2039","version":2},"attestation_state":"computed","paper":{"title":"Depletion force in the infinite-dilution limit in a solvent of nonadditive hard spheres","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","physics.chem-ph"],"primary_cat":"cond-mat.soft","authors_text":"Andr\\'es Santos, Riccardo Fantoni","submitted_at":"2014-04-08T08:35:06Z","abstract_excerpt":"The mutual entropic depletion force felt by two solute \"big\" hard spheres immersed in a binary mixture solvent of nonadditive \"small\" hard spheres is calculated as a function of the surface-to-surface distance by means of canonical Monte Carlo simulations and through a recently proposed rational-function approximation [Phys. Rev. E \\textbf{84}, 041201 (2011)]. Four representative scenarios are investigated: symmetric solute particles and the limit where one of the two solute spheres becomes a planar hard wall, in both cases with symmetric and asymmetric solvents. In all cases, the influence on"},"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":"1404.2039","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2014-04-08T08:35:06Z","cross_cats_sorted":["cond-mat.stat-mech","physics.chem-ph"],"title_canon_sha256":"16b5841ccd7fe9aef3f0ceea0c87d125c8f24caa664a51c32bac38dc78a94d6e","abstract_canon_sha256":"686c038106269355cbfff4bbadbcddbc0295f6fc1a94e4919bae220317860062"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:48:36.426722Z","signature_b64":"MEvdCKyq19opaQ4isF3ed7809OUOupXMYk76sJsAmU981vIBcCVPhAUS6mMdzAk9qkXb9cRR9qSPaeGzTlwiAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dfc7e05859dbf0db825ae4d106d82968b43100afdd2326e87aad9f6972898d1c","last_reissued_at":"2026-05-18T02:48:36.426211Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:48:36.426211Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Depletion force in the infinite-dilution limit in a solvent of nonadditive hard spheres","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","physics.chem-ph"],"primary_cat":"cond-mat.soft","authors_text":"Andr\\'es Santos, Riccardo Fantoni","submitted_at":"2014-04-08T08:35:06Z","abstract_excerpt":"The mutual entropic depletion force felt by two solute \"big\" hard spheres immersed in a binary mixture solvent of nonadditive \"small\" hard spheres is calculated as a function of the surface-to-surface distance by means of canonical Monte Carlo simulations and through a recently proposed rational-function approximation [Phys. Rev. E \\textbf{84}, 041201 (2011)]. Four representative scenarios are investigated: symmetric solute particles and the limit where one of the two solute spheres becomes a planar hard wall, in both cases with symmetric and asymmetric solvents. In all cases, the influence on"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.2039","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1404.2039","created_at":"2026-05-18T02:48:36.426281+00:00"},{"alias_kind":"arxiv_version","alias_value":"1404.2039v2","created_at":"2026-05-18T02:48:36.426281+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.2039","created_at":"2026-05-18T02:48:36.426281+00:00"},{"alias_kind":"pith_short_12","alias_value":"37D6AWCZ3PYN","created_at":"2026-05-18T12:28:11.866339+00:00"},{"alias_kind":"pith_short_16","alias_value":"37D6AWCZ3PYNXAS2","created_at":"2026-05-18T12:28:11.866339+00:00"},{"alias_kind":"pith_short_8","alias_value":"37D6AWCZ","created_at":"2026-05-18T12:28:11.866339+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/37D6AWCZ3PYNXAS24TIQNWBJNC","json":"https://pith.science/pith/37D6AWCZ3PYNXAS24TIQNWBJNC.json","graph_json":"https://pith.science/api/pith-number/37D6AWCZ3PYNXAS24TIQNWBJNC/graph.json","events_json":"https://pith.science/api/pith-number/37D6AWCZ3PYNXAS24TIQNWBJNC/events.json","paper":"https://pith.science/paper/37D6AWCZ"},"agent_actions":{"view_html":"https://pith.science/pith/37D6AWCZ3PYNXAS24TIQNWBJNC","download_json":"https://pith.science/pith/37D6AWCZ3PYNXAS24TIQNWBJNC.json","view_paper":"https://pith.science/paper/37D6AWCZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1404.2039&json=true","fetch_graph":"https://pith.science/api/pith-number/37D6AWCZ3PYNXAS24TIQNWBJNC/graph.json","fetch_events":"https://pith.science/api/pith-number/37D6AWCZ3PYNXAS24TIQNWBJNC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/37D6AWCZ3PYNXAS24TIQNWBJNC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/37D6AWCZ3PYNXAS24TIQNWBJNC/action/storage_attestation","attest_author":"https://pith.science/pith/37D6AWCZ3PYNXAS24TIQNWBJNC/action/author_attestation","sign_citation":"https://pith.science/pith/37D6AWCZ3PYNXAS24TIQNWBJNC/action/citation_signature","submit_replication":"https://pith.science/pith/37D6AWCZ3PYNXAS24TIQNWBJNC/action/replication_record"}},"created_at":"2026-05-18T02:48:36.426281+00:00","updated_at":"2026-05-18T02:48:36.426281+00:00"}