{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:UQTTCJD6DKWN7VPOBJLUFKNMFZ","short_pith_number":"pith:UQTTCJD6","canonical_record":{"source":{"id":"1207.3352","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-07-13T20:00:01Z","cross_cats_sorted":[],"title_canon_sha256":"8e3c2dbb00034a46ef2c73f5739383c6cdb743a6eb9799b33f9e200358f6e8aa","abstract_canon_sha256":"a53a6ce3503a9d57df69201d5ba0a7219232401e60738c2770bd229194b4e09f"},"schema_version":"1.0"},"canonical_sha256":"a42731247e1aacdfd5ee0a5742a9ac2e6e27edc2f21b2baf98067a4fd1b04b00","source":{"kind":"arxiv","id":"1207.3352","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1207.3352","created_at":"2026-05-18T03:22:39Z"},{"alias_kind":"arxiv_version","alias_value":"1207.3352v2","created_at":"2026-05-18T03:22:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.3352","created_at":"2026-05-18T03:22:39Z"},{"alias_kind":"pith_short_12","alias_value":"UQTTCJD6DKWN","created_at":"2026-05-18T12:27:23Z"},{"alias_kind":"pith_short_16","alias_value":"UQTTCJD6DKWN7VPO","created_at":"2026-05-18T12:27:23Z"},{"alias_kind":"pith_short_8","alias_value":"UQTTCJD6","created_at":"2026-05-18T12:27:23Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:UQTTCJD6DKWN7VPOBJLUFKNMFZ","target":"record","payload":{"canonical_record":{"source":{"id":"1207.3352","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-07-13T20:00:01Z","cross_cats_sorted":[],"title_canon_sha256":"8e3c2dbb00034a46ef2c73f5739383c6cdb743a6eb9799b33f9e200358f6e8aa","abstract_canon_sha256":"a53a6ce3503a9d57df69201d5ba0a7219232401e60738c2770bd229194b4e09f"},"schema_version":"1.0"},"canonical_sha256":"a42731247e1aacdfd5ee0a5742a9ac2e6e27edc2f21b2baf98067a4fd1b04b00","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:22:39.269925Z","signature_b64":"T7/ByxepHofkixJebUGloFj4FHaOhGMJoYkIf1riR+ooFQUHz9SMbEQdgzYJFPlCF608STHQ7PbtLa6ouavcDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a42731247e1aacdfd5ee0a5742a9ac2e6e27edc2f21b2baf98067a4fd1b04b00","last_reissued_at":"2026-05-18T03:22:39.269284Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:22:39.269284Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1207.3352","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:22:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pyRE8op2ldUcv5hFBMKvars6cvMS4f9H27fm0Qz7eRwj5PQRrGprHZ/rF+J8JKm2cOMxrrxPyHnRiZR1m/pfBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T14:50:58.593423Z"},"content_sha256":"4996a20fe66cf1bd2e7bffd576e4aa193703cea65060b3da1a57417fd657ae00","schema_version":"1.0","event_id":"sha256:4996a20fe66cf1bd2e7bffd576e4aa193703cea65060b3da1a57417fd657ae00"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:UQTTCJD6DKWN7VPOBJLUFKNMFZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Fermi surfaces in N=4 Super-Yang-Mills theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Christopher Rosen, Oliver DeWolfe, Steven S. Gubser","submitted_at":"2012-07-13T20:00:01Z","abstract_excerpt":"We investigate and classify Fermi surface behavior for a set of fermionic modes in a family of backgrounds holographically dual to N=4 Super-Yang-Mills theory at zero temperature with two distinct chemical potentials. We numerically solve fluctuation equations for every spin-1/2 field in five-dimensional maximally supersymmetric gauged supergravity not mixing with gravitini. Different modes manifest two, one or zero Fermi surface singularities, all associated to non-Fermi liquids, and we calculate dispersion relations and widths of excitations. We study two limits where the zero-temperature en"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.3352","kind":"arxiv","version":2},"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":"2026-05-18T03:22:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ymegpocuVcafgKXeX2noRyXgypiHx6wXDQivnrFr9lZYKQKHFo+0X1rSXRTHB3Yn5XDt7uvilXLDRVzkS/aoBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T14:50:58.593781Z"},"content_sha256":"7103d0c376a1bfdd90ae92cc678250255317e185c53df7750e1e741944d59a2b","schema_version":"1.0","event_id":"sha256:7103d0c376a1bfdd90ae92cc678250255317e185c53df7750e1e741944d59a2b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UQTTCJD6DKWN7VPOBJLUFKNMFZ/bundle.json","state_url":"https://pith.science/pith/UQTTCJD6DKWN7VPOBJLUFKNMFZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UQTTCJD6DKWN7VPOBJLUFKNMFZ/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":"2026-05-29T14:50:58Z","links":{"resolver":"https://pith.science/pith/UQTTCJD6DKWN7VPOBJLUFKNMFZ","bundle":"https://pith.science/pith/UQTTCJD6DKWN7VPOBJLUFKNMFZ/bundle.json","state":"https://pith.science/pith/UQTTCJD6DKWN7VPOBJLUFKNMFZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UQTTCJD6DKWN7VPOBJLUFKNMFZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:UQTTCJD6DKWN7VPOBJLUFKNMFZ","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":"a53a6ce3503a9d57df69201d5ba0a7219232401e60738c2770bd229194b4e09f","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-07-13T20:00:01Z","title_canon_sha256":"8e3c2dbb00034a46ef2c73f5739383c6cdb743a6eb9799b33f9e200358f6e8aa"},"schema_version":"1.0","source":{"id":"1207.3352","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1207.3352","created_at":"2026-05-18T03:22:39Z"},{"alias_kind":"arxiv_version","alias_value":"1207.3352v2","created_at":"2026-05-18T03:22:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.3352","created_at":"2026-05-18T03:22:39Z"},{"alias_kind":"pith_short_12","alias_value":"UQTTCJD6DKWN","created_at":"2026-05-18T12:27:23Z"},{"alias_kind":"pith_short_16","alias_value":"UQTTCJD6DKWN7VPO","created_at":"2026-05-18T12:27:23Z"},{"alias_kind":"pith_short_8","alias_value":"UQTTCJD6","created_at":"2026-05-18T12:27:23Z"}],"graph_snapshots":[{"event_id":"sha256:7103d0c376a1bfdd90ae92cc678250255317e185c53df7750e1e741944d59a2b","target":"graph","created_at":"2026-05-18T03:22:39Z","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 investigate and classify Fermi surface behavior for a set of fermionic modes in a family of backgrounds holographically dual to N=4 Super-Yang-Mills theory at zero temperature with two distinct chemical potentials. We numerically solve fluctuation equations for every spin-1/2 field in five-dimensional maximally supersymmetric gauged supergravity not mixing with gravitini. Different modes manifest two, one or zero Fermi surface singularities, all associated to non-Fermi liquids, and we calculate dispersion relations and widths of excitations. We study two limits where the zero-temperature en","authors_text":"Christopher Rosen, Oliver DeWolfe, Steven S. Gubser","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-07-13T20:00:01Z","title":"Fermi surfaces in N=4 Super-Yang-Mills theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.3352","kind":"arxiv","version":2},"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":"sha256:4996a20fe66cf1bd2e7bffd576e4aa193703cea65060b3da1a57417fd657ae00","target":"record","created_at":"2026-05-18T03:22:39Z","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":"a53a6ce3503a9d57df69201d5ba0a7219232401e60738c2770bd229194b4e09f","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-07-13T20:00:01Z","title_canon_sha256":"8e3c2dbb00034a46ef2c73f5739383c6cdb743a6eb9799b33f9e200358f6e8aa"},"schema_version":"1.0","source":{"id":"1207.3352","kind":"arxiv","version":2}},"canonical_sha256":"a42731247e1aacdfd5ee0a5742a9ac2e6e27edc2f21b2baf98067a4fd1b04b00","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a42731247e1aacdfd5ee0a5742a9ac2e6e27edc2f21b2baf98067a4fd1b04b00","first_computed_at":"2026-05-18T03:22:39.269284Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:22:39.269284Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"T7/ByxepHofkixJebUGloFj4FHaOhGMJoYkIf1riR+ooFQUHz9SMbEQdgzYJFPlCF608STHQ7PbtLa6ouavcDg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:22:39.269925Z","signed_message":"canonical_sha256_bytes"},"source_id":"1207.3352","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4996a20fe66cf1bd2e7bffd576e4aa193703cea65060b3da1a57417fd657ae00","sha256:7103d0c376a1bfdd90ae92cc678250255317e185c53df7750e1e741944d59a2b"],"state_sha256":"eef5a83b618bb29f9e653cd114ea75df80f64431e8859ddd871bac44a88fb938"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LzfNYUhWAeeCn/Vp3bSjjWGvNbx6OGxxVfbXHJq3t1siPOLgSPoqMc4G0aWE9gWr1Y8WnJBfecoCfQL+SiA7AA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-29T14:50:58.595872Z","bundle_sha256":"9af893d972146c431541dd3e2da7cd1c92e0ce0b239ddd1219d0df5116b93dbb"}}