{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:FNPK6K7FW65PFUTTKWSC42KH6K","short_pith_number":"pith:FNPK6K7F","schema_version":"1.0","canonical_sha256":"2b5eaf2be5b7baf2d27355a42e6947f2a1d7166aa156c0e66f9ade5a72f64d31","source":{"kind":"arxiv","id":"2412.11619","version":2},"attestation_state":"computed","paper":{"title":"Time-translation invariance symmetry breaking hidden by finite-scale singularities","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.dis-nn","authors_text":"Dine Ousmane Samary, Ixandra Achitouv, Parham Radpay, Vincent Lahoche","submitted_at":"2024-12-16T10:05:10Z","abstract_excerpt":"In this paper, we consider a renormalization group perspective on the quantum dynamics of a particle moving in the Euclidean $\\mathbb{R}^N$ space through the complex landscape provided by a disordered Hamiltonian of type $2+p$. We focus on the large $N$ limit, where the coarse-graining procedure is unconventional: it is based on the Wigner spectrum of the rank-2 disorder. The main consequence of this choice is that canonical dimensions depend on the scale, and the flow equations fail to become autonomous, preventing the existence of global fixed points. One of the main features of the underlyi"},"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":"2412.11619","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2024-12-16T10:05:10Z","cross_cats_sorted":[],"title_canon_sha256":"d90b9afc8954660af163e9000cb79f84a9247159269509af5a53fe5ed26a82b5","abstract_canon_sha256":"aa9d59df35ce5eeb2567b6aeeec902df9db25f50c070486fc3ea878ff969a69e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:13:45.632409Z","signature_b64":"/z7GxqOIGhYSTjBPL9DJH3jHDVEDNMTuf06oaSzkxUkOqHegPilhmIY4xRNncI2FETdG3a2G+2AoI3E7vJ1kCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2b5eaf2be5b7baf2d27355a42e6947f2a1d7166aa156c0e66f9ade5a72f64d31","last_reissued_at":"2026-07-05T10:13:45.631901Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:13:45.631901Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Time-translation invariance symmetry breaking hidden by finite-scale singularities","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.dis-nn","authors_text":"Dine Ousmane Samary, Ixandra Achitouv, Parham Radpay, Vincent Lahoche","submitted_at":"2024-12-16T10:05:10Z","abstract_excerpt":"In this paper, we consider a renormalization group perspective on the quantum dynamics of a particle moving in the Euclidean $\\mathbb{R}^N$ space through the complex landscape provided by a disordered Hamiltonian of type $2+p$. We focus on the large $N$ limit, where the coarse-graining procedure is unconventional: it is based on the Wigner spectrum of the rank-2 disorder. The main consequence of this choice is that canonical dimensions depend on the scale, and the flow equations fail to become autonomous, preventing the existence of global fixed points. One of the main features of the underlyi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2412.11619","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/2412.11619/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":"2412.11619","created_at":"2026-07-05T10:13:45.631962+00:00"},{"alias_kind":"arxiv_version","alias_value":"2412.11619v2","created_at":"2026-07-05T10:13:45.631962+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2412.11619","created_at":"2026-07-05T10:13:45.631962+00:00"},{"alias_kind":"pith_short_12","alias_value":"FNPK6K7FW65P","created_at":"2026-07-05T10:13:45.631962+00:00"},{"alias_kind":"pith_short_16","alias_value":"FNPK6K7FW65PFUTT","created_at":"2026-07-05T10:13:45.631962+00:00"},{"alias_kind":"pith_short_8","alias_value":"FNPK6K7F","created_at":"2026-07-05T10:13:45.631962+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2509.05507","citing_title":"Stochastic dynamics for group field theories II: Methods for nonequilibrium renormalization group","ref_index":57,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FNPK6K7FW65PFUTTKWSC42KH6K","json":"https://pith.science/pith/FNPK6K7FW65PFUTTKWSC42KH6K.json","graph_json":"https://pith.science/api/pith-number/FNPK6K7FW65PFUTTKWSC42KH6K/graph.json","events_json":"https://pith.science/api/pith-number/FNPK6K7FW65PFUTTKWSC42KH6K/events.json","paper":"https://pith.science/paper/FNPK6K7F"},"agent_actions":{"view_html":"https://pith.science/pith/FNPK6K7FW65PFUTTKWSC42KH6K","download_json":"https://pith.science/pith/FNPK6K7FW65PFUTTKWSC42KH6K.json","view_paper":"https://pith.science/paper/FNPK6K7F","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2412.11619&json=true","fetch_graph":"https://pith.science/api/pith-number/FNPK6K7FW65PFUTTKWSC42KH6K/graph.json","fetch_events":"https://pith.science/api/pith-number/FNPK6K7FW65PFUTTKWSC42KH6K/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FNPK6K7FW65PFUTTKWSC42KH6K/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FNPK6K7FW65PFUTTKWSC42KH6K/action/storage_attestation","attest_author":"https://pith.science/pith/FNPK6K7FW65PFUTTKWSC42KH6K/action/author_attestation","sign_citation":"https://pith.science/pith/FNPK6K7FW65PFUTTKWSC42KH6K/action/citation_signature","submit_replication":"https://pith.science/pith/FNPK6K7FW65PFUTTKWSC42KH6K/action/replication_record"}},"created_at":"2026-07-05T10:13:45.631962+00:00","updated_at":"2026-07-05T10:13:45.631962+00:00"}