{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:3SGJHHXJ7HSQ37GKVEFCWGAKH5","short_pith_number":"pith:3SGJHHXJ","schema_version":"1.0","canonical_sha256":"dc8c939ee9f9e50dfccaa90a2b180a3f51676e5938e64a37662b908ee13fbe0a","source":{"kind":"arxiv","id":"2406.14858","version":1},"attestation_state":"computed","paper":{"title":"A mechanism for quantum-critical Planckian metal phase in high-temperature cuprate superconductors","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Chung-Hou Chung, Khoe Van Nguyen, Kim Remund, Yung-Yeh Chang","submitted_at":"2024-06-21T04:16:11Z","abstract_excerpt":"The mysterious metallic phase showing perfect $T$-linear resistivity and a universal scattering rate $1/\\tau = \\alpha_P k_B T /\\hbar$ with a universal prefactor $\\alpha_P \\sim 1$ and logarithmic-in-temperature singular specific heat coefficient, so-called Planckian metal phase was observed in various overdoped high-$T_c$ cuprate superconductors over a finite range in doping. Here, we propose a microscopic mechanism for this exotic state based on quantum-critical bosonic charge Kondo fluctuations coupled to both spinon and a heavy conduction-electron Fermi surfaces within the heavy-fermion form"},"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":"2406.14858","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-06-21T04:16:11Z","cross_cats_sorted":[],"title_canon_sha256":"338015fc44a5d7afddbf8bc7a3a3f414c9ad5ba58d4fd1ceb63a4663187433d0","abstract_canon_sha256":"31d6c4b4190c9f9b11c7e6e35f2e98ac533b37af92533b42ee2071eb1972d76e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:35:09.433687Z","signature_b64":"Ve9s86OoB67nmkHAJ4GXU3B3VcYrQTYP3Sfba9nQGggkeyoeePOZsg5kGkevVszEcQ41HBHAPkyO5vOT7j6FDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dc8c939ee9f9e50dfccaa90a2b180a3f51676e5938e64a37662b908ee13fbe0a","last_reissued_at":"2026-07-05T08:35:09.433166Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:35:09.433166Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A mechanism for quantum-critical Planckian metal phase in high-temperature cuprate superconductors","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Chung-Hou Chung, Khoe Van Nguyen, Kim Remund, Yung-Yeh Chang","submitted_at":"2024-06-21T04:16:11Z","abstract_excerpt":"The mysterious metallic phase showing perfect $T$-linear resistivity and a universal scattering rate $1/\\tau = \\alpha_P k_B T /\\hbar$ with a universal prefactor $\\alpha_P \\sim 1$ and logarithmic-in-temperature singular specific heat coefficient, so-called Planckian metal phase was observed in various overdoped high-$T_c$ cuprate superconductors over a finite range in doping. Here, we propose a microscopic mechanism for this exotic state based on quantum-critical bosonic charge Kondo fluctuations coupled to both spinon and a heavy conduction-electron Fermi surfaces within the heavy-fermion form"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2406.14858","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2406.14858/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2406.14858","created_at":"2026-07-05T08:35:09.433259+00:00"},{"alias_kind":"arxiv_version","alias_value":"2406.14858v1","created_at":"2026-07-05T08:35:09.433259+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2406.14858","created_at":"2026-07-05T08:35:09.433259+00:00"},{"alias_kind":"pith_short_12","alias_value":"3SGJHHXJ7HSQ","created_at":"2026-07-05T08:35:09.433259+00:00"},{"alias_kind":"pith_short_16","alias_value":"3SGJHHXJ7HSQ37GK","created_at":"2026-07-05T08:35:09.433259+00:00"},{"alias_kind":"pith_short_8","alias_value":"3SGJHHXJ","created_at":"2026-07-05T08:35:09.433259+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.08476","citing_title":"The charge density fluctuations and the Shrinking Fermi Liquid scenario for strange metallicity in cuprates","ref_index":158,"is_internal_anchor":true},{"citing_arxiv_id":"2504.01059","citing_title":"Theory of Linear Magnetoresistance in a Strange Metal","ref_index":19,"is_internal_anchor":false},{"citing_arxiv_id":"2508.20164","citing_title":"Fractionalized Fermi liquids and the cuprate phase diagram","ref_index":104,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3SGJHHXJ7HSQ37GKVEFCWGAKH5","json":"https://pith.science/pith/3SGJHHXJ7HSQ37GKVEFCWGAKH5.json","graph_json":"https://pith.science/api/pith-number/3SGJHHXJ7HSQ37GKVEFCWGAKH5/graph.json","events_json":"https://pith.science/api/pith-number/3SGJHHXJ7HSQ37GKVEFCWGAKH5/events.json","paper":"https://pith.science/paper/3SGJHHXJ"},"agent_actions":{"view_html":"https://pith.science/pith/3SGJHHXJ7HSQ37GKVEFCWGAKH5","download_json":"https://pith.science/pith/3SGJHHXJ7HSQ37GKVEFCWGAKH5.json","view_paper":"https://pith.science/paper/3SGJHHXJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2406.14858&json=true","fetch_graph":"https://pith.science/api/pith-number/3SGJHHXJ7HSQ37GKVEFCWGAKH5/graph.json","fetch_events":"https://pith.science/api/pith-number/3SGJHHXJ7HSQ37GKVEFCWGAKH5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3SGJHHXJ7HSQ37GKVEFCWGAKH5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3SGJHHXJ7HSQ37GKVEFCWGAKH5/action/storage_attestation","attest_author":"https://pith.science/pith/3SGJHHXJ7HSQ37GKVEFCWGAKH5/action/author_attestation","sign_citation":"https://pith.science/pith/3SGJHHXJ7HSQ37GKVEFCWGAKH5/action/citation_signature","submit_replication":"https://pith.science/pith/3SGJHHXJ7HSQ37GKVEFCWGAKH5/action/replication_record"}},"created_at":"2026-07-05T08:35:09.433259+00:00","updated_at":"2026-07-05T08:35:09.433259+00:00"}