{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:EBE4RAS4VFT3MZ65E2J735KYFM","short_pith_number":"pith:EBE4RAS4","canonical_record":{"source":{"id":"1703.06280","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-03-18T10:25:58Z","cross_cats_sorted":["cond-mat.supr-con"],"title_canon_sha256":"be172b377cbff20aa2a197eeee2defa8c2a593cdd9e533c39ef66106d0a0cb45","abstract_canon_sha256":"7a5f34c24b4696aca1e668f884dea9cfb438189ceade3ab557485f04331a5e60"},"schema_version":"1.0"},"canonical_sha256":"2049c8825ca967b667dd2693fdf5582b1ca8186e565e4642a74e40a430480b85","source":{"kind":"arxiv","id":"1703.06280","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1703.06280","created_at":"2026-05-18T00:04:32Z"},{"alias_kind":"arxiv_version","alias_value":"1703.06280v4","created_at":"2026-05-18T00:04:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.06280","created_at":"2026-05-18T00:04:32Z"},{"alias_kind":"pith_short_12","alias_value":"EBE4RAS4VFT3","created_at":"2026-05-18T12:31:12Z"},{"alias_kind":"pith_short_16","alias_value":"EBE4RAS4VFT3MZ65","created_at":"2026-05-18T12:31:12Z"},{"alias_kind":"pith_short_8","alias_value":"EBE4RAS4","created_at":"2026-05-18T12:31:12Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:EBE4RAS4VFT3MZ65E2J735KYFM","target":"record","payload":{"canonical_record":{"source":{"id":"1703.06280","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-03-18T10:25:58Z","cross_cats_sorted":["cond-mat.supr-con"],"title_canon_sha256":"be172b377cbff20aa2a197eeee2defa8c2a593cdd9e533c39ef66106d0a0cb45","abstract_canon_sha256":"7a5f34c24b4696aca1e668f884dea9cfb438189ceade3ab557485f04331a5e60"},"schema_version":"1.0"},"canonical_sha256":"2049c8825ca967b667dd2693fdf5582b1ca8186e565e4642a74e40a430480b85","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:04:32.646503Z","signature_b64":"cPV1wHO9C2TU1UIYKHOrK9KSjx5JAOJ4Rxwr3YTwPIvWasEbD4lr2FcgUDI2CWL29AbJgWbcvp5C5m+2ocKnBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2049c8825ca967b667dd2693fdf5582b1ca8186e565e4642a74e40a430480b85","last_reissued_at":"2026-05-18T00:04:32.645782Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:04:32.645782Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1703.06280","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:04:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3NbXawOJAa5ZJTk3n0tNjjNPs4x2Ko1BFUxRriF8sXBsn8J7bmmlPDnoEmJyRCYW26fqAjVZzC4lqcXAqfIFBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T21:41:22.919616Z"},"content_sha256":"2dc8c7c33b00d00cdcdfea0b5747bbfec2c607b13ab68d025e9bf07eea05c85f","schema_version":"1.0","event_id":"sha256:2dc8c7c33b00d00cdcdfea0b5747bbfec2c607b13ab68d025e9bf07eea05c85f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:EBE4RAS4VFT3MZ65E2J735KYFM","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Coexistence of non-Fermi liquid and Fermi liquid self-energies at all dopings in cuprates","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con"],"primary_cat":"cond-mat.str-el","authors_text":"Sujay Ray, Tanmoy Das","submitted_at":"2017-03-18T10:25:58Z","abstract_excerpt":"Various angle-dependent measurements in hole-doped cuprates suggested that Non-Fermi liquid (NFL) and Fermi-liquid (FL) self-energies coexist in the Brillouin zone. Moreover, it is also found that NFL self-energies survive up to the overdoped region where the resistivity features a global FL-behavior. To address this problem, here we compute the momentum dependent self-energy from a single band Hubbard model. The self-energy is calculated self-consistently by using a momentum-dependent density-fluctuation (MRDF) method. One of our main result is that the computed self-energy exhibits a NFL-lik"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.06280","kind":"arxiv","version":4},"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":"2026-05-18T00:04:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"35q/n0PD2al7lVNSjZAxz39vmDB8wZk2zLW1/B5MRLfigHxlSCCXDklxZ4DvAmChovNRW7BSesXfIZZOF36QDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T21:41:22.919967Z"},"content_sha256":"1ef6fd4ba7dff3c51ec007ca977c230f7b9619cddbf13721fab3aed553be2801","schema_version":"1.0","event_id":"sha256:1ef6fd4ba7dff3c51ec007ca977c230f7b9619cddbf13721fab3aed553be2801"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/EBE4RAS4VFT3MZ65E2J735KYFM/bundle.json","state_url":"https://pith.science/pith/EBE4RAS4VFT3MZ65E2J735KYFM/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/EBE4RAS4VFT3MZ65E2J735KYFM/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":"2026-06-02T21:41:22Z","links":{"resolver":"https://pith.science/pith/EBE4RAS4VFT3MZ65E2J735KYFM","bundle":"https://pith.science/pith/EBE4RAS4VFT3MZ65E2J735KYFM/bundle.json","state":"https://pith.science/pith/EBE4RAS4VFT3MZ65E2J735KYFM/state.json","well_known_bundle":"https://pith.science/.well-known/pith/EBE4RAS4VFT3MZ65E2J735KYFM/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:EBE4RAS4VFT3MZ65E2J735KYFM","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":"7a5f34c24b4696aca1e668f884dea9cfb438189ceade3ab557485f04331a5e60","cross_cats_sorted":["cond-mat.supr-con"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-03-18T10:25:58Z","title_canon_sha256":"be172b377cbff20aa2a197eeee2defa8c2a593cdd9e533c39ef66106d0a0cb45"},"schema_version":"1.0","source":{"id":"1703.06280","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1703.06280","created_at":"2026-05-18T00:04:32Z"},{"alias_kind":"arxiv_version","alias_value":"1703.06280v4","created_at":"2026-05-18T00:04:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.06280","created_at":"2026-05-18T00:04:32Z"},{"alias_kind":"pith_short_12","alias_value":"EBE4RAS4VFT3","created_at":"2026-05-18T12:31:12Z"},{"alias_kind":"pith_short_16","alias_value":"EBE4RAS4VFT3MZ65","created_at":"2026-05-18T12:31:12Z"},{"alias_kind":"pith_short_8","alias_value":"EBE4RAS4","created_at":"2026-05-18T12:31:12Z"}],"graph_snapshots":[{"event_id":"sha256:1ef6fd4ba7dff3c51ec007ca977c230f7b9619cddbf13721fab3aed553be2801","target":"graph","created_at":"2026-05-18T00:04:32Z","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":"Various angle-dependent measurements in hole-doped cuprates suggested that Non-Fermi liquid (NFL) and Fermi-liquid (FL) self-energies coexist in the Brillouin zone. Moreover, it is also found that NFL self-energies survive up to the overdoped region where the resistivity features a global FL-behavior. To address this problem, here we compute the momentum dependent self-energy from a single band Hubbard model. The self-energy is calculated self-consistently by using a momentum-dependent density-fluctuation (MRDF) method. One of our main result is that the computed self-energy exhibits a NFL-lik","authors_text":"Sujay Ray, Tanmoy Das","cross_cats":["cond-mat.supr-con"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-03-18T10:25:58Z","title":"Coexistence of non-Fermi liquid and Fermi liquid self-energies at all dopings in cuprates"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.06280","kind":"arxiv","version":4},"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":"sha256:2dc8c7c33b00d00cdcdfea0b5747bbfec2c607b13ab68d025e9bf07eea05c85f","target":"record","created_at":"2026-05-18T00:04:32Z","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":"7a5f34c24b4696aca1e668f884dea9cfb438189ceade3ab557485f04331a5e60","cross_cats_sorted":["cond-mat.supr-con"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-03-18T10:25:58Z","title_canon_sha256":"be172b377cbff20aa2a197eeee2defa8c2a593cdd9e533c39ef66106d0a0cb45"},"schema_version":"1.0","source":{"id":"1703.06280","kind":"arxiv","version":4}},"canonical_sha256":"2049c8825ca967b667dd2693fdf5582b1ca8186e565e4642a74e40a430480b85","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2049c8825ca967b667dd2693fdf5582b1ca8186e565e4642a74e40a430480b85","first_computed_at":"2026-05-18T00:04:32.645782Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:04:32.645782Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"cPV1wHO9C2TU1UIYKHOrK9KSjx5JAOJ4Rxwr3YTwPIvWasEbD4lr2FcgUDI2CWL29AbJgWbcvp5C5m+2ocKnBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:04:32.646503Z","signed_message":"canonical_sha256_bytes"},"source_id":"1703.06280","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2dc8c7c33b00d00cdcdfea0b5747bbfec2c607b13ab68d025e9bf07eea05c85f","sha256:1ef6fd4ba7dff3c51ec007ca977c230f7b9619cddbf13721fab3aed553be2801"],"state_sha256":"2cdd26e726c1164960f6e3f192ed0ed20af21e417383f27652c597358d6dd145"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3RTSCR9USmqU1LoZ50nJJAxhRjqSUbF0djOv0Hw728GDuTc3d0KwLQTv5mjH5Pva+rTCUsPsbGuJPGyY08oCAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T21:41:22.921954Z","bundle_sha256":"0eeda241f1b6a45a42800f9a8f8b491257f1912fce2a21a0a319d2af3a99fec6"}}