{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:RZ3HZ7PRKFB5VHE3PNA7VJYMXO","short_pith_number":"pith:RZ3HZ7PR","schema_version":"1.0","canonical_sha256":"8e767cfdf15143da9c9b7b41faa70cbb918432562f8629c80c95698285eeb75b","source":{"kind":"arxiv","id":"1303.4236","version":1},"attestation_state":"computed","paper":{"title":"Thermodynamics of two-component log-gases with alternating charges","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Ladislav Samaj","submitted_at":"2013-03-18T13:03:30Z","abstract_excerpt":"We consider a one-dimensional gas of positive and negative unit charges interacting via a logarithmic potential, which is in thermal equilibrium at the (dimensionless) inverse temperature $\\beta$. In a previous paper [Samaj, L.: J. Stat. Phys. 105, 173-191 (2001)], the exact thermodynamics of the unrestricted log-gas of pointlike charges was obtained using an equivalence with a (1+1)-dimensional boundary sine-Gordon model. The present aim is to extend the exact study of the thermodynamics to the log-gas on a line with alternating $\\pm$ charges. The formula for the ordered grand partition funct"},"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":"1303.4236","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2013-03-18T13:03:30Z","cross_cats_sorted":[],"title_canon_sha256":"3bdc63a822c12b3f9789b1f4229345f554ec47ab1d847cc5b455e384b1fbdf2d","abstract_canon_sha256":"fad986ce289586d19fc37b1177f50684b90e78205e92c513dbd7f088a4d73a53"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:11:09.332661Z","signature_b64":"yeJPNLXI5XUGT7NgTbZPCOoZwkhTp9yvogVc0YpgMZII2+raZppcarYc28kZ6Nw66rGDwJFtEVZ/MivNPjWVCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8e767cfdf15143da9c9b7b41faa70cbb918432562f8629c80c95698285eeb75b","last_reissued_at":"2026-05-18T03:11:09.331750Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:11:09.331750Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Thermodynamics of two-component log-gases with alternating charges","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Ladislav Samaj","submitted_at":"2013-03-18T13:03:30Z","abstract_excerpt":"We consider a one-dimensional gas of positive and negative unit charges interacting via a logarithmic potential, which is in thermal equilibrium at the (dimensionless) inverse temperature $\\beta$. In a previous paper [Samaj, L.: J. Stat. Phys. 105, 173-191 (2001)], the exact thermodynamics of the unrestricted log-gas of pointlike charges was obtained using an equivalence with a (1+1)-dimensional boundary sine-Gordon model. The present aim is to extend the exact study of the thermodynamics to the log-gas on a line with alternating $\\pm$ charges. The formula for the ordered grand partition funct"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.4236","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":""},"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":"1303.4236","created_at":"2026-05-18T03:11:09.331907+00:00"},{"alias_kind":"arxiv_version","alias_value":"1303.4236v1","created_at":"2026-05-18T03:11:09.331907+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.4236","created_at":"2026-05-18T03:11:09.331907+00:00"},{"alias_kind":"pith_short_12","alias_value":"RZ3HZ7PRKFB5","created_at":"2026-05-18T12:27:59.945178+00:00"},{"alias_kind":"pith_short_16","alias_value":"RZ3HZ7PRKFB5VHE3","created_at":"2026-05-18T12:27:59.945178+00:00"},{"alias_kind":"pith_short_8","alias_value":"RZ3HZ7PR","created_at":"2026-05-18T12:27:59.945178+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/RZ3HZ7PRKFB5VHE3PNA7VJYMXO","json":"https://pith.science/pith/RZ3HZ7PRKFB5VHE3PNA7VJYMXO.json","graph_json":"https://pith.science/api/pith-number/RZ3HZ7PRKFB5VHE3PNA7VJYMXO/graph.json","events_json":"https://pith.science/api/pith-number/RZ3HZ7PRKFB5VHE3PNA7VJYMXO/events.json","paper":"https://pith.science/paper/RZ3HZ7PR"},"agent_actions":{"view_html":"https://pith.science/pith/RZ3HZ7PRKFB5VHE3PNA7VJYMXO","download_json":"https://pith.science/pith/RZ3HZ7PRKFB5VHE3PNA7VJYMXO.json","view_paper":"https://pith.science/paper/RZ3HZ7PR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1303.4236&json=true","fetch_graph":"https://pith.science/api/pith-number/RZ3HZ7PRKFB5VHE3PNA7VJYMXO/graph.json","fetch_events":"https://pith.science/api/pith-number/RZ3HZ7PRKFB5VHE3PNA7VJYMXO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RZ3HZ7PRKFB5VHE3PNA7VJYMXO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RZ3HZ7PRKFB5VHE3PNA7VJYMXO/action/storage_attestation","attest_author":"https://pith.science/pith/RZ3HZ7PRKFB5VHE3PNA7VJYMXO/action/author_attestation","sign_citation":"https://pith.science/pith/RZ3HZ7PRKFB5VHE3PNA7VJYMXO/action/citation_signature","submit_replication":"https://pith.science/pith/RZ3HZ7PRKFB5VHE3PNA7VJYMXO/action/replication_record"}},"created_at":"2026-05-18T03:11:09.331907+00:00","updated_at":"2026-05-18T03:11:09.331907+00:00"}