{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2020:K3FF36DB2JLSGOJBTPK7QKKJU4","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":"2095c63d7ca87b03ad8dfd6854a84a49a311b443949d8239e01e9ee8e578a668","cross_cats_sorted":["cond-mat.quant-gas","cond-mat.stat-mech","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2020-09-21T12:41:50Z","title_canon_sha256":"5269bf9c9d646126a1496f02caf58c83c5105612c0c00971e9598108b0b23e73"},"schema_version":"1.0","source":{"id":"2009.09817","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2009.09817","created_at":"2026-07-05T02:22:38Z"},{"alias_kind":"arxiv_version","alias_value":"2009.09817v2","created_at":"2026-07-05T02:22:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2009.09817","created_at":"2026-07-05T02:22:38Z"},{"alias_kind":"pith_short_12","alias_value":"K3FF36DB2JLS","created_at":"2026-07-05T02:22:38Z"},{"alias_kind":"pith_short_16","alias_value":"K3FF36DB2JLSGOJB","created_at":"2026-07-05T02:22:38Z"},{"alias_kind":"pith_short_8","alias_value":"K3FF36DB","created_at":"2026-07-05T02:22:38Z"}],"graph_snapshots":[{"event_id":"sha256:2e3635997a4ec3157d510fcc1d93c4f438b3e47d63d76d21263f747b49c659e4","target":"graph","created_at":"2026-07-05T02:22:38Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2009.09817/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In this paper we study the out-of-equilibrium phase diagram of the quantum version of Derrida's Random Energy Model, which is the simplest model of mean-field spin glasses. We interpret its corresponding quantum dynamics in Fock space as a one-particle problem in very high dimension to which we apply different theoretical methods tailored for high-dimensional lattices: the Forward-Scattering Approximation, a mapping to the Rosenzweig-Porter model, and the cavity method. Our results indicate the existence of two transition lines and three distinct dynamical phases: a completely many-body locali","authors_text":"Davide Facoetti, Giulio Biroli, Marco Schir\\'o, Marco Tarzia, Pierpaolo Vivo","cross_cats":["cond-mat.quant-gas","cond-mat.stat-mech","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2020-09-21T12:41:50Z","title":"Out of equilibrium Phase Diagram of the Quantum Random Energy Model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2009.09817","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":"sha256:17715fc5308ada19c66443aba8a3d1edeabdcbf4a0d2f0b16a70a8111abba76b","target":"record","created_at":"2026-07-05T02:22:38Z","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":"2095c63d7ca87b03ad8dfd6854a84a49a311b443949d8239e01e9ee8e578a668","cross_cats_sorted":["cond-mat.quant-gas","cond-mat.stat-mech","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2020-09-21T12:41:50Z","title_canon_sha256":"5269bf9c9d646126a1496f02caf58c83c5105612c0c00971e9598108b0b23e73"},"schema_version":"1.0","source":{"id":"2009.09817","kind":"arxiv","version":2}},"canonical_sha256":"56ca5df861d2572339219bd5f82949a7078b43f2fe310b1bed5423fe3d9e67b0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"56ca5df861d2572339219bd5f82949a7078b43f2fe310b1bed5423fe3d9e67b0","first_computed_at":"2026-07-05T02:22:38.209679Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T02:22:38.209679Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ZzWOkj8iDFUhzzQmqbPTQNNuQAn262vlt6kZ+NKYZNMO875aK4Vd80QQS1hpg8UNESaTsWRa1HDsOfgL5K1ICw==","signature_status":"signed_v1","signed_at":"2026-07-05T02:22:38.210169Z","signed_message":"canonical_sha256_bytes"},"source_id":"2009.09817","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:17715fc5308ada19c66443aba8a3d1edeabdcbf4a0d2f0b16a70a8111abba76b","sha256:2e3635997a4ec3157d510fcc1d93c4f438b3e47d63d76d21263f747b49c659e4"],"state_sha256":"5a5b6accb56d0141a4da3f346b2db6cd74c21ab4c96a0f4b2952eebfe797c8b9"}