{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:QQ5CLMJV4UFI4OPZHWVJAGCATB","short_pith_number":"pith:QQ5CLMJV","canonical_record":{"source":{"id":"1606.00452","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2016-06-01T20:01:06Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"4323934872e1b95a232eaf5ec259b1088c7565eb4959e73ff2f8bad9f283c05b","abstract_canon_sha256":"b1820adf819ad469ab9dbb65f1c179ff2598b35ec7cac6804465fbb680d87055"},"schema_version":"1.0"},"canonical_sha256":"843a25b135e50a8e39f93daa9018409864e6e137015c13735a50d87f2b4f191c","source":{"kind":"arxiv","id":"1606.00452","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1606.00452","created_at":"2026-05-18T01:05:42Z"},{"alias_kind":"arxiv_version","alias_value":"1606.00452v2","created_at":"2026-05-18T01:05:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1606.00452","created_at":"2026-05-18T01:05:42Z"},{"alias_kind":"pith_short_12","alias_value":"QQ5CLMJV4UFI","created_at":"2026-05-18T12:30:41Z"},{"alias_kind":"pith_short_16","alias_value":"QQ5CLMJV4UFI4OPZ","created_at":"2026-05-18T12:30:41Z"},{"alias_kind":"pith_short_8","alias_value":"QQ5CLMJV","created_at":"2026-05-18T12:30:41Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:QQ5CLMJV4UFI4OPZHWVJAGCATB","target":"record","payload":{"canonical_record":{"source":{"id":"1606.00452","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2016-06-01T20:01:06Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"4323934872e1b95a232eaf5ec259b1088c7565eb4959e73ff2f8bad9f283c05b","abstract_canon_sha256":"b1820adf819ad469ab9dbb65f1c179ff2598b35ec7cac6804465fbb680d87055"},"schema_version":"1.0"},"canonical_sha256":"843a25b135e50a8e39f93daa9018409864e6e137015c13735a50d87f2b4f191c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:05:42.971528Z","signature_b64":"2JANC5ngwhViMx2FWdG3uzc5R2tVR//xzjZwMjOOLSAKl6sCwHmR2C/Od0PQbk3Zhc/AcsEar7WsOOtyRtjPBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"843a25b135e50a8e39f93daa9018409864e6e137015c13735a50d87f2b4f191c","last_reissued_at":"2026-05-18T01:05:42.970756Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:05:42.970756Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1606.00452","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":"2026-05-18T01:05:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mXd13L0wViEi5gLGqtrTtoY8zhdSEh0FSbT7N0333eEjhXELFu6JHWy6X9VuXSzQ4Inj+MFXraP6Fg/T5vlhAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T03:04:56.956606Z"},"content_sha256":"0a9bc855aaa72fcffdaf34c709127d21aaf8f4bfe4c9a5b42caa9c8615dfa447","schema_version":"1.0","event_id":"sha256:0a9bc855aaa72fcffdaf34c709127d21aaf8f4bfe4c9a5b42caa9c8615dfa447"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:QQ5CLMJV4UFI4OPZHWVJAGCATB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quantum dynamical field theory for non-equilibrium phase transitions in driven open systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.quant-gas","authors_text":"Jamir Marino, Sebastian Diehl","submitted_at":"2016-06-01T20:01:06Z","abstract_excerpt":"We develop a quantum dynamical field theory for studying phase transitions in driven open systems coupled to Markovian noise, where non-linear noise effects and fluctuations beyond semiclassical approximations influence the critical behaviour. We systematically compare the diagrammatics, the properties of the renormalization group flow and the structure of the fixed points, of the novel quantum dynamical field theory and of its semi-classical counterpart, which is employed to characterise dynamical criticality in three dimensional driven-dissipative condensates. As an application, we perform t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1606.00452","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":"2026-05-18T01:05:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FbBHHXZGvBv89JaiV+2kYfCq09N9jOthqIInC98TayGKYOtiFiGmzCmorwjjpcfPcilUt7OknSly7sMzFLFYAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T03:04:56.957274Z"},"content_sha256":"fbb85b87acfe0c0047a81244641e06dfc9b788d8568cf6f0b05c36f0c4e78a88","schema_version":"1.0","event_id":"sha256:fbb85b87acfe0c0047a81244641e06dfc9b788d8568cf6f0b05c36f0c4e78a88"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/QQ5CLMJV4UFI4OPZHWVJAGCATB/bundle.json","state_url":"https://pith.science/pith/QQ5CLMJV4UFI4OPZHWVJAGCATB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/QQ5CLMJV4UFI4OPZHWVJAGCATB/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":"2026-05-27T03:04:56Z","links":{"resolver":"https://pith.science/pith/QQ5CLMJV4UFI4OPZHWVJAGCATB","bundle":"https://pith.science/pith/QQ5CLMJV4UFI4OPZHWVJAGCATB/bundle.json","state":"https://pith.science/pith/QQ5CLMJV4UFI4OPZHWVJAGCATB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/QQ5CLMJV4UFI4OPZHWVJAGCATB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:QQ5CLMJV4UFI4OPZHWVJAGCATB","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":"b1820adf819ad469ab9dbb65f1c179ff2598b35ec7cac6804465fbb680d87055","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2016-06-01T20:01:06Z","title_canon_sha256":"4323934872e1b95a232eaf5ec259b1088c7565eb4959e73ff2f8bad9f283c05b"},"schema_version":"1.0","source":{"id":"1606.00452","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1606.00452","created_at":"2026-05-18T01:05:42Z"},{"alias_kind":"arxiv_version","alias_value":"1606.00452v2","created_at":"2026-05-18T01:05:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1606.00452","created_at":"2026-05-18T01:05:42Z"},{"alias_kind":"pith_short_12","alias_value":"QQ5CLMJV4UFI","created_at":"2026-05-18T12:30:41Z"},{"alias_kind":"pith_short_16","alias_value":"QQ5CLMJV4UFI4OPZ","created_at":"2026-05-18T12:30:41Z"},{"alias_kind":"pith_short_8","alias_value":"QQ5CLMJV","created_at":"2026-05-18T12:30:41Z"}],"graph_snapshots":[{"event_id":"sha256:fbb85b87acfe0c0047a81244641e06dfc9b788d8568cf6f0b05c36f0c4e78a88","target":"graph","created_at":"2026-05-18T01:05:42Z","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 develop a quantum dynamical field theory for studying phase transitions in driven open systems coupled to Markovian noise, where non-linear noise effects and fluctuations beyond semiclassical approximations influence the critical behaviour. We systematically compare the diagrammatics, the properties of the renormalization group flow and the structure of the fixed points, of the novel quantum dynamical field theory and of its semi-classical counterpart, which is employed to characterise dynamical criticality in three dimensional driven-dissipative condensates. As an application, we perform t","authors_text":"Jamir Marino, Sebastian Diehl","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2016-06-01T20:01:06Z","title":"Quantum dynamical field theory for non-equilibrium phase transitions in driven open systems"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1606.00452","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":"sha256:0a9bc855aaa72fcffdaf34c709127d21aaf8f4bfe4c9a5b42caa9c8615dfa447","target":"record","created_at":"2026-05-18T01:05:42Z","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":"b1820adf819ad469ab9dbb65f1c179ff2598b35ec7cac6804465fbb680d87055","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2016-06-01T20:01:06Z","title_canon_sha256":"4323934872e1b95a232eaf5ec259b1088c7565eb4959e73ff2f8bad9f283c05b"},"schema_version":"1.0","source":{"id":"1606.00452","kind":"arxiv","version":2}},"canonical_sha256":"843a25b135e50a8e39f93daa9018409864e6e137015c13735a50d87f2b4f191c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"843a25b135e50a8e39f93daa9018409864e6e137015c13735a50d87f2b4f191c","first_computed_at":"2026-05-18T01:05:42.970756Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:05:42.970756Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"2JANC5ngwhViMx2FWdG3uzc5R2tVR//xzjZwMjOOLSAKl6sCwHmR2C/Od0PQbk3Zhc/AcsEar7WsOOtyRtjPBg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:05:42.971528Z","signed_message":"canonical_sha256_bytes"},"source_id":"1606.00452","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0a9bc855aaa72fcffdaf34c709127d21aaf8f4bfe4c9a5b42caa9c8615dfa447","sha256:fbb85b87acfe0c0047a81244641e06dfc9b788d8568cf6f0b05c36f0c4e78a88"],"state_sha256":"9d09c2c11766789ea63c978e796b49f062463a09f3f29404cb87b52a0d6d1b54"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hr629YUqc9dbQp5Zvbko4nQwUAS3/MwbzcVGM8EvfLsnBAQF+Zz6BvR+wZMolAYWFRN5AiDAr5jK8s+yx4uFDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T03:04:56.960717Z","bundle_sha256":"c74838762102dfeda865278eebb4bf2aa3360e80d77ce05fbb19eaee73f75626"}}