{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:BOVN4ORUYBQJPVVVY5R5VU5FMO","short_pith_number":"pith:BOVN4ORU","canonical_record":{"source":{"id":"1710.08862","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-10-24T15:58:52Z","cross_cats_sorted":[],"title_canon_sha256":"6d0e73fa73ae825ebd8ed0ef064759cca434513849dd80cbc53194b27559e8ea","abstract_canon_sha256":"eb97b4eb2105d042ecb442473961fdabffc8cc1ba4f888b3ce5ba7714a7feea5"},"schema_version":"1.0"},"canonical_sha256":"0baade3a34c06097d6b5c763dad3a563af920296c8323a940625600d81f71578","source":{"kind":"arxiv","id":"1710.08862","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.08862","created_at":"2026-05-18T00:14:34Z"},{"alias_kind":"arxiv_version","alias_value":"1710.08862v2","created_at":"2026-05-18T00:14:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.08862","created_at":"2026-05-18T00:14:34Z"},{"alias_kind":"pith_short_12","alias_value":"BOVN4ORUYBQJ","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_16","alias_value":"BOVN4ORUYBQJPVVV","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_8","alias_value":"BOVN4ORU","created_at":"2026-05-18T12:31:08Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:BOVN4ORUYBQJPVVVY5R5VU5FMO","target":"record","payload":{"canonical_record":{"source":{"id":"1710.08862","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-10-24T15:58:52Z","cross_cats_sorted":[],"title_canon_sha256":"6d0e73fa73ae825ebd8ed0ef064759cca434513849dd80cbc53194b27559e8ea","abstract_canon_sha256":"eb97b4eb2105d042ecb442473961fdabffc8cc1ba4f888b3ce5ba7714a7feea5"},"schema_version":"1.0"},"canonical_sha256":"0baade3a34c06097d6b5c763dad3a563af920296c8323a940625600d81f71578","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:14:34.412070Z","signature_b64":"LbShP8gC2M6kKrmwZCEdY6oTMUD2jk2NjK/7telDxkno54LPKjHCb8nUccEHz7a358OKTJ/AlCz3OGmSi3AbAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0baade3a34c06097d6b5c763dad3a563af920296c8323a940625600d81f71578","last_reissued_at":"2026-05-18T00:14:34.411519Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:14:34.411519Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1710.08862","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":"2026-05-18T00:14:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+1E0ZAmp5qaHPV6/uAvqqBVQxVipB7iSeA/cPGAOixEGbRkp5THKkUhyY9oEjx8dMrAie+H8fuWMZ5JJT42BAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T05:34:20.467122Z"},"content_sha256":"da6a5ba919f33577ad3fe61f37da82e9b0d0d71722cb65e0d8420f0e6be4929c","schema_version":"1.0","event_id":"sha256:da6a5ba919f33577ad3fe61f37da82e9b0d0d71722cb65e0d8420f0e6be4929c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:BOVN4ORUYBQJPVVVY5R5VU5FMO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quantum criticality and state engineering in the simulated anisotropic quantum Rabi model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"G. Romero, Hong-Gang Luo, J. Q. You, Maoxin Liu, Wen-Long You, Yimin Wang, Yu-Li Dong","submitted_at":"2017-10-24T15:58:52Z","abstract_excerpt":"Promising applications of the anisotropic quantum Rabi model (AQRM) in broad parameter ranges are explored, which is realized with superconducting flux qubits simultaneously driven by two-tone time-dependent magnetic fields. Regarding the quantum phase transitions (QPTs), with assistant of fidelity susceptibility, we extract the scaling functions and the critical exponents, with which the universal scaling of the cumulant ratio is captured with rescaling of the parameters due to the anisotropy. Moreover, a fixed point of the cumulant ratio is predicted at the critical point of the AQRM. In res"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.08862","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":"2026-05-18T00:14:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mRnVnIzLbD56CSlCQZ9cXCVCrnseqrFBuD9hMj5MJbBoC0i+7PmfUCE4Iofd39vK8v0wBf4aaJcnJm4Awbj1DA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T05:34:20.467500Z"},"content_sha256":"f5f0657bcc60619d18b3154ea28f6e78b058b23de4566df79bd9b186c6b0fac2","schema_version":"1.0","event_id":"sha256:f5f0657bcc60619d18b3154ea28f6e78b058b23de4566df79bd9b186c6b0fac2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/BOVN4ORUYBQJPVVVY5R5VU5FMO/bundle.json","state_url":"https://pith.science/pith/BOVN4ORUYBQJPVVVY5R5VU5FMO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/BOVN4ORUYBQJPVVVY5R5VU5FMO/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":"2026-06-04T05:34:20Z","links":{"resolver":"https://pith.science/pith/BOVN4ORUYBQJPVVVY5R5VU5FMO","bundle":"https://pith.science/pith/BOVN4ORUYBQJPVVVY5R5VU5FMO/bundle.json","state":"https://pith.science/pith/BOVN4ORUYBQJPVVVY5R5VU5FMO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/BOVN4ORUYBQJPVVVY5R5VU5FMO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:BOVN4ORUYBQJPVVVY5R5VU5FMO","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":"eb97b4eb2105d042ecb442473961fdabffc8cc1ba4f888b3ce5ba7714a7feea5","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-10-24T15:58:52Z","title_canon_sha256":"6d0e73fa73ae825ebd8ed0ef064759cca434513849dd80cbc53194b27559e8ea"},"schema_version":"1.0","source":{"id":"1710.08862","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.08862","created_at":"2026-05-18T00:14:34Z"},{"alias_kind":"arxiv_version","alias_value":"1710.08862v2","created_at":"2026-05-18T00:14:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.08862","created_at":"2026-05-18T00:14:34Z"},{"alias_kind":"pith_short_12","alias_value":"BOVN4ORUYBQJ","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_16","alias_value":"BOVN4ORUYBQJPVVV","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_8","alias_value":"BOVN4ORU","created_at":"2026-05-18T12:31:08Z"}],"graph_snapshots":[{"event_id":"sha256:f5f0657bcc60619d18b3154ea28f6e78b058b23de4566df79bd9b186c6b0fac2","target":"graph","created_at":"2026-05-18T00:14:34Z","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":"Promising applications of the anisotropic quantum Rabi model (AQRM) in broad parameter ranges are explored, which is realized with superconducting flux qubits simultaneously driven by two-tone time-dependent magnetic fields. Regarding the quantum phase transitions (QPTs), with assistant of fidelity susceptibility, we extract the scaling functions and the critical exponents, with which the universal scaling of the cumulant ratio is captured with rescaling of the parameters due to the anisotropy. Moreover, a fixed point of the cumulant ratio is predicted at the critical point of the AQRM. In res","authors_text":"G. Romero, Hong-Gang Luo, J. Q. You, Maoxin Liu, Wen-Long You, Yimin Wang, Yu-Li Dong","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-10-24T15:58:52Z","title":"Quantum criticality and state engineering in the simulated anisotropic quantum Rabi model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.08862","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:da6a5ba919f33577ad3fe61f37da82e9b0d0d71722cb65e0d8420f0e6be4929c","target":"record","created_at":"2026-05-18T00:14:34Z","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":"eb97b4eb2105d042ecb442473961fdabffc8cc1ba4f888b3ce5ba7714a7feea5","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-10-24T15:58:52Z","title_canon_sha256":"6d0e73fa73ae825ebd8ed0ef064759cca434513849dd80cbc53194b27559e8ea"},"schema_version":"1.0","source":{"id":"1710.08862","kind":"arxiv","version":2}},"canonical_sha256":"0baade3a34c06097d6b5c763dad3a563af920296c8323a940625600d81f71578","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0baade3a34c06097d6b5c763dad3a563af920296c8323a940625600d81f71578","first_computed_at":"2026-05-18T00:14:34.411519Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:14:34.411519Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"LbShP8gC2M6kKrmwZCEdY6oTMUD2jk2NjK/7telDxkno54LPKjHCb8nUccEHz7a358OKTJ/AlCz3OGmSi3AbAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:14:34.412070Z","signed_message":"canonical_sha256_bytes"},"source_id":"1710.08862","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:da6a5ba919f33577ad3fe61f37da82e9b0d0d71722cb65e0d8420f0e6be4929c","sha256:f5f0657bcc60619d18b3154ea28f6e78b058b23de4566df79bd9b186c6b0fac2"],"state_sha256":"85727913f518a7dd05f9f3a736a5ff2c4004c39cd66e53bb711ff0504c31f6bc"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"W2th64M+LQMa2MYCp73CPa+CRNYUf0eASuC6WyWs2Uw+wFrxUBYB9g5fqySxZJoMXLKCmZ7g39QP8JRPYERSDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-04T05:34:20.469660Z","bundle_sha256":"1205dc38ee5a680f4a934b826f25716c04cfbc48dec28d620c5181610c6649cc"}}