{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:BX6MAPYC6A6ZECRVECJENHLXIL","short_pith_number":"pith:BX6MAPYC","canonical_record":{"source":{"id":"1809.09737","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2018-09-25T21:43:35Z","cross_cats_sorted":[],"title_canon_sha256":"ee5ed03075296b47d04121c67a9120ec2c3e26a319174faa5dd7051a5c1164e7","abstract_canon_sha256":"07e5ea54dae86725b6f5d97d92a1dca5e9bd6b89c238e039690b092cfc16b851"},"schema_version":"1.0"},"canonical_sha256":"0dfcc03f02f03d920a352092469d7742fd17892ab7d64fbdda8751017b5bfc46","source":{"kind":"arxiv","id":"1809.09737","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1809.09737","created_at":"2026-05-17T23:43:38Z"},{"alias_kind":"arxiv_version","alias_value":"1809.09737v2","created_at":"2026-05-17T23:43:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1809.09737","created_at":"2026-05-17T23:43:38Z"},{"alias_kind":"pith_short_12","alias_value":"BX6MAPYC6A6Z","created_at":"2026-05-18T12:32:16Z"},{"alias_kind":"pith_short_16","alias_value":"BX6MAPYC6A6ZECRV","created_at":"2026-05-18T12:32:16Z"},{"alias_kind":"pith_short_8","alias_value":"BX6MAPYC","created_at":"2026-05-18T12:32:16Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:BX6MAPYC6A6ZECRVECJENHLXIL","target":"record","payload":{"canonical_record":{"source":{"id":"1809.09737","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2018-09-25T21:43:35Z","cross_cats_sorted":[],"title_canon_sha256":"ee5ed03075296b47d04121c67a9120ec2c3e26a319174faa5dd7051a5c1164e7","abstract_canon_sha256":"07e5ea54dae86725b6f5d97d92a1dca5e9bd6b89c238e039690b092cfc16b851"},"schema_version":"1.0"},"canonical_sha256":"0dfcc03f02f03d920a352092469d7742fd17892ab7d64fbdda8751017b5bfc46","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:43:38.001291Z","signature_b64":"WDTRF+Vs+ywGnQ3oFr0EvaVVHreMe7+nf+x1sG8vbjEXVZxxpB7HBTRYmMUteBjju8oyNHLIqKf0mv59V5ohCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0dfcc03f02f03d920a352092469d7742fd17892ab7d64fbdda8751017b5bfc46","last_reissued_at":"2026-05-17T23:43:38.000735Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:43:38.000735Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1809.09737","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":"2026-05-17T23:43:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AnYc6rIJDp5NJMDvpMDCgBJXj6vQdNwABZfWA3zvQuwFydsjPiOnDUSPSPREHPT9LXNKrFUjn0WnCiF+t1SaDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T07:38:13.200017Z"},"content_sha256":"3b07ec3afc3c35a5eb4cc9c9790451fb8ac90d6db94ca2f76782019b1889951b","schema_version":"1.0","event_id":"sha256:3b07ec3afc3c35a5eb4cc9c9790451fb8ac90d6db94ca2f76782019b1889951b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:BX6MAPYC6A6ZECRVECJENHLXIL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Finite-size scaling of the photon-blockade breakdown dissipative quantum phase transition","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"A. Dombi, A. Vukics, J. M. Fink, P. Domokos","submitted_at":"2018-09-25T21:43:35Z","abstract_excerpt":"We prove that the observable telegraph signal accompanying the bistability in the photon-blockade-breakdown regime of the driven and lossy Jaynes--Cummings model is the finite-size precursor of what in the thermodynamic limit is a genuine first-order phase transition. We construct a finite-size scaling of the system parameters to a well-defined thermodynamic limit, in which the system remains the same microscopic system, but the telegraph signal becomes macroscopic both in its timescale and intensity. The existence of such a finite-size scaling completes and justifies the classification of the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1809.09737","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":"2026-05-17T23:43:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DMzFuHEnTgU8qtOJ5LI1c7WepxWWQ6ET/G3q0S2Fsx+ZZj55MmAKzVklsnwrAIZZGwrHfJ+svaq739he2/pFAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T07:38:13.200381Z"},"content_sha256":"77994ebbc7203caa9c4cffdbb7f34ba4c4d75aeaaa57f797061d37d55c36ad5d","schema_version":"1.0","event_id":"sha256:77994ebbc7203caa9c4cffdbb7f34ba4c4d75aeaaa57f797061d37d55c36ad5d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/BX6MAPYC6A6ZECRVECJENHLXIL/bundle.json","state_url":"https://pith.science/pith/BX6MAPYC6A6ZECRVECJENHLXIL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/BX6MAPYC6A6ZECRVECJENHLXIL/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":"2026-05-28T07:38:13Z","links":{"resolver":"https://pith.science/pith/BX6MAPYC6A6ZECRVECJENHLXIL","bundle":"https://pith.science/pith/BX6MAPYC6A6ZECRVECJENHLXIL/bundle.json","state":"https://pith.science/pith/BX6MAPYC6A6ZECRVECJENHLXIL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/BX6MAPYC6A6ZECRVECJENHLXIL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:BX6MAPYC6A6ZECRVECJENHLXIL","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":"07e5ea54dae86725b6f5d97d92a1dca5e9bd6b89c238e039690b092cfc16b851","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2018-09-25T21:43:35Z","title_canon_sha256":"ee5ed03075296b47d04121c67a9120ec2c3e26a319174faa5dd7051a5c1164e7"},"schema_version":"1.0","source":{"id":"1809.09737","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1809.09737","created_at":"2026-05-17T23:43:38Z"},{"alias_kind":"arxiv_version","alias_value":"1809.09737v2","created_at":"2026-05-17T23:43:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1809.09737","created_at":"2026-05-17T23:43:38Z"},{"alias_kind":"pith_short_12","alias_value":"BX6MAPYC6A6Z","created_at":"2026-05-18T12:32:16Z"},{"alias_kind":"pith_short_16","alias_value":"BX6MAPYC6A6ZECRV","created_at":"2026-05-18T12:32:16Z"},{"alias_kind":"pith_short_8","alias_value":"BX6MAPYC","created_at":"2026-05-18T12:32:16Z"}],"graph_snapshots":[{"event_id":"sha256:77994ebbc7203caa9c4cffdbb7f34ba4c4d75aeaaa57f797061d37d55c36ad5d","target":"graph","created_at":"2026-05-17T23:43:38Z","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 prove that the observable telegraph signal accompanying the bistability in the photon-blockade-breakdown regime of the driven and lossy Jaynes--Cummings model is the finite-size precursor of what in the thermodynamic limit is a genuine first-order phase transition. We construct a finite-size scaling of the system parameters to a well-defined thermodynamic limit, in which the system remains the same microscopic system, but the telegraph signal becomes macroscopic both in its timescale and intensity. The existence of such a finite-size scaling completes and justifies the classification of the","authors_text":"A. Dombi, A. Vukics, J. M. Fink, P. Domokos","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2018-09-25T21:43:35Z","title":"Finite-size scaling of the photon-blockade breakdown dissipative quantum phase transition"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1809.09737","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":"sha256:3b07ec3afc3c35a5eb4cc9c9790451fb8ac90d6db94ca2f76782019b1889951b","target":"record","created_at":"2026-05-17T23:43:38Z","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":"07e5ea54dae86725b6f5d97d92a1dca5e9bd6b89c238e039690b092cfc16b851","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2018-09-25T21:43:35Z","title_canon_sha256":"ee5ed03075296b47d04121c67a9120ec2c3e26a319174faa5dd7051a5c1164e7"},"schema_version":"1.0","source":{"id":"1809.09737","kind":"arxiv","version":2}},"canonical_sha256":"0dfcc03f02f03d920a352092469d7742fd17892ab7d64fbdda8751017b5bfc46","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0dfcc03f02f03d920a352092469d7742fd17892ab7d64fbdda8751017b5bfc46","first_computed_at":"2026-05-17T23:43:38.000735Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:43:38.000735Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"WDTRF+Vs+ywGnQ3oFr0EvaVVHreMe7+nf+x1sG8vbjEXVZxxpB7HBTRYmMUteBjju8oyNHLIqKf0mv59V5ohCg==","signature_status":"signed_v1","signed_at":"2026-05-17T23:43:38.001291Z","signed_message":"canonical_sha256_bytes"},"source_id":"1809.09737","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3b07ec3afc3c35a5eb4cc9c9790451fb8ac90d6db94ca2f76782019b1889951b","sha256:77994ebbc7203caa9c4cffdbb7f34ba4c4d75aeaaa57f797061d37d55c36ad5d"],"state_sha256":"edae09ad8c00ed5196d02f7c9351b91c4b841685ab107f0be79061d6bd224ed2"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qlPmDZN8m+KQE0B4BXypu3r1ZW8gnPyeJeh46IK7FQ/h9/0Zo2vd9yPndidFEnBB1NTqcNxiOjs7toQo38XyAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T07:38:13.202466Z","bundle_sha256":"997ebd44896769b42fffdd519742ac17eb746fc94dc50308562228394ff31eac"}}