{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:ZQDCEBRNLM4XOVSPIBCEA6Q3IH","short_pith_number":"pith:ZQDCEBRN","schema_version":"1.0","canonical_sha256":"cc0622062d5b3977564f4044407a1b41e44144654911deebd077bfee87218270","source":{"kind":"arxiv","id":"1503.00589","version":2},"attestation_state":"computed","paper":{"title":"Frustrated mixed spin-1/2 and spin-1 Ising ferrimagnets on a triangular lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"A. Bob\\'ak, M. \\v{Z}ukovi\\v{c}","submitted_at":"2015-03-02T16:12:52Z","abstract_excerpt":"Mixed spin-1/2 and spin-1 Ising ferrimagnets on a triangular lattice with sublattices A, B and C are studied for two spin value distributions $(S_{\\rm A},S_{\\rm B},S_{\\rm C})=(1/2,1/2,1)$ and $(1/2,1,1)$ by Monte Carlo simulations. The non-bipartite character of the lattice induces geometrical frustration in both systems, which leads to the critical behavior rather different from their ferromagnetic counterparts. We confirm second-order phase transitions belonging to the standard Ising universality class occurring at higher temperatures, however, in both models these change at tricritical poin"},"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":"1503.00589","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2015-03-02T16:12:52Z","cross_cats_sorted":[],"title_canon_sha256":"e34076dfe65312facd3738f21802060ebfa5cbbf196f4f92ac5cd2d1412b8eb3","abstract_canon_sha256":"9ef51c90cfc8c13f300e8eea39d804a255e6fa3388e26ca6861b090b082052fc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:59:57.675123Z","signature_b64":"8RllczK9AbXuMZ2ltB6jAd4lCHiu5n3g/pFw+SncZJGbvTY2UkumBds3GHgYS3hKbmrdnz5fd7yIlJxKK8DICA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cc0622062d5b3977564f4044407a1b41e44144654911deebd077bfee87218270","last_reissued_at":"2026-05-18T01:59:57.674594Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:59:57.674594Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Frustrated mixed spin-1/2 and spin-1 Ising ferrimagnets on a triangular lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"A. Bob\\'ak, M. \\v{Z}ukovi\\v{c}","submitted_at":"2015-03-02T16:12:52Z","abstract_excerpt":"Mixed spin-1/2 and spin-1 Ising ferrimagnets on a triangular lattice with sublattices A, B and C are studied for two spin value distributions $(S_{\\rm A},S_{\\rm B},S_{\\rm C})=(1/2,1/2,1)$ and $(1/2,1,1)$ by Monte Carlo simulations. The non-bipartite character of the lattice induces geometrical frustration in both systems, which leads to the critical behavior rather different from their ferromagnetic counterparts. We confirm second-order phase transitions belonging to the standard Ising universality class occurring at higher temperatures, however, in both models these change at tricritical poin"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1503.00589","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":"1503.00589","created_at":"2026-05-18T01:59:57.674666+00:00"},{"alias_kind":"arxiv_version","alias_value":"1503.00589v2","created_at":"2026-05-18T01:59:57.674666+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1503.00589","created_at":"2026-05-18T01:59:57.674666+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZQDCEBRNLM4X","created_at":"2026-05-18T12:29:52.810259+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZQDCEBRNLM4XOVSP","created_at":"2026-05-18T12:29:52.810259+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZQDCEBRN","created_at":"2026-05-18T12:29:52.810259+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/ZQDCEBRNLM4XOVSPIBCEA6Q3IH","json":"https://pith.science/pith/ZQDCEBRNLM4XOVSPIBCEA6Q3IH.json","graph_json":"https://pith.science/api/pith-number/ZQDCEBRNLM4XOVSPIBCEA6Q3IH/graph.json","events_json":"https://pith.science/api/pith-number/ZQDCEBRNLM4XOVSPIBCEA6Q3IH/events.json","paper":"https://pith.science/paper/ZQDCEBRN"},"agent_actions":{"view_html":"https://pith.science/pith/ZQDCEBRNLM4XOVSPIBCEA6Q3IH","download_json":"https://pith.science/pith/ZQDCEBRNLM4XOVSPIBCEA6Q3IH.json","view_paper":"https://pith.science/paper/ZQDCEBRN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1503.00589&json=true","fetch_graph":"https://pith.science/api/pith-number/ZQDCEBRNLM4XOVSPIBCEA6Q3IH/graph.json","fetch_events":"https://pith.science/api/pith-number/ZQDCEBRNLM4XOVSPIBCEA6Q3IH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZQDCEBRNLM4XOVSPIBCEA6Q3IH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZQDCEBRNLM4XOVSPIBCEA6Q3IH/action/storage_attestation","attest_author":"https://pith.science/pith/ZQDCEBRNLM4XOVSPIBCEA6Q3IH/action/author_attestation","sign_citation":"https://pith.science/pith/ZQDCEBRNLM4XOVSPIBCEA6Q3IH/action/citation_signature","submit_replication":"https://pith.science/pith/ZQDCEBRNLM4XOVSPIBCEA6Q3IH/action/replication_record"}},"created_at":"2026-05-18T01:59:57.674666+00:00","updated_at":"2026-05-18T01:59:57.674666+00:00"}