{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:JJ5PUHLHGVEJ7QMDRODDTBSJUP","short_pith_number":"pith:JJ5PUHLH","schema_version":"1.0","canonical_sha256":"4a7afa1d6735489fc1838b86398649a3d3bcb90d78d768e6a53dbbf622c836a3","source":{"kind":"arxiv","id":"1509.01611","version":1},"attestation_state":"computed","paper":{"title":"Power Law Liquid - A Unified Form of Low-Energy Nodal Electronic Interactions in Hole Doped Cuprate Superconductors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"D. S. Dessau, G.B. Arnold, G. Gu, H. Eisaki, H. Li, J.A. Waugh, J.S. Wen, N.C. Plumb, Q. Wang, S. Parham, T.J. Reber, X. Zhou, Y. Cao, Y. Yoshida, Z.J. Xu, Z. Sun","submitted_at":"2015-09-04T21:15:29Z","abstract_excerpt":"The strange-metal phase of the cuprate high temperature superconductors, above where the superconductivity sets in as a function of temperature, is widely considered more exotic and mysterious than the superconductivity itself. Here, based upon detailed angle resolved photoemission spectroscopy measurements of Bi$_2$Sr$_2$CaCu$_2$O$_8$$_+$$_\\delta$ over a wide range of doping levels, we present a new unifying phenomenology for the non-Fermi liquid normal-state interactions (scattering rates) in the nodal direction. This new phenomenology has a continuously varying power law exponent (hence nam"},"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":"1509.01611","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2015-09-04T21:15:29Z","cross_cats_sorted":[],"title_canon_sha256":"5bf27be0a03d7f99693c51475d1d83e1600697d95a6c7372f16797b0deb844bd","abstract_canon_sha256":"4bf7e9311af7a37a1b51120f5a6b5d911181ff5a1c45b805a036987501fee8ff"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:33:51.070395Z","signature_b64":"2vxAYhThNEevtXekdrKG2w3QgVbdwjlPBVousA9UNynoVr/VcVZ0fYj0U/5+SzNS/70ncG3sR1T5mb/nN47dCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4a7afa1d6735489fc1838b86398649a3d3bcb90d78d768e6a53dbbf622c836a3","last_reissued_at":"2026-05-18T01:33:51.069807Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:33:51.069807Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Power Law Liquid - A Unified Form of Low-Energy Nodal Electronic Interactions in Hole Doped Cuprate Superconductors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"D. S. Dessau, G.B. Arnold, G. Gu, H. Eisaki, H. Li, J.A. Waugh, J.S. Wen, N.C. Plumb, Q. Wang, S. Parham, T.J. Reber, X. Zhou, Y. Cao, Y. Yoshida, Z.J. Xu, Z. Sun","submitted_at":"2015-09-04T21:15:29Z","abstract_excerpt":"The strange-metal phase of the cuprate high temperature superconductors, above where the superconductivity sets in as a function of temperature, is widely considered more exotic and mysterious than the superconductivity itself. Here, based upon detailed angle resolved photoemission spectroscopy measurements of Bi$_2$Sr$_2$CaCu$_2$O$_8$$_+$$_\\delta$ over a wide range of doping levels, we present a new unifying phenomenology for the non-Fermi liquid normal-state interactions (scattering rates) in the nodal direction. This new phenomenology has a continuously varying power law exponent (hence nam"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.01611","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":"1509.01611","created_at":"2026-05-18T01:33:51.069902+00:00"},{"alias_kind":"arxiv_version","alias_value":"1509.01611v1","created_at":"2026-05-18T01:33:51.069902+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.01611","created_at":"2026-05-18T01:33:51.069902+00:00"},{"alias_kind":"pith_short_12","alias_value":"JJ5PUHLHGVEJ","created_at":"2026-05-18T12:29:27.538025+00:00"},{"alias_kind":"pith_short_16","alias_value":"JJ5PUHLHGVEJ7QMD","created_at":"2026-05-18T12:29:27.538025+00:00"},{"alias_kind":"pith_short_8","alias_value":"JJ5PUHLH","created_at":"2026-05-18T12:29:27.538025+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/JJ5PUHLHGVEJ7QMDRODDTBSJUP","json":"https://pith.science/pith/JJ5PUHLHGVEJ7QMDRODDTBSJUP.json","graph_json":"https://pith.science/api/pith-number/JJ5PUHLHGVEJ7QMDRODDTBSJUP/graph.json","events_json":"https://pith.science/api/pith-number/JJ5PUHLHGVEJ7QMDRODDTBSJUP/events.json","paper":"https://pith.science/paper/JJ5PUHLH"},"agent_actions":{"view_html":"https://pith.science/pith/JJ5PUHLHGVEJ7QMDRODDTBSJUP","download_json":"https://pith.science/pith/JJ5PUHLHGVEJ7QMDRODDTBSJUP.json","view_paper":"https://pith.science/paper/JJ5PUHLH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1509.01611&json=true","fetch_graph":"https://pith.science/api/pith-number/JJ5PUHLHGVEJ7QMDRODDTBSJUP/graph.json","fetch_events":"https://pith.science/api/pith-number/JJ5PUHLHGVEJ7QMDRODDTBSJUP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JJ5PUHLHGVEJ7QMDRODDTBSJUP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JJ5PUHLHGVEJ7QMDRODDTBSJUP/action/storage_attestation","attest_author":"https://pith.science/pith/JJ5PUHLHGVEJ7QMDRODDTBSJUP/action/author_attestation","sign_citation":"https://pith.science/pith/JJ5PUHLHGVEJ7QMDRODDTBSJUP/action/citation_signature","submit_replication":"https://pith.science/pith/JJ5PUHLHGVEJ7QMDRODDTBSJUP/action/replication_record"}},"created_at":"2026-05-18T01:33:51.069902+00:00","updated_at":"2026-05-18T01:33:51.069902+00:00"}