{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:M3CONWSJZ5Z2OE6DSJ22Z4NCHG","short_pith_number":"pith:M3CONWSJ","canonical_record":{"source":{"id":"1012.3751","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-12-16T21:00:06Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"a6e34b96508459b6a96bd1353b3a9ea75f452d0720c0a8d1548663d9ac93a793","abstract_canon_sha256":"a97ec4804d569766ab722b742ed0fd9bac75b232cb0209f9c5c3c35d61376c41"},"schema_version":"1.0"},"canonical_sha256":"66c4e6da49cf73a713c39275acf1a239af15d1c6647f31685ea79814f6db21ce","source":{"kind":"arxiv","id":"1012.3751","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1012.3751","created_at":"2026-05-18T04:26:12Z"},{"alias_kind":"arxiv_version","alias_value":"1012.3751v1","created_at":"2026-05-18T04:26:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1012.3751","created_at":"2026-05-18T04:26:12Z"},{"alias_kind":"pith_short_12","alias_value":"M3CONWSJZ5Z2","created_at":"2026-05-18T12:26:10Z"},{"alias_kind":"pith_short_16","alias_value":"M3CONWSJZ5Z2OE6D","created_at":"2026-05-18T12:26:10Z"},{"alias_kind":"pith_short_8","alias_value":"M3CONWSJ","created_at":"2026-05-18T12:26:10Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:M3CONWSJZ5Z2OE6DSJ22Z4NCHG","target":"record","payload":{"canonical_record":{"source":{"id":"1012.3751","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-12-16T21:00:06Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"a6e34b96508459b6a96bd1353b3a9ea75f452d0720c0a8d1548663d9ac93a793","abstract_canon_sha256":"a97ec4804d569766ab722b742ed0fd9bac75b232cb0209f9c5c3c35d61376c41"},"schema_version":"1.0"},"canonical_sha256":"66c4e6da49cf73a713c39275acf1a239af15d1c6647f31685ea79814f6db21ce","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:26:12.844030Z","signature_b64":"4zmLaBXEAYL3h0T1rVQpbsno2BpvIZFA1nGs/TZAvds20HMYI0+PQttr9hcwFClfn/uIGZ1oFNOmdVYRBh05Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"66c4e6da49cf73a713c39275acf1a239af15d1c6647f31685ea79814f6db21ce","last_reissued_at":"2026-05-18T04:26:12.843277Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:26:12.843277Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1012.3751","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:26:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"EsK61RqzuPc+KO7NO5nAMu9jOPM7166yuhAnIDlWnFzO44Z2T3Xd2QiKfVezA/u39sQMy2WDAtc6XES23vKLAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-23T19:09:35.265262Z"},"content_sha256":"5f5c4f07f5f160c576a51e61a3cb097302ca8d8c09839d3b7fc5f8bcad367f70","schema_version":"1.0","event_id":"sha256:5f5c4f07f5f160c576a51e61a3cb097302ca8d8c09839d3b7fc5f8bcad367f70"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:M3CONWSJZ5Z2OE6DSJ22Z4NCHG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dynamical Gap and Cuprate-like Physics from Holography","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"hep-th","authors_text":"Ka Wai Lo, Mohammad Edalati, Philip W. Phillips, Robert G. Leigh","submitted_at":"2010-12-16T21:00:06Z","abstract_excerpt":"We study the properties of fermion correlators in a boundary theory dual to the Reissner-Nordstr\\\"om AdS_{d+1} background in the presence of a bulk dipole (Pauli) interaction term with strength p. We show that by simply changing the value of the parameter p we can tune continuously from a Fermi liquid (small p), to a marginal Fermi liquid behavior at a critical value of p, to a generic non-Fermi liquid at intermediate values of p, and finally to a Mott insulator at large values of the bulk Pauli coupling. As all of these phases are seen in the cuprate phase diagram, the holographic model we st"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1012.3751","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:26:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ja6CA3vshKZrS2x7oCtMv7YNmdL/jnp3Ip66X6lRZgQBcZ5YkXgo1AUcXs8p6MvCcjEAm3mHg7jvigMv30YJCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-23T19:09:35.266034Z"},"content_sha256":"6ac6db8d4b7f30752a67a49bf78e935858e255bdf8ddcddb945000dd7362cc96","schema_version":"1.0","event_id":"sha256:6ac6db8d4b7f30752a67a49bf78e935858e255bdf8ddcddb945000dd7362cc96"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/M3CONWSJZ5Z2OE6DSJ22Z4NCHG/bundle.json","state_url":"https://pith.science/pith/M3CONWSJZ5Z2OE6DSJ22Z4NCHG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/M3CONWSJZ5Z2OE6DSJ22Z4NCHG/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":"2026-05-23T19:09:35Z","links":{"resolver":"https://pith.science/pith/M3CONWSJZ5Z2OE6DSJ22Z4NCHG","bundle":"https://pith.science/pith/M3CONWSJZ5Z2OE6DSJ22Z4NCHG/bundle.json","state":"https://pith.science/pith/M3CONWSJZ5Z2OE6DSJ22Z4NCHG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/M3CONWSJZ5Z2OE6DSJ22Z4NCHG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:M3CONWSJZ5Z2OE6DSJ22Z4NCHG","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":"a97ec4804d569766ab722b742ed0fd9bac75b232cb0209f9c5c3c35d61376c41","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-12-16T21:00:06Z","title_canon_sha256":"a6e34b96508459b6a96bd1353b3a9ea75f452d0720c0a8d1548663d9ac93a793"},"schema_version":"1.0","source":{"id":"1012.3751","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1012.3751","created_at":"2026-05-18T04:26:12Z"},{"alias_kind":"arxiv_version","alias_value":"1012.3751v1","created_at":"2026-05-18T04:26:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1012.3751","created_at":"2026-05-18T04:26:12Z"},{"alias_kind":"pith_short_12","alias_value":"M3CONWSJZ5Z2","created_at":"2026-05-18T12:26:10Z"},{"alias_kind":"pith_short_16","alias_value":"M3CONWSJZ5Z2OE6D","created_at":"2026-05-18T12:26:10Z"},{"alias_kind":"pith_short_8","alias_value":"M3CONWSJ","created_at":"2026-05-18T12:26:10Z"}],"graph_snapshots":[{"event_id":"sha256:6ac6db8d4b7f30752a67a49bf78e935858e255bdf8ddcddb945000dd7362cc96","target":"graph","created_at":"2026-05-18T04:26:12Z","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":"We study the properties of fermion correlators in a boundary theory dual to the Reissner-Nordstr\\\"om AdS_{d+1} background in the presence of a bulk dipole (Pauli) interaction term with strength p. We show that by simply changing the value of the parameter p we can tune continuously from a Fermi liquid (small p), to a marginal Fermi liquid behavior at a critical value of p, to a generic non-Fermi liquid at intermediate values of p, and finally to a Mott insulator at large values of the bulk Pauli coupling. As all of these phases are seen in the cuprate phase diagram, the holographic model we st","authors_text":"Ka Wai Lo, Mohammad Edalati, Philip W. Phillips, Robert G. Leigh","cross_cats":["cond-mat.str-el"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-12-16T21:00:06Z","title":"Dynamical Gap and Cuprate-like Physics from Holography"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1012.3751","kind":"arxiv","version":1},"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":"sha256:5f5c4f07f5f160c576a51e61a3cb097302ca8d8c09839d3b7fc5f8bcad367f70","target":"record","created_at":"2026-05-18T04:26:12Z","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":"a97ec4804d569766ab722b742ed0fd9bac75b232cb0209f9c5c3c35d61376c41","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-12-16T21:00:06Z","title_canon_sha256":"a6e34b96508459b6a96bd1353b3a9ea75f452d0720c0a8d1548663d9ac93a793"},"schema_version":"1.0","source":{"id":"1012.3751","kind":"arxiv","version":1}},"canonical_sha256":"66c4e6da49cf73a713c39275acf1a239af15d1c6647f31685ea79814f6db21ce","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"66c4e6da49cf73a713c39275acf1a239af15d1c6647f31685ea79814f6db21ce","first_computed_at":"2026-05-18T04:26:12.843277Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:26:12.843277Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4zmLaBXEAYL3h0T1rVQpbsno2BpvIZFA1nGs/TZAvds20HMYI0+PQttr9hcwFClfn/uIGZ1oFNOmdVYRBh05Dg==","signature_status":"signed_v1","signed_at":"2026-05-18T04:26:12.844030Z","signed_message":"canonical_sha256_bytes"},"source_id":"1012.3751","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5f5c4f07f5f160c576a51e61a3cb097302ca8d8c09839d3b7fc5f8bcad367f70","sha256:6ac6db8d4b7f30752a67a49bf78e935858e255bdf8ddcddb945000dd7362cc96"],"state_sha256":"35055734656951abde3e62c6677f7b2bf83036f155577170e5eab9c2fd161f26"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1Vv0PlaNPXzWWE3llSKdpPeyyYmHxh+/xZ7mlyW90WSM/3ZF+7oC967jYJAEtClkJHCxzfkrAohrJcW7j2sPDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-23T19:09:35.270085Z","bundle_sha256":"0b3b855c47cf723858f9f487c503a1befecbe34e1dd6877acb316afa8d05e228"}}