{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:PUG5WTU3JPN3BNRCMKABJZLJWU","short_pith_number":"pith:PUG5WTU3","schema_version":"1.0","canonical_sha256":"7d0ddb4e9b4bdbb0b622628014e569b50a5455f47959f48bb12fdda4bec39d93","source":{"kind":"arxiv","id":"1110.4559","version":3},"attestation_state":"computed","paper":{"title":"Holographic non-relativistic fermionic fixed point and bulk dipole coupling","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","gr-qc"],"primary_cat":"hep-th","authors_text":"Hongbao Zhang, Wei-Jia Li","submitted_at":"2011-10-20T15:55:01Z","abstract_excerpt":"Inspired by the recently discovered non-relativistic fermionic fixed points, we investigate how the presence of bulk dipole coupling modifies the spectral function at one of these novel fixed points. As a result, although the infinite flat band is always visible in the presence of the bulk dipole coupling as well as chemical potential, the band is modified in a remarkable way at small momenta up to the order of magnitude of bulk dipole coupling. On the other hand, like a phoenix, a new Fermi surface sprouts from the formed gap when the bulk dipole coupling is pushed up further such as to overs"},"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":"1110.4559","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-10-20T15:55:01Z","cross_cats_sorted":["cond-mat.str-el","gr-qc"],"title_canon_sha256":"ace843af2c8fb83eb95d72dd7b244143a9382d8a479f5973cb666cc0934f25e6","abstract_canon_sha256":"16ea77abf616fdeac74a94bed62a4d5d01607dfab221941820e274a7c8472735"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:21:35.170004Z","signature_b64":"NIwm/gd9fUcmYe/hfkjYZhXLkmQYB3j98UF6QiidzCVRFODhWJqvypcU0Dy83Q6exkOIqFIWndq7zzq2WFz8AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7d0ddb4e9b4bdbb0b622628014e569b50a5455f47959f48bb12fdda4bec39d93","last_reissued_at":"2026-05-18T02:21:35.169470Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:21:35.169470Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Holographic non-relativistic fermionic fixed point and bulk dipole coupling","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","gr-qc"],"primary_cat":"hep-th","authors_text":"Hongbao Zhang, Wei-Jia Li","submitted_at":"2011-10-20T15:55:01Z","abstract_excerpt":"Inspired by the recently discovered non-relativistic fermionic fixed points, we investigate how the presence of bulk dipole coupling modifies the spectral function at one of these novel fixed points. As a result, although the infinite flat band is always visible in the presence of the bulk dipole coupling as well as chemical potential, the band is modified in a remarkable way at small momenta up to the order of magnitude of bulk dipole coupling. On the other hand, like a phoenix, a new Fermi surface sprouts from the formed gap when the bulk dipole coupling is pushed up further such as to overs"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1110.4559","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1110.4559","created_at":"2026-05-18T02:21:35.169548+00:00"},{"alias_kind":"arxiv_version","alias_value":"1110.4559v3","created_at":"2026-05-18T02:21:35.169548+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1110.4559","created_at":"2026-05-18T02:21:35.169548+00:00"},{"alias_kind":"pith_short_12","alias_value":"PUG5WTU3JPN3","created_at":"2026-05-18T12:26:39.201973+00:00"},{"alias_kind":"pith_short_16","alias_value":"PUG5WTU3JPN3BNRC","created_at":"2026-05-18T12:26:39.201973+00:00"},{"alias_kind":"pith_short_8","alias_value":"PUG5WTU3","created_at":"2026-05-18T12:26:39.201973+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2608.06887","citing_title":"The spectral gap of the ABJM model: A holographic perspective from uplifted higher-dimensional geometries","ref_index":4,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PUG5WTU3JPN3BNRCMKABJZLJWU","json":"https://pith.science/pith/PUG5WTU3JPN3BNRCMKABJZLJWU.json","graph_json":"https://pith.science/api/pith-number/PUG5WTU3JPN3BNRCMKABJZLJWU/graph.json","events_json":"https://pith.science/api/pith-number/PUG5WTU3JPN3BNRCMKABJZLJWU/events.json","paper":"https://pith.science/paper/PUG5WTU3"},"agent_actions":{"view_html":"https://pith.science/pith/PUG5WTU3JPN3BNRCMKABJZLJWU","download_json":"https://pith.science/pith/PUG5WTU3JPN3BNRCMKABJZLJWU.json","view_paper":"https://pith.science/paper/PUG5WTU3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1110.4559&json=true","fetch_graph":"https://pith.science/api/pith-number/PUG5WTU3JPN3BNRCMKABJZLJWU/graph.json","fetch_events":"https://pith.science/api/pith-number/PUG5WTU3JPN3BNRCMKABJZLJWU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PUG5WTU3JPN3BNRCMKABJZLJWU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PUG5WTU3JPN3BNRCMKABJZLJWU/action/storage_attestation","attest_author":"https://pith.science/pith/PUG5WTU3JPN3BNRCMKABJZLJWU/action/author_attestation","sign_citation":"https://pith.science/pith/PUG5WTU3JPN3BNRCMKABJZLJWU/action/citation_signature","submit_replication":"https://pith.science/pith/PUG5WTU3JPN3BNRCMKABJZLJWU/action/replication_record"}},"created_at":"2026-05-18T02:21:35.169548+00:00","updated_at":"2026-05-18T02:21:35.169548+00:00"}