{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:NPVPKYGDMAFDC3GM73VJ3ES6RS","short_pith_number":"pith:NPVPKYGD","schema_version":"1.0","canonical_sha256":"6beaf560c3600a316cccfeea9d925e8cbe3db84405ab6d4e1cf9aaa2165f76fb","source":{"kind":"arxiv","id":"1604.08384","version":1},"attestation_state":"computed","paper":{"title":"Tuning towards dynamic freezing using a two-rate protocol","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Bhaskar Mukherjee, K. Sengupta, Satyaki Kar","submitted_at":"2016-04-28T12:14:19Z","abstract_excerpt":"We study periodically driven closed quantum systems where two parameters of the system Hamiltonian are driven with frequencies $\\omega_1$ and $\\omega_2=r \\omega_1$. We show that such drives may be used to tune towards dynamics induced freezing where the wavefunction of the state of the system after a drive cycle at time $T= 2\\pi/\\omega_1$ has almost perfect overlap with the initial state. We locate regions in the $(\\omega_1 ,r)$ plane where the freezing is near exact for a class of integrable and a specific non-integrable model. The integrable models that we study encompass Ising and XY models"},"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":"1604.08384","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2016-04-28T12:14:19Z","cross_cats_sorted":[],"title_canon_sha256":"a4b2665db907a7aa27a8e39bed8d84817757e1031b236f0cc67fe5485fd2bddf","abstract_canon_sha256":"b102514c9ae422fc70c1edc6078f82a79c77e09fdb2d3791d5fcd62a9d93ea4c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:08:09.676214Z","signature_b64":"BlgYWEz8KMGS2NmGfvhqZj2O6Ie+ZfcSgO6v3eUxNXZ+FkMSYTddLhUkfTPKvCsZ/oSmKqxUJIPDog22daIbDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6beaf560c3600a316cccfeea9d925e8cbe3db84405ab6d4e1cf9aaa2165f76fb","last_reissued_at":"2026-05-18T01:08:09.675721Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:08:09.675721Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Tuning towards dynamic freezing using a two-rate protocol","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Bhaskar Mukherjee, K. Sengupta, Satyaki Kar","submitted_at":"2016-04-28T12:14:19Z","abstract_excerpt":"We study periodically driven closed quantum systems where two parameters of the system Hamiltonian are driven with frequencies $\\omega_1$ and $\\omega_2=r \\omega_1$. We show that such drives may be used to tune towards dynamics induced freezing where the wavefunction of the state of the system after a drive cycle at time $T= 2\\pi/\\omega_1$ has almost perfect overlap with the initial state. We locate regions in the $(\\omega_1 ,r)$ plane where the freezing is near exact for a class of integrable and a specific non-integrable model. The integrable models that we study encompass Ising and XY models"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.08384","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":"1604.08384","created_at":"2026-05-18T01:08:09.675805+00:00"},{"alias_kind":"arxiv_version","alias_value":"1604.08384v1","created_at":"2026-05-18T01:08:09.675805+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.08384","created_at":"2026-05-18T01:08:09.675805+00:00"},{"alias_kind":"pith_short_12","alias_value":"NPVPKYGDMAFD","created_at":"2026-05-18T12:30:36.002864+00:00"},{"alias_kind":"pith_short_16","alias_value":"NPVPKYGDMAFDC3GM","created_at":"2026-05-18T12:30:36.002864+00:00"},{"alias_kind":"pith_short_8","alias_value":"NPVPKYGD","created_at":"2026-05-18T12:30:36.002864+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/NPVPKYGDMAFDC3GM73VJ3ES6RS","json":"https://pith.science/pith/NPVPKYGDMAFDC3GM73VJ3ES6RS.json","graph_json":"https://pith.science/api/pith-number/NPVPKYGDMAFDC3GM73VJ3ES6RS/graph.json","events_json":"https://pith.science/api/pith-number/NPVPKYGDMAFDC3GM73VJ3ES6RS/events.json","paper":"https://pith.science/paper/NPVPKYGD"},"agent_actions":{"view_html":"https://pith.science/pith/NPVPKYGDMAFDC3GM73VJ3ES6RS","download_json":"https://pith.science/pith/NPVPKYGDMAFDC3GM73VJ3ES6RS.json","view_paper":"https://pith.science/paper/NPVPKYGD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1604.08384&json=true","fetch_graph":"https://pith.science/api/pith-number/NPVPKYGDMAFDC3GM73VJ3ES6RS/graph.json","fetch_events":"https://pith.science/api/pith-number/NPVPKYGDMAFDC3GM73VJ3ES6RS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NPVPKYGDMAFDC3GM73VJ3ES6RS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NPVPKYGDMAFDC3GM73VJ3ES6RS/action/storage_attestation","attest_author":"https://pith.science/pith/NPVPKYGDMAFDC3GM73VJ3ES6RS/action/author_attestation","sign_citation":"https://pith.science/pith/NPVPKYGDMAFDC3GM73VJ3ES6RS/action/citation_signature","submit_replication":"https://pith.science/pith/NPVPKYGDMAFDC3GM73VJ3ES6RS/action/replication_record"}},"created_at":"2026-05-18T01:08:09.675805+00:00","updated_at":"2026-05-18T01:08:09.675805+00:00"}