{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:FJ6BIP4B5DVAF5H7FYQWGNLL7B","short_pith_number":"pith:FJ6BIP4B","canonical_record":{"source":{"id":"1206.4719","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-06-20T20:58:49Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"8608bb315c1f82620abf5551ef8247e226f57d25c1720b37fe4f66fbe440843a","abstract_canon_sha256":"77b9f861ea41fb355d183a5a211fdaa400cbf568258866aa25fb80532c4ec819"},"schema_version":"1.0"},"canonical_sha256":"2a7c143f81e8ea02f4ff2e2163356bf8485f3d15c7973649de34bdde1353e3e2","source":{"kind":"arxiv","id":"1206.4719","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1206.4719","created_at":"2026-05-18T03:45:31Z"},{"alias_kind":"arxiv_version","alias_value":"1206.4719v1","created_at":"2026-05-18T03:45:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1206.4719","created_at":"2026-05-18T03:45:31Z"},{"alias_kind":"pith_short_12","alias_value":"FJ6BIP4B5DVA","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_16","alias_value":"FJ6BIP4B5DVAF5H7","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_8","alias_value":"FJ6BIP4B","created_at":"2026-05-18T12:27:06Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:FJ6BIP4B5DVAF5H7FYQWGNLL7B","target":"record","payload":{"canonical_record":{"source":{"id":"1206.4719","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-06-20T20:58:49Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"8608bb315c1f82620abf5551ef8247e226f57d25c1720b37fe4f66fbe440843a","abstract_canon_sha256":"77b9f861ea41fb355d183a5a211fdaa400cbf568258866aa25fb80532c4ec819"},"schema_version":"1.0"},"canonical_sha256":"2a7c143f81e8ea02f4ff2e2163356bf8485f3d15c7973649de34bdde1353e3e2","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:45:31.495775Z","signature_b64":"nN4AmqMim7cfddBo1C3B2I2x4iFxWOTHAuQrI/yHyi8vGf07WjShOiPCZ4WvQyGPXWt/LeybIiZ6xEayK77sAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2a7c143f81e8ea02f4ff2e2163356bf8485f3d15c7973649de34bdde1353e3e2","last_reissued_at":"2026-05-18T03:45:31.494953Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:45:31.494953Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1206.4719","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":"2026-05-18T03:45:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"G3H7K8KRIGDwMYMEsAExUj3tqUAZ9IZvlio3gYDjmHtSEiHPk1a4iPb7xfiJy1ApvVxPYFPZl3Y9daNXZniWBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T04:55:10.051907Z"},"content_sha256":"9f704eb6d78239dfd9b86f1238881aebfd8213258f84898db78ca833e758c2f9","schema_version":"1.0","event_id":"sha256:9f704eb6d78239dfd9b86f1238881aebfd8213258f84898db78ca833e758c2f9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:FJ6BIP4B5DVAF5H7FYQWGNLL7B","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Strange Metals in One Spatial Dimension","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"hep-th","authors_text":"Akikazu Hashimoto, Igor R. Klebanov, Kareljan Schoutens, Rajesh Gopakumar, Subir Sachdev","submitted_at":"2012-06-20T20:58:49Z","abstract_excerpt":"We consider 1+1 dimensional SU(N) gauge theory coupled to a multiplet of massive Dirac fermions transforming in the adjoint representation of the gauge group. The only global symmetry of this theory is a U(1) associated with the conserved Dirac fermion number, and we study the theory at variable, non-zero densities. The high density limit is characterized by a deconfined Fermi surface state with Fermi wavevector equal to that of free gauge-charged fermions. Its low energy fluctuations are described by a coset conformal field theory with central charge c=(N^2-1)/3 and an emergent N=(2,2) supers"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1206.4719","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":"2026-05-18T03:45:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wivWprV0/rARVCk69us29lcy8LiFsJvI1wDITXcssJfwrBb7RwjmrWTRSuTFL/m9SMJV6sqvb2Vtf+MHLtXWAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T04:55:10.052628Z"},"content_sha256":"37a842626855d42043987d7cf1443edd487cf12c53fb186c584c443a6021e95b","schema_version":"1.0","event_id":"sha256:37a842626855d42043987d7cf1443edd487cf12c53fb186c584c443a6021e95b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FJ6BIP4B5DVAF5H7FYQWGNLL7B/bundle.json","state_url":"https://pith.science/pith/FJ6BIP4B5DVAF5H7FYQWGNLL7B/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FJ6BIP4B5DVAF5H7FYQWGNLL7B/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":"2026-06-09T04:55:10Z","links":{"resolver":"https://pith.science/pith/FJ6BIP4B5DVAF5H7FYQWGNLL7B","bundle":"https://pith.science/pith/FJ6BIP4B5DVAF5H7FYQWGNLL7B/bundle.json","state":"https://pith.science/pith/FJ6BIP4B5DVAF5H7FYQWGNLL7B/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FJ6BIP4B5DVAF5H7FYQWGNLL7B/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:FJ6BIP4B5DVAF5H7FYQWGNLL7B","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":"77b9f861ea41fb355d183a5a211fdaa400cbf568258866aa25fb80532c4ec819","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-06-20T20:58:49Z","title_canon_sha256":"8608bb315c1f82620abf5551ef8247e226f57d25c1720b37fe4f66fbe440843a"},"schema_version":"1.0","source":{"id":"1206.4719","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1206.4719","created_at":"2026-05-18T03:45:31Z"},{"alias_kind":"arxiv_version","alias_value":"1206.4719v1","created_at":"2026-05-18T03:45:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1206.4719","created_at":"2026-05-18T03:45:31Z"},{"alias_kind":"pith_short_12","alias_value":"FJ6BIP4B5DVA","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_16","alias_value":"FJ6BIP4B5DVAF5H7","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_8","alias_value":"FJ6BIP4B","created_at":"2026-05-18T12:27:06Z"}],"graph_snapshots":[{"event_id":"sha256:37a842626855d42043987d7cf1443edd487cf12c53fb186c584c443a6021e95b","target":"graph","created_at":"2026-05-18T03:45:31Z","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 consider 1+1 dimensional SU(N) gauge theory coupled to a multiplet of massive Dirac fermions transforming in the adjoint representation of the gauge group. The only global symmetry of this theory is a U(1) associated with the conserved Dirac fermion number, and we study the theory at variable, non-zero densities. The high density limit is characterized by a deconfined Fermi surface state with Fermi wavevector equal to that of free gauge-charged fermions. Its low energy fluctuations are described by a coset conformal field theory with central charge c=(N^2-1)/3 and an emergent N=(2,2) supers","authors_text":"Akikazu Hashimoto, Igor R. Klebanov, Kareljan Schoutens, Rajesh Gopakumar, Subir Sachdev","cross_cats":["cond-mat.str-el"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-06-20T20:58:49Z","title":"Strange Metals in One Spatial Dimension"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1206.4719","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":"sha256:9f704eb6d78239dfd9b86f1238881aebfd8213258f84898db78ca833e758c2f9","target":"record","created_at":"2026-05-18T03:45:31Z","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":"77b9f861ea41fb355d183a5a211fdaa400cbf568258866aa25fb80532c4ec819","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-06-20T20:58:49Z","title_canon_sha256":"8608bb315c1f82620abf5551ef8247e226f57d25c1720b37fe4f66fbe440843a"},"schema_version":"1.0","source":{"id":"1206.4719","kind":"arxiv","version":1}},"canonical_sha256":"2a7c143f81e8ea02f4ff2e2163356bf8485f3d15c7973649de34bdde1353e3e2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2a7c143f81e8ea02f4ff2e2163356bf8485f3d15c7973649de34bdde1353e3e2","first_computed_at":"2026-05-18T03:45:31.494953Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:45:31.494953Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"nN4AmqMim7cfddBo1C3B2I2x4iFxWOTHAuQrI/yHyi8vGf07WjShOiPCZ4WvQyGPXWt/LeybIiZ6xEayK77sAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:45:31.495775Z","signed_message":"canonical_sha256_bytes"},"source_id":"1206.4719","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9f704eb6d78239dfd9b86f1238881aebfd8213258f84898db78ca833e758c2f9","sha256:37a842626855d42043987d7cf1443edd487cf12c53fb186c584c443a6021e95b"],"state_sha256":"dfcb08ccab7b2077ac2e1a7fb33b515d0784bffec5291339976d9cb5dffe2d0f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"H1b12gRymDoJLTPDcxyi8idpU6Hz9aBHJeWQmZn4a/BwncoEiNxCb02HAapslkEFgKJ1MgUJYz+5ruDJ1cfSBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-09T04:55:10.056333Z","bundle_sha256":"2b930fe89c3fc9d298f98a9bc7cc02acc8d9c98cadd4f3da7ef004d71a25dd79"}}