{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:XQTV6LGTPRFDJF7G4SFPOV2LR7","short_pith_number":"pith:XQTV6LGT","schema_version":"1.0","canonical_sha256":"bc275f2cd37c4a3497e6e48af7574b8ff1d1b913723aa763579f576dec5a8736","source":{"kind":"arxiv","id":"1907.04971","version":1},"attestation_state":"computed","paper":{"title":"Hanany-Witten Transition in Quantum Curves","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"Naotaka Kubo, Sanefumi Moriyama","submitted_at":"2019-07-11T01:40:25Z","abstract_excerpt":"It was known that the U$(N)^4$ super Chern-Simons matrix model describing the worldvolume theory of D3-branes with two NS5-branes and two $(1,k)$5-branes in IIB brane configuration (dual to M2-branes after taking the T-duality and the M-theory lift) corresponds to the $D_5$ quantum curve. For deformations of these two objects, on one hand the super Chern-Simons matrix model has three degrees of freedom (of relative rank deformations interpreted as fractional branes in brane configurations), while on the other hand the $D_5$ curve has five degrees of freedom (characterized by point configuratio"},"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":"1907.04971","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2019-07-11T01:40:25Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"f167ebe9d903f3c5d0aea98006936da6448f76deb4543d81b535f5fbf01f92f5","abstract_canon_sha256":"c7b81c0e5c0bb3257c99cc5c84f32ee9636c5f717d950044f5445fa043d40602"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:36:27.888572Z","signature_b64":"TIYwkEQam41WnVIMfxoVBFoyrl7aOOtBj075j56w2TMf5Yhmm1lBwaV8aGGzBFEe3sXEA5XKiOJPNLY+zWwgBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bc275f2cd37c4a3497e6e48af7574b8ff1d1b913723aa763579f576dec5a8736","last_reissued_at":"2026-07-05T00:36:27.888029Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:36:27.888029Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hanany-Witten Transition in Quantum Curves","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"Naotaka Kubo, Sanefumi Moriyama","submitted_at":"2019-07-11T01:40:25Z","abstract_excerpt":"It was known that the U$(N)^4$ super Chern-Simons matrix model describing the worldvolume theory of D3-branes with two NS5-branes and two $(1,k)$5-branes in IIB brane configuration (dual to M2-branes after taking the T-duality and the M-theory lift) corresponds to the $D_5$ quantum curve. For deformations of these two objects, on one hand the super Chern-Simons matrix model has three degrees of freedom (of relative rank deformations interpreted as fractional branes in brane configurations), while on the other hand the $D_5$ curve has five degrees of freedom (characterized by point configuratio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1907.04971","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/1907.04971/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":"1907.04971","created_at":"2026-07-05T00:36:27.888091+00:00"},{"alias_kind":"arxiv_version","alias_value":"1907.04971v1","created_at":"2026-07-05T00:36:27.888091+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1907.04971","created_at":"2026-07-05T00:36:27.888091+00:00"},{"alias_kind":"pith_short_12","alias_value":"XQTV6LGTPRFD","created_at":"2026-07-05T00:36:27.888091+00:00"},{"alias_kind":"pith_short_16","alias_value":"XQTV6LGTPRFDJF7G","created_at":"2026-07-05T00:36:27.888091+00:00"},{"alias_kind":"pith_short_8","alias_value":"XQTV6LGT","created_at":"2026-07-05T00:36:27.888091+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.19877","citing_title":"Factorized Quantum Curves and Minuscule Vertices in 3D Duality Cascades with FI Parameters","ref_index":51,"is_internal_anchor":false},{"citing_arxiv_id":"2603.19159","citing_title":"$S^3$ partition functions and Equivariant CY$_4 $/CY$_3$ correspondence from Quantum curves","ref_index":58,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XQTV6LGTPRFDJF7G4SFPOV2LR7","json":"https://pith.science/pith/XQTV6LGTPRFDJF7G4SFPOV2LR7.json","graph_json":"https://pith.science/api/pith-number/XQTV6LGTPRFDJF7G4SFPOV2LR7/graph.json","events_json":"https://pith.science/api/pith-number/XQTV6LGTPRFDJF7G4SFPOV2LR7/events.json","paper":"https://pith.science/paper/XQTV6LGT"},"agent_actions":{"view_html":"https://pith.science/pith/XQTV6LGTPRFDJF7G4SFPOV2LR7","download_json":"https://pith.science/pith/XQTV6LGTPRFDJF7G4SFPOV2LR7.json","view_paper":"https://pith.science/paper/XQTV6LGT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1907.04971&json=true","fetch_graph":"https://pith.science/api/pith-number/XQTV6LGTPRFDJF7G4SFPOV2LR7/graph.json","fetch_events":"https://pith.science/api/pith-number/XQTV6LGTPRFDJF7G4SFPOV2LR7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XQTV6LGTPRFDJF7G4SFPOV2LR7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XQTV6LGTPRFDJF7G4SFPOV2LR7/action/storage_attestation","attest_author":"https://pith.science/pith/XQTV6LGTPRFDJF7G4SFPOV2LR7/action/author_attestation","sign_citation":"https://pith.science/pith/XQTV6LGTPRFDJF7G4SFPOV2LR7/action/citation_signature","submit_replication":"https://pith.science/pith/XQTV6LGTPRFDJF7G4SFPOV2LR7/action/replication_record"}},"created_at":"2026-07-05T00:36:27.888091+00:00","updated_at":"2026-07-05T00:36:27.888091+00:00"}