{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:2TQZCRGIYAUV6M46IGVOSAEAV7","short_pith_number":"pith:2TQZCRGI","schema_version":"1.0","canonical_sha256":"d4e19144c8c0295f339e41aae90080affabcdcf9c703182fb20627f434951020","source":{"kind":"arxiv","id":"1110.6799","version":1},"attestation_state":"computed","paper":{"title":"Phase controllable dynamical localization: a generalization of the Dunlap-Kenkre result","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.quant-gas"],"primary_cat":"cond-mat.stat-mech","authors_text":"Navinder Singh","submitted_at":"2011-10-31T14:11:27Z","abstract_excerpt":"Dunlap-Kenkre result states that Dynamical Localization (DL) of a field driven quantum particle in a discrete periodic lattice happens when the ratio of the field magnitude to the field frequency (say, $\\eta$) of the diagonal sinusoidal drive is a root of the ordinary Bessel function of order 0. This has been experimentally verified. A generalization of the Dunlap-Kenkre result is presented here. We analytically show that if we have an off-diagonal driving field (with modulation $\\delta$) and diagonal driving field with different frequencies (say $\\omega_1$ and $\\omega_2$ respectively) and a d"},"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":"1110.6799","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-10-31T14:11:27Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.quant-gas"],"title_canon_sha256":"de759c84390ec3c3dcba0539506a8402705538a17d51e8f50fc3ebf8965fb9b4","abstract_canon_sha256":"1d445d95a0ba61f88737e512d4b3b2769c721c98f0c55fa9816526eee5a37dc5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:09:54.167300Z","signature_b64":"Fs6iDuheAmhADScEFe0Ucn1i7Jjdi05XVhkiBiU3W7mwN+r3T0HKRez+YpZ3+VaFNzfqX1O76iMLZLrVX3BOCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d4e19144c8c0295f339e41aae90080affabcdcf9c703182fb20627f434951020","last_reissued_at":"2026-05-18T04:09:54.166806Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:09:54.166806Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Phase controllable dynamical localization: a generalization of the Dunlap-Kenkre result","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.quant-gas"],"primary_cat":"cond-mat.stat-mech","authors_text":"Navinder Singh","submitted_at":"2011-10-31T14:11:27Z","abstract_excerpt":"Dunlap-Kenkre result states that Dynamical Localization (DL) of a field driven quantum particle in a discrete periodic lattice happens when the ratio of the field magnitude to the field frequency (say, $\\eta$) of the diagonal sinusoidal drive is a root of the ordinary Bessel function of order 0. This has been experimentally verified. A generalization of the Dunlap-Kenkre result is presented here. We analytically show that if we have an off-diagonal driving field (with modulation $\\delta$) and diagonal driving field with different frequencies (say $\\omega_1$ and $\\omega_2$ respectively) and a d"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1110.6799","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":""},"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":"1110.6799","created_at":"2026-05-18T04:09:54.166876+00:00"},{"alias_kind":"arxiv_version","alias_value":"1110.6799v1","created_at":"2026-05-18T04:09:54.166876+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1110.6799","created_at":"2026-05-18T04:09:54.166876+00:00"},{"alias_kind":"pith_short_12","alias_value":"2TQZCRGIYAUV","created_at":"2026-05-18T12:26:18.847500+00:00"},{"alias_kind":"pith_short_16","alias_value":"2TQZCRGIYAUV6M46","created_at":"2026-05-18T12:26:18.847500+00:00"},{"alias_kind":"pith_short_8","alias_value":"2TQZCRGI","created_at":"2026-05-18T12:26:18.847500+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/2TQZCRGIYAUV6M46IGVOSAEAV7","json":"https://pith.science/pith/2TQZCRGIYAUV6M46IGVOSAEAV7.json","graph_json":"https://pith.science/api/pith-number/2TQZCRGIYAUV6M46IGVOSAEAV7/graph.json","events_json":"https://pith.science/api/pith-number/2TQZCRGIYAUV6M46IGVOSAEAV7/events.json","paper":"https://pith.science/paper/2TQZCRGI"},"agent_actions":{"view_html":"https://pith.science/pith/2TQZCRGIYAUV6M46IGVOSAEAV7","download_json":"https://pith.science/pith/2TQZCRGIYAUV6M46IGVOSAEAV7.json","view_paper":"https://pith.science/paper/2TQZCRGI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1110.6799&json=true","fetch_graph":"https://pith.science/api/pith-number/2TQZCRGIYAUV6M46IGVOSAEAV7/graph.json","fetch_events":"https://pith.science/api/pith-number/2TQZCRGIYAUV6M46IGVOSAEAV7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2TQZCRGIYAUV6M46IGVOSAEAV7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2TQZCRGIYAUV6M46IGVOSAEAV7/action/storage_attestation","attest_author":"https://pith.science/pith/2TQZCRGIYAUV6M46IGVOSAEAV7/action/author_attestation","sign_citation":"https://pith.science/pith/2TQZCRGIYAUV6M46IGVOSAEAV7/action/citation_signature","submit_replication":"https://pith.science/pith/2TQZCRGIYAUV6M46IGVOSAEAV7/action/replication_record"}},"created_at":"2026-05-18T04:09:54.166876+00:00","updated_at":"2026-05-18T04:09:54.166876+00:00"}