{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:6VTCIMVEMLKWPA7WMQBPJXC2S7","short_pith_number":"pith:6VTCIMVE","schema_version":"1.0","canonical_sha256":"f5662432a462d56783f66402f4dc5a97fb2576bc6b9c4e975c3a29273531838c","source":{"kind":"arxiv","id":"2010.03560","version":1},"attestation_state":"computed","paper":{"title":"Holographic non-Fermi liquids at large $d$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"hep-th","authors_text":"Milind Shyani, Shamit Kachru","submitted_at":"2020-10-07T17:59:58Z","abstract_excerpt":"Motivated by the results of Dynamical Mean Field Theory, we study the two-point function of fermions moving in a charged black brane background in $AdS_{d+1}$ in the limit of large $d$. We observe the emergence of a locally critical form of the fermion self-energy, with a strongly constrained range of possible scaling behaviors at large $d$. Novelties compared to the analysis in $d=3,4$ include an enlarged regime of temperatures where the results apply, and the analytical tractability of the calculations."},"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":"2010.03560","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2020-10-07T17:59:58Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"c91baeb7759e08e343e5f204c59c4d14e3e3339c9e2727252496fcec084fc304","abstract_canon_sha256":"a8c4eba3b13d1b3a72b2d51717a9241e302b43678fa77064d45b9aee6908c880"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:41:14.052461Z","signature_b64":"UiOsTt4Z/D902XfDdiQtB7TLSp4Spc6gIyhZ6g1rSdpx0hBuL03DHiG7DqDa5DdTi+GvNbsgbi2FIi8upVThBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f5662432a462d56783f66402f4dc5a97fb2576bc6b9c4e975c3a29273531838c","last_reissued_at":"2026-07-05T01:41:14.052111Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:41:14.052111Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Holographic non-Fermi liquids at large $d$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"hep-th","authors_text":"Milind Shyani, Shamit Kachru","submitted_at":"2020-10-07T17:59:58Z","abstract_excerpt":"Motivated by the results of Dynamical Mean Field Theory, we study the two-point function of fermions moving in a charged black brane background in $AdS_{d+1}$ in the limit of large $d$. We observe the emergence of a locally critical form of the fermion self-energy, with a strongly constrained range of possible scaling behaviors at large $d$. Novelties compared to the analysis in $d=3,4$ include an enlarged regime of temperatures where the results apply, and the analytical tractability of the calculations."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2010.03560","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/2010.03560/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":"2010.03560","created_at":"2026-07-05T01:41:14.052168+00:00"},{"alias_kind":"arxiv_version","alias_value":"2010.03560v1","created_at":"2026-07-05T01:41:14.052168+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2010.03560","created_at":"2026-07-05T01:41:14.052168+00:00"},{"alias_kind":"pith_short_12","alias_value":"6VTCIMVEMLKW","created_at":"2026-07-05T01:41:14.052168+00:00"},{"alias_kind":"pith_short_16","alias_value":"6VTCIMVEMLKWPA7W","created_at":"2026-07-05T01:41:14.052168+00:00"},{"alias_kind":"pith_short_8","alias_value":"6VTCIMVE","created_at":"2026-07-05T01:41:14.052168+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/6VTCIMVEMLKWPA7WMQBPJXC2S7","json":"https://pith.science/pith/6VTCIMVEMLKWPA7WMQBPJXC2S7.json","graph_json":"https://pith.science/api/pith-number/6VTCIMVEMLKWPA7WMQBPJXC2S7/graph.json","events_json":"https://pith.science/api/pith-number/6VTCIMVEMLKWPA7WMQBPJXC2S7/events.json","paper":"https://pith.science/paper/6VTCIMVE"},"agent_actions":{"view_html":"https://pith.science/pith/6VTCIMVEMLKWPA7WMQBPJXC2S7","download_json":"https://pith.science/pith/6VTCIMVEMLKWPA7WMQBPJXC2S7.json","view_paper":"https://pith.science/paper/6VTCIMVE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2010.03560&json=true","fetch_graph":"https://pith.science/api/pith-number/6VTCIMVEMLKWPA7WMQBPJXC2S7/graph.json","fetch_events":"https://pith.science/api/pith-number/6VTCIMVEMLKWPA7WMQBPJXC2S7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6VTCIMVEMLKWPA7WMQBPJXC2S7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6VTCIMVEMLKWPA7WMQBPJXC2S7/action/storage_attestation","attest_author":"https://pith.science/pith/6VTCIMVEMLKWPA7WMQBPJXC2S7/action/author_attestation","sign_citation":"https://pith.science/pith/6VTCIMVEMLKWPA7WMQBPJXC2S7/action/citation_signature","submit_replication":"https://pith.science/pith/6VTCIMVEMLKWPA7WMQBPJXC2S7/action/replication_record"}},"created_at":"2026-07-05T01:41:14.052168+00:00","updated_at":"2026-07-05T01:41:14.052168+00:00"}