{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:OK6G4JA2RPT7ATKH67BRII4IC7","short_pith_number":"pith:OK6G4JA2","schema_version":"1.0","canonical_sha256":"72bc6e241a8be7f04d47f7c314238817e1d991dff09345dc3a84497ad982e484","source":{"kind":"arxiv","id":"1705.00262","version":1},"attestation_state":"computed","paper":{"title":"Condensation of Lee-Yang zeros in scalar field theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"hep-th","authors_text":"C.E.Tsagkarakis, F.K.Diakonos, N.G.Antoniou, X.N.Maintas","submitted_at":"2017-04-30T01:51:01Z","abstract_excerpt":"We show that, at the critical temperature, there is a class of Lee-Yang zeros of the partition function in a general scalar field theory, which location scales with the size of the system with a characteristic exponent expressed in terms of the isothermal critical exponent $\\delta$. In the thermodynamic limit the zeros belonging to this class condense to the critical point {\\zeta}=1 on the real axis in the complex fugacity plane while the complementary set of zeros (with Re {\\zeta} < 1) covers uniformly the unit circle. Although the aforementioned class degenerates to a single point for an inf"},"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":"1705.00262","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-04-30T01:51:01Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"9028b39efb6f4d410a8beced5c1f4714805fa23cb928f501b2c2719049772869","abstract_canon_sha256":"910c6473d210a6b4b701fc3a1f2dfae82a734fda1d1d6ff68f68406c87970820"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:42:52.216943Z","signature_b64":"jzoV2EBQY4nTfWXSMuvD+kUjjKR5OzbFe1LJSHFisbGTIdHoUFUiFtS8TsrYJIZPDjzykmyxKbEQ9uvVoKvyAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"72bc6e241a8be7f04d47f7c314238817e1d991dff09345dc3a84497ad982e484","last_reissued_at":"2026-05-18T00:42:52.216190Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:42:52.216190Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Condensation of Lee-Yang zeros in scalar field theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"hep-th","authors_text":"C.E.Tsagkarakis, F.K.Diakonos, N.G.Antoniou, X.N.Maintas","submitted_at":"2017-04-30T01:51:01Z","abstract_excerpt":"We show that, at the critical temperature, there is a class of Lee-Yang zeros of the partition function in a general scalar field theory, which location scales with the size of the system with a characteristic exponent expressed in terms of the isothermal critical exponent $\\delta$. In the thermodynamic limit the zeros belonging to this class condense to the critical point {\\zeta}=1 on the real axis in the complex fugacity plane while the complementary set of zeros (with Re {\\zeta} < 1) covers uniformly the unit circle. Although the aforementioned class degenerates to a single point for an inf"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.00262","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":"1705.00262","created_at":"2026-05-18T00:42:52.216292+00:00"},{"alias_kind":"arxiv_version","alias_value":"1705.00262v1","created_at":"2026-05-18T00:42:52.216292+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.00262","created_at":"2026-05-18T00:42:52.216292+00:00"},{"alias_kind":"pith_short_12","alias_value":"OK6G4JA2RPT7","created_at":"2026-05-18T12:31:34.259226+00:00"},{"alias_kind":"pith_short_16","alias_value":"OK6G4JA2RPT7ATKH","created_at":"2026-05-18T12:31:34.259226+00:00"},{"alias_kind":"pith_short_8","alias_value":"OK6G4JA2","created_at":"2026-05-18T12:31:34.259226+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/OK6G4JA2RPT7ATKH67BRII4IC7","json":"https://pith.science/pith/OK6G4JA2RPT7ATKH67BRII4IC7.json","graph_json":"https://pith.science/api/pith-number/OK6G4JA2RPT7ATKH67BRII4IC7/graph.json","events_json":"https://pith.science/api/pith-number/OK6G4JA2RPT7ATKH67BRII4IC7/events.json","paper":"https://pith.science/paper/OK6G4JA2"},"agent_actions":{"view_html":"https://pith.science/pith/OK6G4JA2RPT7ATKH67BRII4IC7","download_json":"https://pith.science/pith/OK6G4JA2RPT7ATKH67BRII4IC7.json","view_paper":"https://pith.science/paper/OK6G4JA2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1705.00262&json=true","fetch_graph":"https://pith.science/api/pith-number/OK6G4JA2RPT7ATKH67BRII4IC7/graph.json","fetch_events":"https://pith.science/api/pith-number/OK6G4JA2RPT7ATKH67BRII4IC7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OK6G4JA2RPT7ATKH67BRII4IC7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OK6G4JA2RPT7ATKH67BRII4IC7/action/storage_attestation","attest_author":"https://pith.science/pith/OK6G4JA2RPT7ATKH67BRII4IC7/action/author_attestation","sign_citation":"https://pith.science/pith/OK6G4JA2RPT7ATKH67BRII4IC7/action/citation_signature","submit_replication":"https://pith.science/pith/OK6G4JA2RPT7ATKH67BRII4IC7/action/replication_record"}},"created_at":"2026-05-18T00:42:52.216292+00:00","updated_at":"2026-05-18T00:42:52.216292+00:00"}