{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:HQM4JJOGJ75RGUGOIAC47D5RQH","short_pith_number":"pith:HQM4JJOG","schema_version":"1.0","canonical_sha256":"3c19c4a5c64ffb1350ce4005cf8fb181ed4b509650268ef519c93f0d6e0c0359","source":{"kind":"arxiv","id":"2005.10563","version":2},"attestation_state":"computed","paper":{"title":"Elliptic lift of the Shiraishi function as a non-stationary double-elliptic function","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP","math.QA"],"primary_cat":"hep-th","authors_text":"A. Mironov, A. Morozov, H. Awata, H. Kanno","submitted_at":"2020-05-21T10:47:21Z","abstract_excerpt":"As a development of arXiv:1912.12897, we note that the ordinary Shiraishi functions have an insufficient number of parameters to describe generic eigenfunctions of double elliptic system (Dell). The lacking parameter can be provided by substituting elliptic instead of the ordinary Gamma functions in the coefficients of the series. These new functions (ELS-functions) are conjectured to be functions governed by compactified DIM networks which can simultaneously play the three roles: solutions to non-stationary Dell equations, Dell conformal blocks with the degenerate field (surface operator) ins"},"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":"2005.10563","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2020-05-21T10:47:21Z","cross_cats_sorted":["math-ph","math.MP","math.QA"],"title_canon_sha256":"3fb3bc43ac6a13810c53019083c1ac39caf47ab127cb004da48294bf6ae46f88","abstract_canon_sha256":"5381ccc727a4b55e0f3ddaa2ef6bae5a20f0dc9cc720ef8dc7247565070753cc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:32:44.896440Z","signature_b64":"U+In9O17jBErjnC4rUqevg72HuSBViUZ16xmLYMutRUsmnOcR0TA2sX2cuTJzK35TgoOEZNCu+SttOc8GZMjCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3c19c4a5c64ffb1350ce4005cf8fb181ed4b509650268ef519c93f0d6e0c0359","last_reissued_at":"2026-07-05T01:32:44.896091Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:32:44.896091Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Elliptic lift of the Shiraishi function as a non-stationary double-elliptic function","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP","math.QA"],"primary_cat":"hep-th","authors_text":"A. Mironov, A. Morozov, H. Awata, H. Kanno","submitted_at":"2020-05-21T10:47:21Z","abstract_excerpt":"As a development of arXiv:1912.12897, we note that the ordinary Shiraishi functions have an insufficient number of parameters to describe generic eigenfunctions of double elliptic system (Dell). The lacking parameter can be provided by substituting elliptic instead of the ordinary Gamma functions in the coefficients of the series. These new functions (ELS-functions) are conjectured to be functions governed by compactified DIM networks which can simultaneously play the three roles: solutions to non-stationary Dell equations, Dell conformal blocks with the degenerate field (surface operator) ins"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2005.10563","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/2005.10563/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":"2005.10563","created_at":"2026-07-05T01:32:44.896147+00:00"},{"alias_kind":"arxiv_version","alias_value":"2005.10563v2","created_at":"2026-07-05T01:32:44.896147+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2005.10563","created_at":"2026-07-05T01:32:44.896147+00:00"},{"alias_kind":"pith_short_12","alias_value":"HQM4JJOGJ75R","created_at":"2026-07-05T01:32:44.896147+00:00"},{"alias_kind":"pith_short_16","alias_value":"HQM4JJOGJ75RGUGO","created_at":"2026-07-05T01:32:44.896147+00:00"},{"alias_kind":"pith_short_8","alias_value":"HQM4JJOG","created_at":"2026-07-05T01:32:44.896147+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.06738","citing_title":"Integrable systems inspired by DAHA and DIM algebra: type $C^\\vee C$ versus type $A$","ref_index":71,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HQM4JJOGJ75RGUGOIAC47D5RQH","json":"https://pith.science/pith/HQM4JJOGJ75RGUGOIAC47D5RQH.json","graph_json":"https://pith.science/api/pith-number/HQM4JJOGJ75RGUGOIAC47D5RQH/graph.json","events_json":"https://pith.science/api/pith-number/HQM4JJOGJ75RGUGOIAC47D5RQH/events.json","paper":"https://pith.science/paper/HQM4JJOG"},"agent_actions":{"view_html":"https://pith.science/pith/HQM4JJOGJ75RGUGOIAC47D5RQH","download_json":"https://pith.science/pith/HQM4JJOGJ75RGUGOIAC47D5RQH.json","view_paper":"https://pith.science/paper/HQM4JJOG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2005.10563&json=true","fetch_graph":"https://pith.science/api/pith-number/HQM4JJOGJ75RGUGOIAC47D5RQH/graph.json","fetch_events":"https://pith.science/api/pith-number/HQM4JJOGJ75RGUGOIAC47D5RQH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HQM4JJOGJ75RGUGOIAC47D5RQH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HQM4JJOGJ75RGUGOIAC47D5RQH/action/storage_attestation","attest_author":"https://pith.science/pith/HQM4JJOGJ75RGUGOIAC47D5RQH/action/author_attestation","sign_citation":"https://pith.science/pith/HQM4JJOGJ75RGUGOIAC47D5RQH/action/citation_signature","submit_replication":"https://pith.science/pith/HQM4JJOGJ75RGUGOIAC47D5RQH/action/replication_record"}},"created_at":"2026-07-05T01:32:44.896147+00:00","updated_at":"2026-07-05T01:32:44.896147+00:00"}