{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:RBMOWUCVMOU72FBLR6KS3UF4ML","short_pith_number":"pith:RBMOWUCV","canonical_record":{"source":{"id":"1312.7347","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-12-27T21:00:01Z","cross_cats_sorted":[],"title_canon_sha256":"5c720dd1628a7ac379c85178329339143d1ed01bfe94e4cf8b30f0308f2941f5","abstract_canon_sha256":"10b357df4a1b823c46d6332ee2c0641986b1cf147030862d740f37a3eb7ae242"},"schema_version":"1.0"},"canonical_sha256":"8858eb505563a9fd142b8f952dd0bc62c9eb07b5c7e5163b5d63255a83722b70","source":{"kind":"arxiv","id":"1312.7347","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1312.7347","created_at":"2026-05-18T02:25:47Z"},{"alias_kind":"arxiv_version","alias_value":"1312.7347v1","created_at":"2026-05-18T02:25:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.7347","created_at":"2026-05-18T02:25:47Z"},{"alias_kind":"pith_short_12","alias_value":"RBMOWUCVMOU7","created_at":"2026-05-18T12:27:57Z"},{"alias_kind":"pith_short_16","alias_value":"RBMOWUCVMOU72FBL","created_at":"2026-05-18T12:27:57Z"},{"alias_kind":"pith_short_8","alias_value":"RBMOWUCV","created_at":"2026-05-18T12:27:57Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:RBMOWUCVMOU72FBLR6KS3UF4ML","target":"record","payload":{"canonical_record":{"source":{"id":"1312.7347","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-12-27T21:00:01Z","cross_cats_sorted":[],"title_canon_sha256":"5c720dd1628a7ac379c85178329339143d1ed01bfe94e4cf8b30f0308f2941f5","abstract_canon_sha256":"10b357df4a1b823c46d6332ee2c0641986b1cf147030862d740f37a3eb7ae242"},"schema_version":"1.0"},"canonical_sha256":"8858eb505563a9fd142b8f952dd0bc62c9eb07b5c7e5163b5d63255a83722b70","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:25:47.527070Z","signature_b64":"KBkmVAJmj4deEotoNDtFycDzN7/40CT78j03wKpm+SrhV8t2qry8f718mDhWXsKarZQGyxjkOYPwQM6zLaWOBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8858eb505563a9fd142b8f952dd0bc62c9eb07b5c7e5163b5d63255a83722b70","last_reissued_at":"2026-05-18T02:25:47.526566Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:25:47.526566Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1312.7347","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":"2026-05-18T02:25:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Gc6nh7yxTp05wRnPd1TTrUmgL9/7ZDStI6XP+nH2yuU+XT/5necWMX81xm7TGv12yQ6XFiSxqGxXlCCbyJ4lBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T14:48:53.961583Z"},"content_sha256":"a07f1b9a11d3e53214d9d39a99d8f25e70762b3dc23cde083a0fc1a1508cfaf1","schema_version":"1.0","event_id":"sha256:a07f1b9a11d3e53214d9d39a99d8f25e70762b3dc23cde083a0fc1a1508cfaf1"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:RBMOWUCVMOU72FBLR6KS3UF4ML","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Minding the Gap in N=4 Super-Yang-Mills","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":"2013-12-27T21:00:01Z","abstract_excerpt":"We analyze fermionic response in the geometry holographically dual to zero-temperature N=4 Super-Yang-Mills theory with two equal nonvanishing chemical potentials, which is characterized by a singular horizon and zero ground state entropy. We show that fermionic fluctuations are completely stable within a gap in energy around a Fermi surface singularity, beyond which non-Fermi liquid behavior returns. This gap disappears abruptly once the final charge is turned on, and is associated to a discontinuity in the corresponding chemical potential. We also show that the singular near-horizon geometry"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.7347","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":"2026-05-18T02:25:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DuYMvNEWOBWrzxYF4HqE+fxcI/i/lnbdtg5Z3n96bcCTSFS5I9EitSbSWiBp37xdI0VduLZIVj/rQxzokI+iDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T14:48:53.962240Z"},"content_sha256":"2a8f2fa6f33362b8c20fcbe04e8316da16e39ff20ce050bca59f49ba58232899","schema_version":"1.0","event_id":"sha256:2a8f2fa6f33362b8c20fcbe04e8316da16e39ff20ce050bca59f49ba58232899"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RBMOWUCVMOU72FBLR6KS3UF4ML/bundle.json","state_url":"https://pith.science/pith/RBMOWUCVMOU72FBLR6KS3UF4ML/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RBMOWUCVMOU72FBLR6KS3UF4ML/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":"2026-05-29T14:48:53Z","links":{"resolver":"https://pith.science/pith/RBMOWUCVMOU72FBLR6KS3UF4ML","bundle":"https://pith.science/pith/RBMOWUCVMOU72FBLR6KS3UF4ML/bundle.json","state":"https://pith.science/pith/RBMOWUCVMOU72FBLR6KS3UF4ML/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RBMOWUCVMOU72FBLR6KS3UF4ML/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:RBMOWUCVMOU72FBLR6KS3UF4ML","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":"10b357df4a1b823c46d6332ee2c0641986b1cf147030862d740f37a3eb7ae242","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-12-27T21:00:01Z","title_canon_sha256":"5c720dd1628a7ac379c85178329339143d1ed01bfe94e4cf8b30f0308f2941f5"},"schema_version":"1.0","source":{"id":"1312.7347","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1312.7347","created_at":"2026-05-18T02:25:47Z"},{"alias_kind":"arxiv_version","alias_value":"1312.7347v1","created_at":"2026-05-18T02:25:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.7347","created_at":"2026-05-18T02:25:47Z"},{"alias_kind":"pith_short_12","alias_value":"RBMOWUCVMOU7","created_at":"2026-05-18T12:27:57Z"},{"alias_kind":"pith_short_16","alias_value":"RBMOWUCVMOU72FBL","created_at":"2026-05-18T12:27:57Z"},{"alias_kind":"pith_short_8","alias_value":"RBMOWUCV","created_at":"2026-05-18T12:27:57Z"}],"graph_snapshots":[{"event_id":"sha256:2a8f2fa6f33362b8c20fcbe04e8316da16e39ff20ce050bca59f49ba58232899","target":"graph","created_at":"2026-05-18T02:25:47Z","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 analyze fermionic response in the geometry holographically dual to zero-temperature N=4 Super-Yang-Mills theory with two equal nonvanishing chemical potentials, which is characterized by a singular horizon and zero ground state entropy. We show that fermionic fluctuations are completely stable within a gap in energy around a Fermi surface singularity, beyond which non-Fermi liquid behavior returns. This gap disappears abruptly once the final charge is turned on, and is associated to a discontinuity in the corresponding chemical potential. We also show that the singular near-horizon geometry","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":"2013-12-27T21:00:01Z","title":"Minding the Gap in N=4 Super-Yang-Mills"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.7347","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:a07f1b9a11d3e53214d9d39a99d8f25e70762b3dc23cde083a0fc1a1508cfaf1","target":"record","created_at":"2026-05-18T02:25:47Z","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":"10b357df4a1b823c46d6332ee2c0641986b1cf147030862d740f37a3eb7ae242","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-12-27T21:00:01Z","title_canon_sha256":"5c720dd1628a7ac379c85178329339143d1ed01bfe94e4cf8b30f0308f2941f5"},"schema_version":"1.0","source":{"id":"1312.7347","kind":"arxiv","version":1}},"canonical_sha256":"8858eb505563a9fd142b8f952dd0bc62c9eb07b5c7e5163b5d63255a83722b70","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8858eb505563a9fd142b8f952dd0bc62c9eb07b5c7e5163b5d63255a83722b70","first_computed_at":"2026-05-18T02:25:47.526566Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:25:47.526566Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"KBkmVAJmj4deEotoNDtFycDzN7/40CT78j03wKpm+SrhV8t2qry8f718mDhWXsKarZQGyxjkOYPwQM6zLaWOBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:25:47.527070Z","signed_message":"canonical_sha256_bytes"},"source_id":"1312.7347","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a07f1b9a11d3e53214d9d39a99d8f25e70762b3dc23cde083a0fc1a1508cfaf1","sha256:2a8f2fa6f33362b8c20fcbe04e8316da16e39ff20ce050bca59f49ba58232899"],"state_sha256":"54a67b1c03f886034435d91a4376438e94f2aa289541d6263b120fcb31d9e8a7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IAQoZn8m88gL5xmx27TFb1AVcKNPv5xS9yTA9Y0kxR13AoihOngyaGpxbuNvKpAlm2jt66FRSzhAXDx+z1NdBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-29T14:48:53.965968Z","bundle_sha256":"f7730101513705c21eb345791ee5cf2300684eefc6ff289bdb817434e804c34c"}}