{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:YNSCI54XRFTKHQH6DVSTMJOTLP","short_pith_number":"pith:YNSCI54X","canonical_record":{"source":{"id":"1708.08175","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-08-28T03:29:23Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"d1694614813c01e7f63b8fe294090b6f079b0afc5aba1c8e62185e29cc1fe007","abstract_canon_sha256":"ccef2a7117d628b53d0038fc65bbe006179be42116fe0a889b69f3db2c4dff78"},"schema_version":"1.0"},"canonical_sha256":"c3642477978966a3c0fe1d653625d35bedfc7204144ff077e400029e41a1d3e5","source":{"kind":"arxiv","id":"1708.08175","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.08175","created_at":"2026-05-18T00:25:23Z"},{"alias_kind":"arxiv_version","alias_value":"1708.08175v2","created_at":"2026-05-18T00:25:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.08175","created_at":"2026-05-18T00:25:23Z"},{"alias_kind":"pith_short_12","alias_value":"YNSCI54XRFTK","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_16","alias_value":"YNSCI54XRFTKHQH6","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_8","alias_value":"YNSCI54X","created_at":"2026-05-18T12:31:56Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:YNSCI54XRFTKHQH6DVSTMJOTLP","target":"record","payload":{"canonical_record":{"source":{"id":"1708.08175","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-08-28T03:29:23Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"d1694614813c01e7f63b8fe294090b6f079b0afc5aba1c8e62185e29cc1fe007","abstract_canon_sha256":"ccef2a7117d628b53d0038fc65bbe006179be42116fe0a889b69f3db2c4dff78"},"schema_version":"1.0"},"canonical_sha256":"c3642477978966a3c0fe1d653625d35bedfc7204144ff077e400029e41a1d3e5","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:25:23.544849Z","signature_b64":"pQXOIo5jIM73fOunX0FNFL2xnAL5vybry7TUPFHAn5vEyTT21gVhWeoRPbPNZHCwIIT3FHjyytW2SNCIrcXpBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c3642477978966a3c0fe1d653625d35bedfc7204144ff077e400029e41a1d3e5","last_reissued_at":"2026-05-18T00:25:23.544419Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:25:23.544419Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1708.08175","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":"2026-05-18T00:25:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rAAaPSNmx4Isem0LdNL4GS4isu289b+BCUs81AognRb7WricapS974+B1Z46zFWoS5uooNJ2K+cq8Cllt6kmDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T13:20:33.679179Z"},"content_sha256":"83891658aff77051e138dbe4c6d4761604d50633927d2919479595d0ab090da5","schema_version":"1.0","event_id":"sha256:83891658aff77051e138dbe4c6d4761604d50633927d2919479595d0ab090da5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:YNSCI54XRFTKHQH6DVSTMJOTLP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dissipative Phase Transition in the Open Quantum Rabi Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"quant-ph","authors_text":"Martin B. Plenio, Myung-Joong Hwang, Peter Rabl","submitted_at":"2017-08-28T03:29:23Z","abstract_excerpt":"We demonstrate that the open quantum Rabi model (QRM) exhibits a second-order dissipative phase transition (DPT) and propose a method to observe this transition with trapped ions. The interplay between the ultrastrong qubit-oscillator coupling and the oscillator damping brings the system into a steady-state with a diverging number of excitations, in which a DPT is allowed to occur even with a finite number of system components. The universality class of the open QRM, modified from the closed QRM by a Markovian bath, is identified by finding critical exponents and scaling functions using the Ke"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.08175","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":"2026-05-18T00:25:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jDdbx2W+FTXDUB6tQvRaqfUUeIQxltAUHrOIeyCqT6J9xWCAaFzPAXCk1/Yw2E/ASVmPZRFVHSYHUg5BkObaDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T13:20:33.679862Z"},"content_sha256":"cffad94c09e53fb96db620b5614a2b05d4a1082522fd1d61636031e0c5898afa","schema_version":"1.0","event_id":"sha256:cffad94c09e53fb96db620b5614a2b05d4a1082522fd1d61636031e0c5898afa"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YNSCI54XRFTKHQH6DVSTMJOTLP/bundle.json","state_url":"https://pith.science/pith/YNSCI54XRFTKHQH6DVSTMJOTLP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YNSCI54XRFTKHQH6DVSTMJOTLP/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":"2026-05-25T13:20:33Z","links":{"resolver":"https://pith.science/pith/YNSCI54XRFTKHQH6DVSTMJOTLP","bundle":"https://pith.science/pith/YNSCI54XRFTKHQH6DVSTMJOTLP/bundle.json","state":"https://pith.science/pith/YNSCI54XRFTKHQH6DVSTMJOTLP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YNSCI54XRFTKHQH6DVSTMJOTLP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:YNSCI54XRFTKHQH6DVSTMJOTLP","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":"ccef2a7117d628b53d0038fc65bbe006179be42116fe0a889b69f3db2c4dff78","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-08-28T03:29:23Z","title_canon_sha256":"d1694614813c01e7f63b8fe294090b6f079b0afc5aba1c8e62185e29cc1fe007"},"schema_version":"1.0","source":{"id":"1708.08175","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.08175","created_at":"2026-05-18T00:25:23Z"},{"alias_kind":"arxiv_version","alias_value":"1708.08175v2","created_at":"2026-05-18T00:25:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.08175","created_at":"2026-05-18T00:25:23Z"},{"alias_kind":"pith_short_12","alias_value":"YNSCI54XRFTK","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_16","alias_value":"YNSCI54XRFTKHQH6","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_8","alias_value":"YNSCI54X","created_at":"2026-05-18T12:31:56Z"}],"graph_snapshots":[{"event_id":"sha256:cffad94c09e53fb96db620b5614a2b05d4a1082522fd1d61636031e0c5898afa","target":"graph","created_at":"2026-05-18T00:25:23Z","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 demonstrate that the open quantum Rabi model (QRM) exhibits a second-order dissipative phase transition (DPT) and propose a method to observe this transition with trapped ions. The interplay between the ultrastrong qubit-oscillator coupling and the oscillator damping brings the system into a steady-state with a diverging number of excitations, in which a DPT is allowed to occur even with a finite number of system components. The universality class of the open QRM, modified from the closed QRM by a Markovian bath, is identified by finding critical exponents and scaling functions using the Ke","authors_text":"Martin B. Plenio, Myung-Joong Hwang, Peter Rabl","cross_cats":["cond-mat.mes-hall"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-08-28T03:29:23Z","title":"Dissipative Phase Transition in the Open Quantum Rabi Model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.08175","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":"sha256:83891658aff77051e138dbe4c6d4761604d50633927d2919479595d0ab090da5","target":"record","created_at":"2026-05-18T00:25:23Z","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":"ccef2a7117d628b53d0038fc65bbe006179be42116fe0a889b69f3db2c4dff78","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-08-28T03:29:23Z","title_canon_sha256":"d1694614813c01e7f63b8fe294090b6f079b0afc5aba1c8e62185e29cc1fe007"},"schema_version":"1.0","source":{"id":"1708.08175","kind":"arxiv","version":2}},"canonical_sha256":"c3642477978966a3c0fe1d653625d35bedfc7204144ff077e400029e41a1d3e5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c3642477978966a3c0fe1d653625d35bedfc7204144ff077e400029e41a1d3e5","first_computed_at":"2026-05-18T00:25:23.544419Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:25:23.544419Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"pQXOIo5jIM73fOunX0FNFL2xnAL5vybry7TUPFHAn5vEyTT21gVhWeoRPbPNZHCwIIT3FHjyytW2SNCIrcXpBw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:25:23.544849Z","signed_message":"canonical_sha256_bytes"},"source_id":"1708.08175","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:83891658aff77051e138dbe4c6d4761604d50633927d2919479595d0ab090da5","sha256:cffad94c09e53fb96db620b5614a2b05d4a1082522fd1d61636031e0c5898afa"],"state_sha256":"4c1c66464d8dc497f07b354e2294c07b4299c815319afe94122a4588bac661a5"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"uckbr0uJIBhawUnb1QB8E62z6d5SbV8XfZpTE70S6TUOHNadNJctsOzy5hcvaD431simfeCKiKvzGy+h+UkwBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T13:20:33.683097Z","bundle_sha256":"da262d81d14ffda38aeca32b6511d98b288679f4686d23dc526f1cb31d0a6535"}}