{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:HD3SKIL3HMBCPXBHKQRLBES2WU","short_pith_number":"pith:HD3SKIL3","schema_version":"1.0","canonical_sha256":"38f725217b3b0227dc275422b0925ab52e3048959f1b80ccf362d3bffacf3c7e","source":{"kind":"arxiv","id":"1509.01415","version":1},"attestation_state":"computed","paper":{"title":"Slope-Reversed Mott Transition in Multiorbital Systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Aaram J. Kim, Gun Sang Jeon, MooYoung Choi","submitted_at":"2015-09-04T11:49:09Z","abstract_excerpt":"We examine finite-temperature phase transitions in the two-orbital Hubbard model with different bandwidths by means of the dynamical mean-field theory combined with the continuous-time quantum Monte Carlo method. It is found that there emerges a peculiar slope-reversed first-order Mott transition between the orbital-selective Mott phase and the Mott insulator phase in the presence of Ising-type Hund's coupling. The origin of the slope-reversed phase transition is clarified by the analysis of the temperature dependence of the energy density. It turns out that the increase of Hund's coupling low"},"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":"1509.01415","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2015-09-04T11:49:09Z","cross_cats_sorted":[],"title_canon_sha256":"1ad2c56ffeee04b7bbe7e5d407898062d34238cb4f6de49ef19d64dc6b57fa2a","abstract_canon_sha256":"f71f80d279b5882c8d6aaa363c4a20438662e11807a12f538b9457f3be71b3aa"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:28:46.382050Z","signature_b64":"FrFkFXcGRGApLmyyd47ogbSj6WCOtxQ2WD06kV8SrMeHds/B5VXmWGKkcV8ytcQToF9VbsHha3pFhltzn1GwAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"38f725217b3b0227dc275422b0925ab52e3048959f1b80ccf362d3bffacf3c7e","last_reissued_at":"2026-05-18T01:28:46.381434Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:28:46.381434Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Slope-Reversed Mott Transition in Multiorbital Systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Aaram J. Kim, Gun Sang Jeon, MooYoung Choi","submitted_at":"2015-09-04T11:49:09Z","abstract_excerpt":"We examine finite-temperature phase transitions in the two-orbital Hubbard model with different bandwidths by means of the dynamical mean-field theory combined with the continuous-time quantum Monte Carlo method. It is found that there emerges a peculiar slope-reversed first-order Mott transition between the orbital-selective Mott phase and the Mott insulator phase in the presence of Ising-type Hund's coupling. The origin of the slope-reversed phase transition is clarified by the analysis of the temperature dependence of the energy density. It turns out that the increase of Hund's coupling low"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.01415","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":"1509.01415","created_at":"2026-05-18T01:28:46.381522+00:00"},{"alias_kind":"arxiv_version","alias_value":"1509.01415v1","created_at":"2026-05-18T01:28:46.381522+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.01415","created_at":"2026-05-18T01:28:46.381522+00:00"},{"alias_kind":"pith_short_12","alias_value":"HD3SKIL3HMBC","created_at":"2026-05-18T12:29:22.688609+00:00"},{"alias_kind":"pith_short_16","alias_value":"HD3SKIL3HMBCPXBH","created_at":"2026-05-18T12:29:22.688609+00:00"},{"alias_kind":"pith_short_8","alias_value":"HD3SKIL3","created_at":"2026-05-18T12:29:22.688609+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/HD3SKIL3HMBCPXBHKQRLBES2WU","json":"https://pith.science/pith/HD3SKIL3HMBCPXBHKQRLBES2WU.json","graph_json":"https://pith.science/api/pith-number/HD3SKIL3HMBCPXBHKQRLBES2WU/graph.json","events_json":"https://pith.science/api/pith-number/HD3SKIL3HMBCPXBHKQRLBES2WU/events.json","paper":"https://pith.science/paper/HD3SKIL3"},"agent_actions":{"view_html":"https://pith.science/pith/HD3SKIL3HMBCPXBHKQRLBES2WU","download_json":"https://pith.science/pith/HD3SKIL3HMBCPXBHKQRLBES2WU.json","view_paper":"https://pith.science/paper/HD3SKIL3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1509.01415&json=true","fetch_graph":"https://pith.science/api/pith-number/HD3SKIL3HMBCPXBHKQRLBES2WU/graph.json","fetch_events":"https://pith.science/api/pith-number/HD3SKIL3HMBCPXBHKQRLBES2WU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HD3SKIL3HMBCPXBHKQRLBES2WU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HD3SKIL3HMBCPXBHKQRLBES2WU/action/storage_attestation","attest_author":"https://pith.science/pith/HD3SKIL3HMBCPXBHKQRLBES2WU/action/author_attestation","sign_citation":"https://pith.science/pith/HD3SKIL3HMBCPXBHKQRLBES2WU/action/citation_signature","submit_replication":"https://pith.science/pith/HD3SKIL3HMBCPXBHKQRLBES2WU/action/replication_record"}},"created_at":"2026-05-18T01:28:46.381522+00:00","updated_at":"2026-05-18T01:28:46.381522+00:00"}