{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:TUKV37SHUVO2R7N736H5EXLC3W","short_pith_number":"pith:TUKV37SH","schema_version":"1.0","canonical_sha256":"9d155dfe47a55da8fdbfdf8fd25d62ddaef408eb6cf172e5226801866f7408ab","source":{"kind":"arxiv","id":"1405.6321","version":2},"attestation_state":"computed","paper":{"title":"Poisson to GOE transition in the distribution of the ratio of consecutive level spacings","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nlin.CD","quant-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"H. N. Deota, N. D. Chavda, V. K. B. Kota","submitted_at":"2014-05-24T17:00:28Z","abstract_excerpt":"Probability distribution for the ratio ($r$) of consecutive level spacings of the eigenvalues of a Poisson (generating regular spectra) spectrum and that of a GOE random matrix ensemble are given recently. Going beyond these, for the ensemble generated by the Hamiltonian $H_\\lambda = (H_0+\\lambda V)/\\sqrt{1+\\lambda^2}$ interpolating Poisson ($\\lambda=0$) and GOE ($\\lambda \\rightarrow \\infty$) we have analyzed the transition curves for $\\langle r\\rangle$ and $\\langle \\tilde{r}\\rangle$ as $\\lambda$ changes from $0$ to $\\infty$; $\\tilde{r} = min(r,1/r)$. Here, $V$ is a GOE ensemble of real symmet"},"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":"1405.6321","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-05-24T17:00:28Z","cross_cats_sorted":["nlin.CD","quant-ph"],"title_canon_sha256":"fc821ca2293e83a1d52cd27b9ddc435e3c300e3f989c686386ad7563510f9bec","abstract_canon_sha256":"6f54f9f8cddb879343b0e4b7a5ccce698af60b0e06bb4761d5f9e09994c45c08"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:43:06.682152Z","signature_b64":"4aE/TMK9WxrqwrZkpBGGZ0NXJK665Rrv9rvEeH1FfLwEZIENGvtIrw3I96G/txMVxoziPhpl8OHpPZhrlT4uAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9d155dfe47a55da8fdbfdf8fd25d62ddaef408eb6cf172e5226801866f7408ab","last_reissued_at":"2026-05-18T01:43:06.681226Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:43:06.681226Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Poisson to GOE transition in the distribution of the ratio of consecutive level spacings","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nlin.CD","quant-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"H. N. Deota, N. D. Chavda, V. K. B. Kota","submitted_at":"2014-05-24T17:00:28Z","abstract_excerpt":"Probability distribution for the ratio ($r$) of consecutive level spacings of the eigenvalues of a Poisson (generating regular spectra) spectrum and that of a GOE random matrix ensemble are given recently. Going beyond these, for the ensemble generated by the Hamiltonian $H_\\lambda = (H_0+\\lambda V)/\\sqrt{1+\\lambda^2}$ interpolating Poisson ($\\lambda=0$) and GOE ($\\lambda \\rightarrow \\infty$) we have analyzed the transition curves for $\\langle r\\rangle$ and $\\langle \\tilde{r}\\rangle$ as $\\lambda$ changes from $0$ to $\\infty$; $\\tilde{r} = min(r,1/r)$. Here, $V$ is a GOE ensemble of real symmet"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1405.6321","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":""},"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":"1405.6321","created_at":"2026-05-18T01:43:06.681382+00:00"},{"alias_kind":"arxiv_version","alias_value":"1405.6321v2","created_at":"2026-05-18T01:43:06.681382+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1405.6321","created_at":"2026-05-18T01:43:06.681382+00:00"},{"alias_kind":"pith_short_12","alias_value":"TUKV37SHUVO2","created_at":"2026-05-18T12:28:52.271510+00:00"},{"alias_kind":"pith_short_16","alias_value":"TUKV37SHUVO2R7N7","created_at":"2026-05-18T12:28:52.271510+00:00"},{"alias_kind":"pith_short_8","alias_value":"TUKV37SH","created_at":"2026-05-18T12:28:52.271510+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/TUKV37SHUVO2R7N736H5EXLC3W","json":"https://pith.science/pith/TUKV37SHUVO2R7N736H5EXLC3W.json","graph_json":"https://pith.science/api/pith-number/TUKV37SHUVO2R7N736H5EXLC3W/graph.json","events_json":"https://pith.science/api/pith-number/TUKV37SHUVO2R7N736H5EXLC3W/events.json","paper":"https://pith.science/paper/TUKV37SH"},"agent_actions":{"view_html":"https://pith.science/pith/TUKV37SHUVO2R7N736H5EXLC3W","download_json":"https://pith.science/pith/TUKV37SHUVO2R7N736H5EXLC3W.json","view_paper":"https://pith.science/paper/TUKV37SH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1405.6321&json=true","fetch_graph":"https://pith.science/api/pith-number/TUKV37SHUVO2R7N736H5EXLC3W/graph.json","fetch_events":"https://pith.science/api/pith-number/TUKV37SHUVO2R7N736H5EXLC3W/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TUKV37SHUVO2R7N736H5EXLC3W/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TUKV37SHUVO2R7N736H5EXLC3W/action/storage_attestation","attest_author":"https://pith.science/pith/TUKV37SHUVO2R7N736H5EXLC3W/action/author_attestation","sign_citation":"https://pith.science/pith/TUKV37SHUVO2R7N736H5EXLC3W/action/citation_signature","submit_replication":"https://pith.science/pith/TUKV37SHUVO2R7N736H5EXLC3W/action/replication_record"}},"created_at":"2026-05-18T01:43:06.681382+00:00","updated_at":"2026-05-18T01:43:06.681382+00:00"}