{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:4DFWRGJCLAHS4JIQI7OQJ4XB4W","short_pith_number":"pith:4DFWRGJC","canonical_record":{"source":{"id":"1610.09752","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-10-31T01:02:03Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"8e5a52d00d57cf1cb87a6563bc2900621725f155082bc6c6daad6b2c79367bea","abstract_canon_sha256":"b2fb9186916b57d86503a466cc0efaf3e85e357bfedea2e0cc4345c626704cd2"},"schema_version":"1.0"},"canonical_sha256":"e0cb689922580f2e251047dd04f2e1e588a2de96faafc9f4f3fbd02fae1afcb9","source":{"kind":"arxiv","id":"1610.09752","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1610.09752","created_at":"2026-05-18T00:38:21Z"},{"alias_kind":"arxiv_version","alias_value":"1610.09752v1","created_at":"2026-05-18T00:38:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.09752","created_at":"2026-05-18T00:38:21Z"},{"alias_kind":"pith_short_12","alias_value":"4DFWRGJCLAHS","created_at":"2026-05-18T12:29:58Z"},{"alias_kind":"pith_short_16","alias_value":"4DFWRGJCLAHS4JIQ","created_at":"2026-05-18T12:29:58Z"},{"alias_kind":"pith_short_8","alias_value":"4DFWRGJC","created_at":"2026-05-18T12:29:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:4DFWRGJCLAHS4JIQI7OQJ4XB4W","target":"record","payload":{"canonical_record":{"source":{"id":"1610.09752","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-10-31T01:02:03Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"8e5a52d00d57cf1cb87a6563bc2900621725f155082bc6c6daad6b2c79367bea","abstract_canon_sha256":"b2fb9186916b57d86503a466cc0efaf3e85e357bfedea2e0cc4345c626704cd2"},"schema_version":"1.0"},"canonical_sha256":"e0cb689922580f2e251047dd04f2e1e588a2de96faafc9f4f3fbd02fae1afcb9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:38:21.152221Z","signature_b64":"Ilfo/FbTw4xvtn04ZTwBuFErqf70/lvveIMEXvvJfA4rXyO8xPufYb/E65Fx9rySM24s+cSrpZh2zEVwzDeyAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e0cb689922580f2e251047dd04f2e1e588a2de96faafc9f4f3fbd02fae1afcb9","last_reissued_at":"2026-05-18T00:38:21.151687Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:38:21.151687Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1610.09752","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":"2026-05-18T00:38:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qFMcYSUfsoFdWn2w+9/T1POdDLcqzzNRYSeBB5puoLpYnWCsnooUd1SVrBD7k33I+MS8mpkCC/A0xdDZeGkBDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T21:58:25.723280Z"},"content_sha256":"cab1ee1f0a596aede4d78e8e8b0223b8e20c49d1f8e7a093b6c3d14c73d21f64","schema_version":"1.0","event_id":"sha256:cab1ee1f0a596aede4d78e8e8b0223b8e20c49d1f8e7a093b6c3d14c73d21f64"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:4DFWRGJCLAHS4JIQI7OQJ4XB4W","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Universal Critical Behaviors in Non-Hermitian Phase Transitions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"quant-ph","authors_text":"Bo-Bo Wei, Liang Jin","submitted_at":"2016-10-31T01:02:03Z","abstract_excerpt":"Quantum phase transitions also occur in non-Hermitian systems. In this work we show that density functional theory, for the first time, uncovers universal behaviors for phase transitions in non-Hermitian many-body systems. To be specific, we first prove that the non-degenerate steady state of a non-Hermitian quantum many-body system is a universal function of the first derivative of the steady state energy with respect to the control parameter. This finding has far-reaching consequences for non-Hermitian systems: (i) It bridges the nonanalytic behavior in physical observable and nonanalytic be"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.09752","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":"2026-05-18T00:38:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XD1+5mpdfwk/QsfIXTuDXLMIpygm3jwlWYk69tGnU0DXpRF5UrGwqK/NN4/pi6FWVt1Fmb9tFRDv3wvHdCpnDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T21:58:25.723648Z"},"content_sha256":"f1ae99aab45f12f11a5b65e0a93096641124dc7a2537a83954fdd9c7b5340ebf","schema_version":"1.0","event_id":"sha256:f1ae99aab45f12f11a5b65e0a93096641124dc7a2537a83954fdd9c7b5340ebf"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4DFWRGJCLAHS4JIQI7OQJ4XB4W/bundle.json","state_url":"https://pith.science/pith/4DFWRGJCLAHS4JIQI7OQJ4XB4W/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4DFWRGJCLAHS4JIQI7OQJ4XB4W/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":"2026-06-04T21:58:25Z","links":{"resolver":"https://pith.science/pith/4DFWRGJCLAHS4JIQI7OQJ4XB4W","bundle":"https://pith.science/pith/4DFWRGJCLAHS4JIQI7OQJ4XB4W/bundle.json","state":"https://pith.science/pith/4DFWRGJCLAHS4JIQI7OQJ4XB4W/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4DFWRGJCLAHS4JIQI7OQJ4XB4W/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:4DFWRGJCLAHS4JIQI7OQJ4XB4W","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":"b2fb9186916b57d86503a466cc0efaf3e85e357bfedea2e0cc4345c626704cd2","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-10-31T01:02:03Z","title_canon_sha256":"8e5a52d00d57cf1cb87a6563bc2900621725f155082bc6c6daad6b2c79367bea"},"schema_version":"1.0","source":{"id":"1610.09752","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1610.09752","created_at":"2026-05-18T00:38:21Z"},{"alias_kind":"arxiv_version","alias_value":"1610.09752v1","created_at":"2026-05-18T00:38:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.09752","created_at":"2026-05-18T00:38:21Z"},{"alias_kind":"pith_short_12","alias_value":"4DFWRGJCLAHS","created_at":"2026-05-18T12:29:58Z"},{"alias_kind":"pith_short_16","alias_value":"4DFWRGJCLAHS4JIQ","created_at":"2026-05-18T12:29:58Z"},{"alias_kind":"pith_short_8","alias_value":"4DFWRGJC","created_at":"2026-05-18T12:29:58Z"}],"graph_snapshots":[{"event_id":"sha256:f1ae99aab45f12f11a5b65e0a93096641124dc7a2537a83954fdd9c7b5340ebf","target":"graph","created_at":"2026-05-18T00:38:21Z","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":"Quantum phase transitions also occur in non-Hermitian systems. In this work we show that density functional theory, for the first time, uncovers universal behaviors for phase transitions in non-Hermitian many-body systems. To be specific, we first prove that the non-degenerate steady state of a non-Hermitian quantum many-body system is a universal function of the first derivative of the steady state energy with respect to the control parameter. This finding has far-reaching consequences for non-Hermitian systems: (i) It bridges the nonanalytic behavior in physical observable and nonanalytic be","authors_text":"Bo-Bo Wei, Liang Jin","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-10-31T01:02:03Z","title":"Universal Critical Behaviors in Non-Hermitian Phase Transitions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.09752","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:cab1ee1f0a596aede4d78e8e8b0223b8e20c49d1f8e7a093b6c3d14c73d21f64","target":"record","created_at":"2026-05-18T00:38:21Z","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":"b2fb9186916b57d86503a466cc0efaf3e85e357bfedea2e0cc4345c626704cd2","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-10-31T01:02:03Z","title_canon_sha256":"8e5a52d00d57cf1cb87a6563bc2900621725f155082bc6c6daad6b2c79367bea"},"schema_version":"1.0","source":{"id":"1610.09752","kind":"arxiv","version":1}},"canonical_sha256":"e0cb689922580f2e251047dd04f2e1e588a2de96faafc9f4f3fbd02fae1afcb9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e0cb689922580f2e251047dd04f2e1e588a2de96faafc9f4f3fbd02fae1afcb9","first_computed_at":"2026-05-18T00:38:21.151687Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:38:21.151687Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Ilfo/FbTw4xvtn04ZTwBuFErqf70/lvveIMEXvvJfA4rXyO8xPufYb/E65Fx9rySM24s+cSrpZh2zEVwzDeyAg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:38:21.152221Z","signed_message":"canonical_sha256_bytes"},"source_id":"1610.09752","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cab1ee1f0a596aede4d78e8e8b0223b8e20c49d1f8e7a093b6c3d14c73d21f64","sha256:f1ae99aab45f12f11a5b65e0a93096641124dc7a2537a83954fdd9c7b5340ebf"],"state_sha256":"f7a11f617c1d34b3c16ac9052d4bac97248f61a7dfb1dbc53fef59bc21620c3a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YTAegqXJSH3bU8U1dCwHSdLhrLbLHQj6DtWXYDoyHwU4VL6D4lKKYOnvyYZy3+IS3HanagqkUv2O+vyb8g81Aw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-04T21:58:25.725791Z","bundle_sha256":"37844dbb05a275928fdfc0a6344cfce1e370085286c48619ad4bd51abeb3df0e"}}