{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:OHIF5GAOSGWWN55M3EIROQUZPF","short_pith_number":"pith:OHIF5GAO","canonical_record":{"source":{"id":"1004.1164","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2010-04-07T19:38:26Z","cross_cats_sorted":[],"title_canon_sha256":"970cf1db2d6cd9a7fc1e4a7254936013cc4ccf6195b1ed12b20df680c0bd5863","abstract_canon_sha256":"d81ec04a04641fbfcffc095b1bd0eed22419f8fba0707d0cc7502588cd5398f5"},"schema_version":"1.0"},"canonical_sha256":"71d05e980e91ad66f7acd9111742997970a96548080c082e92d33760a30ff43e","source":{"kind":"arxiv","id":"1004.1164","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1004.1164","created_at":"2026-05-18T02:24:17Z"},{"alias_kind":"arxiv_version","alias_value":"1004.1164v3","created_at":"2026-05-18T02:24:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1004.1164","created_at":"2026-05-18T02:24:17Z"},{"alias_kind":"pith_short_12","alias_value":"OHIF5GAOSGWW","created_at":"2026-05-18T12:26:12Z"},{"alias_kind":"pith_short_16","alias_value":"OHIF5GAOSGWWN55M","created_at":"2026-05-18T12:26:12Z"},{"alias_kind":"pith_short_8","alias_value":"OHIF5GAO","created_at":"2026-05-18T12:26:12Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:OHIF5GAOSGWWN55M3EIROQUZPF","target":"record","payload":{"canonical_record":{"source":{"id":"1004.1164","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2010-04-07T19:38:26Z","cross_cats_sorted":[],"title_canon_sha256":"970cf1db2d6cd9a7fc1e4a7254936013cc4ccf6195b1ed12b20df680c0bd5863","abstract_canon_sha256":"d81ec04a04641fbfcffc095b1bd0eed22419f8fba0707d0cc7502588cd5398f5"},"schema_version":"1.0"},"canonical_sha256":"71d05e980e91ad66f7acd9111742997970a96548080c082e92d33760a30ff43e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:24:17.010413Z","signature_b64":"nBpVjlcGuNIsWkxaWyjDx846UhAnKtQDQmvpNnnjKLVZA86x7HsyHp0sbIxtIaDlz+fpKGn2zwsMMXWhjgs8Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"71d05e980e91ad66f7acd9111742997970a96548080c082e92d33760a30ff43e","last_reissued_at":"2026-05-18T02:24:17.009605Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:24:17.009605Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1004.1164","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:24:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xuqroUnKMUyoO8+MFW0pzABkVPcpbs/woiS00rqtmB/H21iBNPBju1vSln3yCBouyPUVidm9nt8bVvEM50mUDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T19:19:14.591959Z"},"content_sha256":"95e073f65cd146c23a5ea34fb9c131394acf9f0413eb325f2b24b26cddc827e5","schema_version":"1.0","event_id":"sha256:95e073f65cd146c23a5ea34fb9c131394acf9f0413eb325f2b24b26cddc827e5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:OHIF5GAOSGWWN55M3EIROQUZPF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quantum criticality and correlations in the cuprate superconductors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"J. M. P. Carmelo","submitted_at":"2010-04-07T19:38:26Z","abstract_excerpt":"A description of the electronic correlations contained in the Hubbard model on the square-lattice perturbed by very weak three-dimensional uniaxial anisotropy in terms of the residual interactions of charge $c$ fermions and spin-neutral composite two-spinon $s1$ fermions is used to access further information on the origin of quantum critical behavior in the hole-doped cuprate superconductors. Excellent quantitative agreement with their anisotropic linear-$\\omega$ one-electron scattering rate and normal-state linear-$T$ resistivity is achieved. Our results provide strong evidence that the norma"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1004.1164","kind":"arxiv","version":3},"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":"2026-05-18T02:24:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Rny/aDS8PRNEykHYbw0XKcjnpZF7VfZaEhVJFn6+zqrY7+pqnisG6cnNevViikYED4CyMpYGk/i+XulUT9ThDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T19:19:14.592302Z"},"content_sha256":"04fdabe78bd75480805ee00a50fc440adb48b63f2aecba44e59db24abfa251c1","schema_version":"1.0","event_id":"sha256:04fdabe78bd75480805ee00a50fc440adb48b63f2aecba44e59db24abfa251c1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/OHIF5GAOSGWWN55M3EIROQUZPF/bundle.json","state_url":"https://pith.science/pith/OHIF5GAOSGWWN55M3EIROQUZPF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/OHIF5GAOSGWWN55M3EIROQUZPF/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":"2026-06-24T19:19:14Z","links":{"resolver":"https://pith.science/pith/OHIF5GAOSGWWN55M3EIROQUZPF","bundle":"https://pith.science/pith/OHIF5GAOSGWWN55M3EIROQUZPF/bundle.json","state":"https://pith.science/pith/OHIF5GAOSGWWN55M3EIROQUZPF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/OHIF5GAOSGWWN55M3EIROQUZPF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:OHIF5GAOSGWWN55M3EIROQUZPF","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":"d81ec04a04641fbfcffc095b1bd0eed22419f8fba0707d0cc7502588cd5398f5","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2010-04-07T19:38:26Z","title_canon_sha256":"970cf1db2d6cd9a7fc1e4a7254936013cc4ccf6195b1ed12b20df680c0bd5863"},"schema_version":"1.0","source":{"id":"1004.1164","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1004.1164","created_at":"2026-05-18T02:24:17Z"},{"alias_kind":"arxiv_version","alias_value":"1004.1164v3","created_at":"2026-05-18T02:24:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1004.1164","created_at":"2026-05-18T02:24:17Z"},{"alias_kind":"pith_short_12","alias_value":"OHIF5GAOSGWW","created_at":"2026-05-18T12:26:12Z"},{"alias_kind":"pith_short_16","alias_value":"OHIF5GAOSGWWN55M","created_at":"2026-05-18T12:26:12Z"},{"alias_kind":"pith_short_8","alias_value":"OHIF5GAO","created_at":"2026-05-18T12:26:12Z"}],"graph_snapshots":[{"event_id":"sha256:04fdabe78bd75480805ee00a50fc440adb48b63f2aecba44e59db24abfa251c1","target":"graph","created_at":"2026-05-18T02:24:17Z","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":"A description of the electronic correlations contained in the Hubbard model on the square-lattice perturbed by very weak three-dimensional uniaxial anisotropy in terms of the residual interactions of charge $c$ fermions and spin-neutral composite two-spinon $s1$ fermions is used to access further information on the origin of quantum critical behavior in the hole-doped cuprate superconductors. Excellent quantitative agreement with their anisotropic linear-$\\omega$ one-electron scattering rate and normal-state linear-$T$ resistivity is achieved. Our results provide strong evidence that the norma","authors_text":"J. M. P. Carmelo","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2010-04-07T19:38:26Z","title":"Quantum criticality and correlations in the cuprate superconductors"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1004.1164","kind":"arxiv","version":3},"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":"sha256:95e073f65cd146c23a5ea34fb9c131394acf9f0413eb325f2b24b26cddc827e5","target":"record","created_at":"2026-05-18T02:24:17Z","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":"d81ec04a04641fbfcffc095b1bd0eed22419f8fba0707d0cc7502588cd5398f5","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2010-04-07T19:38:26Z","title_canon_sha256":"970cf1db2d6cd9a7fc1e4a7254936013cc4ccf6195b1ed12b20df680c0bd5863"},"schema_version":"1.0","source":{"id":"1004.1164","kind":"arxiv","version":3}},"canonical_sha256":"71d05e980e91ad66f7acd9111742997970a96548080c082e92d33760a30ff43e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"71d05e980e91ad66f7acd9111742997970a96548080c082e92d33760a30ff43e","first_computed_at":"2026-05-18T02:24:17.009605Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:24:17.009605Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"nBpVjlcGuNIsWkxaWyjDx846UhAnKtQDQmvpNnnjKLVZA86x7HsyHp0sbIxtIaDlz+fpKGn2zwsMMXWhjgs8Bg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:24:17.010413Z","signed_message":"canonical_sha256_bytes"},"source_id":"1004.1164","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:95e073f65cd146c23a5ea34fb9c131394acf9f0413eb325f2b24b26cddc827e5","sha256:04fdabe78bd75480805ee00a50fc440adb48b63f2aecba44e59db24abfa251c1"],"state_sha256":"45fd3bb72a3510d0d3b680bf72c709d514ae54e92b94108850d1382d65af6e4c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UJ+2h0aMSE6jUUZmcqtEWyBhPlGJNz7aDoonj4ETRg1c2ZTyQrGNJ1KTTNWRPckCWWEKE6JkijWSwIK9DxFXCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-24T19:19:14.594223Z","bundle_sha256":"50985435908b21adf0c665dd835e78108dd23bb78067dd21e168ef2008888c4d"}}