{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:VCIM2EXEPBSSEB67Z3OO34D66K","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":"501df3f5d99e2dd9086e253f82ce9a14ab807591587e3ea84952f264344e44ee","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2023-03-31T17:11:03Z","title_canon_sha256":"6d123ccdcdbb84200fe903ba56ee4739bcdd63534c93c1c38f71c26c3627497e"},"schema_version":"1.0","source":{"id":"2303.18213","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2303.18213","created_at":"2026-07-05T06:29:45Z"},{"alias_kind":"arxiv_version","alias_value":"2303.18213v1","created_at":"2026-07-05T06:29:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2303.18213","created_at":"2026-07-05T06:29:45Z"},{"alias_kind":"pith_short_12","alias_value":"VCIM2EXEPBSS","created_at":"2026-07-05T06:29:45Z"},{"alias_kind":"pith_short_16","alias_value":"VCIM2EXEPBSSEB67","created_at":"2026-07-05T06:29:45Z"},{"alias_kind":"pith_short_8","alias_value":"VCIM2EXE","created_at":"2026-07-05T06:29:45Z"}],"graph_snapshots":[{"event_id":"sha256:71bd27b7e1116402d6a8f40cc9887d383d3f3a3b18c0727a28b838c024b99ba4","target":"graph","created_at":"2026-07-05T06:29:45Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2303.18213/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Dephasing in quantum systems is typically the result of its interaction with environmental degrees of freedom. We investigate within a spin-boson model the influence of a super-Ohmic environment on the dynamics of a quantum two-state system. A super-Ohmic enviroment, thereby, models typical bulk phonons which are a common disturbance for solid state quantum systems as, for example, NV centers. By applying the numerically exact quasi-adiabatic path integral approach we show that for strong system-bath coupling, pseudo-coherent dynamics emerges, i.e., oscillatory dynamics at short times due to s","authors_text":"Florian Otterpohl, Michael Thorwart, Peter Nalbach, Philipp Nacke","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2023-03-31T17:11:03Z","title":"Dephasing and pseudo-coherent quantum dynamics in super-Ohmic environments"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2303.18213","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:ea5389ad15a03a71f263001fc710f9698a0363e6a51c0afe43f8fd3ef945bc61","target":"record","created_at":"2026-07-05T06:29:45Z","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":"501df3f5d99e2dd9086e253f82ce9a14ab807591587e3ea84952f264344e44ee","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2023-03-31T17:11:03Z","title_canon_sha256":"6d123ccdcdbb84200fe903ba56ee4739bcdd63534c93c1c38f71c26c3627497e"},"schema_version":"1.0","source":{"id":"2303.18213","kind":"arxiv","version":1}},"canonical_sha256":"a890cd12e478652207dfcedcedf07ef28408af6fdfd1ba0db5aa460c9b29c97c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a890cd12e478652207dfcedcedf07ef28408af6fdfd1ba0db5aa460c9b29c97c","first_computed_at":"2026-07-05T06:29:45.144898Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:29:45.144898Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"jFdUPGdYAAx4VU29tlHExwJDBdGJqcmeWXeGv9BtD6KIylqLCK6DUdpt+pt2afiRaA5zKwCZOgyLNYmNtGe9DA==","signature_status":"signed_v1","signed_at":"2026-07-05T06:29:45.145304Z","signed_message":"canonical_sha256_bytes"},"source_id":"2303.18213","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ea5389ad15a03a71f263001fc710f9698a0363e6a51c0afe43f8fd3ef945bc61","sha256:71bd27b7e1116402d6a8f40cc9887d383d3f3a3b18c0727a28b838c024b99ba4"],"state_sha256":"ba94819a17ec5e2a1ad44629606f00a2fd7184aafac986ac9624bbbd632944d3"}