{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:J4GFMYFSSJSVMG46UKPWABUOZW","short_pith_number":"pith:J4GFMYFS","schema_version":"1.0","canonical_sha256":"4f0c5660b29265561b9ea29f60068ecda5e13f0ba8dd94db21bc3dd68e9fdb02","source":{"kind":"arxiv","id":"2312.02039","version":2},"attestation_state":"computed","paper":{"title":"Entanglement-magic separation in hybrid quantum circuits","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"quant-ph","authors_text":"Emanuele Tirrito, Gerald E. Fux, Marcello Dalmonte, Rosario Fazio","submitted_at":"2023-12-04T16:57:33Z","abstract_excerpt":"Magic describes the distance of a quantum state to its closest stabilizer state. It is -- like entanglement -- a necessary resource for a potential quantum advantage over classical computing. We study magic, quantified by stabilizer entropy, in a hybrid quantum circuit with projective measurements and a controlled injection of non-Clifford resources. We discover a phase transition between a (sub)-extensive and area law scaling of magic controlled by the rate of measurements. The same circuit also exhibits a phase transition in entanglement that appears, however, at a different critical measure"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2312.02039","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2023-12-04T16:57:33Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"e9abf6a2068131e2fb8637f1ed226ebf8c9afc28ab9ed39259aaec562bb4780e","abstract_canon_sha256":"ba6bb3259a45ac5109368909ea76eb66d7d30036930fe88bce26f61dc8ab71bd"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:39:20.382680Z","signature_b64":"qPvmSEJX5y4GFwOD4wq8/vgrJdq51Q6/hku+1zeWKeKgXXgkntuOKIQMVdON0R0ubr2vRwY7YYmMktZtARJUCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4f0c5660b29265561b9ea29f60068ecda5e13f0ba8dd94db21bc3dd68e9fdb02","last_reissued_at":"2026-07-05T09:39:20.382245Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:39:20.382245Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Entanglement-magic separation in hybrid quantum circuits","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"quant-ph","authors_text":"Emanuele Tirrito, Gerald E. Fux, Marcello Dalmonte, Rosario Fazio","submitted_at":"2023-12-04T16:57:33Z","abstract_excerpt":"Magic describes the distance of a quantum state to its closest stabilizer state. It is -- like entanglement -- a necessary resource for a potential quantum advantage over classical computing. We study magic, quantified by stabilizer entropy, in a hybrid quantum circuit with projective measurements and a controlled injection of non-Clifford resources. We discover a phase transition between a (sub)-extensive and area law scaling of magic controlled by the rate of measurements. The same circuit also exhibits a phase transition in entanglement that appears, however, at a different critical measure"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2312.02039","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2312.02039/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2312.02039","created_at":"2026-07-05T09:39:20.382297+00:00"},{"alias_kind":"arxiv_version","alias_value":"2312.02039v2","created_at":"2026-07-05T09:39:20.382297+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2312.02039","created_at":"2026-07-05T09:39:20.382297+00:00"},{"alias_kind":"pith_short_12","alias_value":"J4GFMYFSSJSV","created_at":"2026-07-05T09:39:20.382297+00:00"},{"alias_kind":"pith_short_16","alias_value":"J4GFMYFSSJSVMG46","created_at":"2026-07-05T09:39:20.382297+00:00"},{"alias_kind":"pith_short_8","alias_value":"J4GFMYFS","created_at":"2026-07-05T09:39:20.382297+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2508.20252","citing_title":"Classical Simulations of Low Magic Quantum Dynamics","ref_index":19,"is_internal_anchor":false},{"citing_arxiv_id":"2605.22424","citing_title":"Long-range nonstabilizerness of topologically encoded states from mutual information","ref_index":42,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/J4GFMYFSSJSVMG46UKPWABUOZW","json":"https://pith.science/pith/J4GFMYFSSJSVMG46UKPWABUOZW.json","graph_json":"https://pith.science/api/pith-number/J4GFMYFSSJSVMG46UKPWABUOZW/graph.json","events_json":"https://pith.science/api/pith-number/J4GFMYFSSJSVMG46UKPWABUOZW/events.json","paper":"https://pith.science/paper/J4GFMYFS"},"agent_actions":{"view_html":"https://pith.science/pith/J4GFMYFSSJSVMG46UKPWABUOZW","download_json":"https://pith.science/pith/J4GFMYFSSJSVMG46UKPWABUOZW.json","view_paper":"https://pith.science/paper/J4GFMYFS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2312.02039&json=true","fetch_graph":"https://pith.science/api/pith-number/J4GFMYFSSJSVMG46UKPWABUOZW/graph.json","fetch_events":"https://pith.science/api/pith-number/J4GFMYFSSJSVMG46UKPWABUOZW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/J4GFMYFSSJSVMG46UKPWABUOZW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/J4GFMYFSSJSVMG46UKPWABUOZW/action/storage_attestation","attest_author":"https://pith.science/pith/J4GFMYFSSJSVMG46UKPWABUOZW/action/author_attestation","sign_citation":"https://pith.science/pith/J4GFMYFSSJSVMG46UKPWABUOZW/action/citation_signature","submit_replication":"https://pith.science/pith/J4GFMYFSSJSVMG46UKPWABUOZW/action/replication_record"}},"created_at":"2026-07-05T09:39:20.382297+00:00","updated_at":"2026-07-05T09:39:20.382297+00:00"}