{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:W74KM3PHHKEAHVOD5QJ6MCUWXS","short_pith_number":"pith:W74KM3PH","schema_version":"1.0","canonical_sha256":"b7f8a66de73a8803d5c3ec13e60a96bcb081f77ccbf63b0a850ab64b3599ccac","source":{"kind":"arxiv","id":"2606.20807","version":1},"attestation_state":"computed","paper":{"title":"Tuning ergodicity breaking: Anomalous diffusion under asymptotic power-law forcing","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"(2) Instituto de Ciencias, 3), (3) National Scientific, 85867-970 Foz do Igua\\c{c}u, Argentina, Argentina), Brazil, Buenos Aires, Los Polvorines, Luciano C. Lapas (3) ((1) Instituto Latino-Americano de Ci\\^encias da Vida e da Natureza, M. Florencia Carusela (2, Paran\\'a, Raul V. B. Mor\\'as (1), Technical Research Council, Universidade Federal da Integra\\c{c}\\~ao Latino-Americana, Universidad Nacional de General Sarmiento","submitted_at":"2026-06-18T18:00:23Z","abstract_excerpt":"In non-Markovian systems, distinct dynamical phases arise from the competition between internal memory and external forcing, encompassing thermalization, persistent ergodicity breaking, and runaway energy growth. This study shows that the scaling parameter $\\eta$ governs the emergent phase diagram within a system described by the Generalized Langevin Equation, particularly when subjected to external drives with asymptotic power-law tails. Three universal regimes for diffusive processes are delineated by this parameter: thermalization ($\\eta > 0$), non-ergodic saturation ($\\eta = 0$), and a for"},"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":"2606.20807","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-06-18T18:00:23Z","cross_cats_sorted":[],"title_canon_sha256":"e204d8063fe05eb37abba15690f55d07f7651f60e06701e1d237ffeb89e32c90","abstract_canon_sha256":"b66da50e323b70933ac253be729dac4b1d68836d2102c663ec64e57ac66e4000"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-23T00:11:59.355354Z","signature_b64":"qxWNpe/E72IvG8s2TgVhHld265TlpJ18yLnU2nPjW0eg/eJuBTG6hITSf8NxyGyxqdBwuFfne15DpDDWvhTDCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b7f8a66de73a8803d5c3ec13e60a96bcb081f77ccbf63b0a850ab64b3599ccac","last_reissued_at":"2026-06-23T00:11:59.354944Z","signature_status":"signed_v1","first_computed_at":"2026-06-23T00:11:59.354944Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Tuning ergodicity breaking: Anomalous diffusion under asymptotic power-law forcing","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"(2) Instituto de Ciencias, 3), (3) National Scientific, 85867-970 Foz do Igua\\c{c}u, Argentina, Argentina), Brazil, Buenos Aires, Los Polvorines, Luciano C. Lapas (3) ((1) Instituto Latino-Americano de Ci\\^encias da Vida e da Natureza, M. Florencia Carusela (2, Paran\\'a, Raul V. B. Mor\\'as (1), Technical Research Council, Universidade Federal da Integra\\c{c}\\~ao Latino-Americana, Universidad Nacional de General Sarmiento","submitted_at":"2026-06-18T18:00:23Z","abstract_excerpt":"In non-Markovian systems, distinct dynamical phases arise from the competition between internal memory and external forcing, encompassing thermalization, persistent ergodicity breaking, and runaway energy growth. This study shows that the scaling parameter $\\eta$ governs the emergent phase diagram within a system described by the Generalized Langevin Equation, particularly when subjected to external drives with asymptotic power-law tails. Three universal regimes for diffusive processes are delineated by this parameter: thermalization ($\\eta > 0$), non-ergodic saturation ($\\eta = 0$), and a for"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.20807","kind":"arxiv","version":1},"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/2606.20807/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":"2606.20807","created_at":"2026-06-23T00:11:59.355000+00:00"},{"alias_kind":"arxiv_version","alias_value":"2606.20807v1","created_at":"2026-06-23T00:11:59.355000+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.20807","created_at":"2026-06-23T00:11:59.355000+00:00"},{"alias_kind":"pith_short_12","alias_value":"W74KM3PHHKEA","created_at":"2026-06-23T00:11:59.355000+00:00"},{"alias_kind":"pith_short_16","alias_value":"W74KM3PHHKEAHVOD","created_at":"2026-06-23T00:11:59.355000+00:00"},{"alias_kind":"pith_short_8","alias_value":"W74KM3PH","created_at":"2026-06-23T00:11:59.355000+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/W74KM3PHHKEAHVOD5QJ6MCUWXS","json":"https://pith.science/pith/W74KM3PHHKEAHVOD5QJ6MCUWXS.json","graph_json":"https://pith.science/api/pith-number/W74KM3PHHKEAHVOD5QJ6MCUWXS/graph.json","events_json":"https://pith.science/api/pith-number/W74KM3PHHKEAHVOD5QJ6MCUWXS/events.json","paper":"https://pith.science/paper/W74KM3PH"},"agent_actions":{"view_html":"https://pith.science/pith/W74KM3PHHKEAHVOD5QJ6MCUWXS","download_json":"https://pith.science/pith/W74KM3PHHKEAHVOD5QJ6MCUWXS.json","view_paper":"https://pith.science/paper/W74KM3PH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2606.20807&json=true","fetch_graph":"https://pith.science/api/pith-number/W74KM3PHHKEAHVOD5QJ6MCUWXS/graph.json","fetch_events":"https://pith.science/api/pith-number/W74KM3PHHKEAHVOD5QJ6MCUWXS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/W74KM3PHHKEAHVOD5QJ6MCUWXS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/W74KM3PHHKEAHVOD5QJ6MCUWXS/action/storage_attestation","attest_author":"https://pith.science/pith/W74KM3PHHKEAHVOD5QJ6MCUWXS/action/author_attestation","sign_citation":"https://pith.science/pith/W74KM3PHHKEAHVOD5QJ6MCUWXS/action/citation_signature","submit_replication":"https://pith.science/pith/W74KM3PHHKEAHVOD5QJ6MCUWXS/action/replication_record"}},"created_at":"2026-06-23T00:11:59.355000+00:00","updated_at":"2026-06-23T00:11:59.355000+00:00"}