{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:7NTO5P7LVSCTQLVFCYARBPJWQB","short_pith_number":"pith:7NTO5P7L","canonical_record":{"source":{"id":"1209.4349","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2012-09-19T19:56:30Z","cross_cats_sorted":[],"title_canon_sha256":"8d4b86cd54298bdbbd80db111fc4bd385c79aea19abc028d6646d7e8a7e3e89e","abstract_canon_sha256":"8671634eb7268948d01b91e6a4387566ec18655ba4fc0c4168954d913c0ca097"},"schema_version":"1.0"},"canonical_sha256":"fb66eebfebac85382ea5160110bd3680462cec3dd5582f1e671de57b694114e7","source":{"kind":"arxiv","id":"1209.4349","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1209.4349","created_at":"2026-05-18T03:10:14Z"},{"alias_kind":"arxiv_version","alias_value":"1209.4349v2","created_at":"2026-05-18T03:10:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1209.4349","created_at":"2026-05-18T03:10:14Z"},{"alias_kind":"pith_short_12","alias_value":"7NTO5P7LVSCT","created_at":"2026-05-18T12:26:58Z"},{"alias_kind":"pith_short_16","alias_value":"7NTO5P7LVSCTQLVF","created_at":"2026-05-18T12:26:58Z"},{"alias_kind":"pith_short_8","alias_value":"7NTO5P7L","created_at":"2026-05-18T12:26:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:7NTO5P7LVSCTQLVFCYARBPJWQB","target":"record","payload":{"canonical_record":{"source":{"id":"1209.4349","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2012-09-19T19:56:30Z","cross_cats_sorted":[],"title_canon_sha256":"8d4b86cd54298bdbbd80db111fc4bd385c79aea19abc028d6646d7e8a7e3e89e","abstract_canon_sha256":"8671634eb7268948d01b91e6a4387566ec18655ba4fc0c4168954d913c0ca097"},"schema_version":"1.0"},"canonical_sha256":"fb66eebfebac85382ea5160110bd3680462cec3dd5582f1e671de57b694114e7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:10:14.539808Z","signature_b64":"0Hf4kYmbG+AiqkHOz1PTzKIBEbR7nbeCG87aQXN3It9JZJFU99EnERUSsp7Z8mx/X1XPDRT69APoF4DFMdp8BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fb66eebfebac85382ea5160110bd3680462cec3dd5582f1e671de57b694114e7","last_reissued_at":"2026-05-18T03:10:14.539155Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:10:14.539155Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1209.4349","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:10:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yOh8sPQn76uebrzD59FdLH25tIDNgGs1VuUlhpai3sAs0aQR7PPS7PnzrOioH7WKl1UAciTslQ72EWeb7lnqCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T02:37:35.802947Z"},"content_sha256":"c6e51c8b9107038097a99bb230428e0431cee9af2b50224a6b66a83adac44b43","schema_version":"1.0","event_id":"sha256:c6e51c8b9107038097a99bb230428e0431cee9af2b50224a6b66a83adac44b43"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:7NTO5P7LVSCTQLVFCYARBPJWQB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Entropy, frustration and large thermopower of doped Mott insulators on the fcc lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A.-M. S. Tremblay, B. Sriram Shastry, Louis-Fran\\c{c}ois Arsenault, Patrick S\\'emon","submitted_at":"2012-09-19T19:56:30Z","abstract_excerpt":"Electronic frustration and strong correlations may lead to large Seebeck coefficients. To understand this physics on general grounds, we compute the thermopower of the one-band Hubbard model on the 3-dimensional fcc lattice over the whole range of fillings for intermediate and large interaction strength. Dynamical mean-field theory shows that when the density approaches half-filling, the fcc lattice at strong coupling exhibits a large low temperature Seebeck coefficient $S$. The largest effect occurs as one approaches $n=1$ from dopings where electronic frustration is maximized. The high-frequ"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1209.4349","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:10:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HEzS+2JQSRfJS1kpFGrAdhzUuDxASqsfFYJjwNLPpDgKza7o6t7hLSBDiUlA5kVZToMy13kwMX2wvAk9j9OaAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T02:37:35.803308Z"},"content_sha256":"301346778629338053b76aeb399aaec1d0ec6e1a04e19ee1530664bb6f0f16de","schema_version":"1.0","event_id":"sha256:301346778629338053b76aeb399aaec1d0ec6e1a04e19ee1530664bb6f0f16de"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/7NTO5P7LVSCTQLVFCYARBPJWQB/bundle.json","state_url":"https://pith.science/pith/7NTO5P7LVSCTQLVFCYARBPJWQB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/7NTO5P7LVSCTQLVFCYARBPJWQB/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-30T02:37:35Z","links":{"resolver":"https://pith.science/pith/7NTO5P7LVSCTQLVFCYARBPJWQB","bundle":"https://pith.science/pith/7NTO5P7LVSCTQLVFCYARBPJWQB/bundle.json","state":"https://pith.science/pith/7NTO5P7LVSCTQLVFCYARBPJWQB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/7NTO5P7LVSCTQLVFCYARBPJWQB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:7NTO5P7LVSCTQLVFCYARBPJWQB","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"8671634eb7268948d01b91e6a4387566ec18655ba4fc0c4168954d913c0ca097","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2012-09-19T19:56:30Z","title_canon_sha256":"8d4b86cd54298bdbbd80db111fc4bd385c79aea19abc028d6646d7e8a7e3e89e"},"schema_version":"1.0","source":{"id":"1209.4349","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1209.4349","created_at":"2026-05-18T03:10:14Z"},{"alias_kind":"arxiv_version","alias_value":"1209.4349v2","created_at":"2026-05-18T03:10:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1209.4349","created_at":"2026-05-18T03:10:14Z"},{"alias_kind":"pith_short_12","alias_value":"7NTO5P7LVSCT","created_at":"2026-05-18T12:26:58Z"},{"alias_kind":"pith_short_16","alias_value":"7NTO5P7LVSCTQLVF","created_at":"2026-05-18T12:26:58Z"},{"alias_kind":"pith_short_8","alias_value":"7NTO5P7L","created_at":"2026-05-18T12:26:58Z"}],"graph_snapshots":[{"event_id":"sha256:301346778629338053b76aeb399aaec1d0ec6e1a04e19ee1530664bb6f0f16de","target":"graph","created_at":"2026-05-18T03:10:14Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"Electronic frustration and strong correlations may lead to large Seebeck coefficients. To understand this physics on general grounds, we compute the thermopower of the one-band Hubbard model on the 3-dimensional fcc lattice over the whole range of fillings for intermediate and large interaction strength. Dynamical mean-field theory shows that when the density approaches half-filling, the fcc lattice at strong coupling exhibits a large low temperature Seebeck coefficient $S$. The largest effect occurs as one approaches $n=1$ from dopings where electronic frustration is maximized. The high-frequ","authors_text":"A.-M. S. Tremblay, B. Sriram Shastry, Louis-Fran\\c{c}ois Arsenault, Patrick S\\'emon","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2012-09-19T19:56:30Z","title":"Entropy, frustration and large thermopower of doped Mott insulators on the fcc lattice"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1209.4349","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:c6e51c8b9107038097a99bb230428e0431cee9af2b50224a6b66a83adac44b43","target":"record","created_at":"2026-05-18T03:10:14Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"8671634eb7268948d01b91e6a4387566ec18655ba4fc0c4168954d913c0ca097","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2012-09-19T19:56:30Z","title_canon_sha256":"8d4b86cd54298bdbbd80db111fc4bd385c79aea19abc028d6646d7e8a7e3e89e"},"schema_version":"1.0","source":{"id":"1209.4349","kind":"arxiv","version":2}},"canonical_sha256":"fb66eebfebac85382ea5160110bd3680462cec3dd5582f1e671de57b694114e7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"fb66eebfebac85382ea5160110bd3680462cec3dd5582f1e671de57b694114e7","first_computed_at":"2026-05-18T03:10:14.539155Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:10:14.539155Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"0Hf4kYmbG+AiqkHOz1PTzKIBEbR7nbeCG87aQXN3It9JZJFU99EnERUSsp7Z8mx/X1XPDRT69APoF4DFMdp8BA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:10:14.539808Z","signed_message":"canonical_sha256_bytes"},"source_id":"1209.4349","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c6e51c8b9107038097a99bb230428e0431cee9af2b50224a6b66a83adac44b43","sha256:301346778629338053b76aeb399aaec1d0ec6e1a04e19ee1530664bb6f0f16de"],"state_sha256":"830d46fd5de4384185011bcf18ec04d0195b0147b242214bd9ada900af45dddd"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+hkLwL9NxRtkhncCltOF4FihH0sMExgREebToPlRmc6o6DR6epRJ1iuczlj9p4BeRfqIkyNJlLjZA3gBetKnBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T02:37:35.805759Z","bundle_sha256":"8a9e98bee26afad3164de587c5ce0f550c2a3228ab3b6a00b8e49c575eaf1052"}}