{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:27OV6L7RAERJMWK5IXSWSR2N6X","short_pith_number":"pith:27OV6L7R","canonical_record":{"source":{"id":"1303.0753","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-03-04T16:55:56Z","cross_cats_sorted":["math-ph","math.MP","nlin.SI"],"title_canon_sha256":"6c03c692998b06e8c3d2694ac6f5947bf2ac8ec54dc068b5c1d31e573b49def1","abstract_canon_sha256":"7bef7fafaf3435709e7c558caea92bba61746791e357a2f561038d7b15d8e700"},"schema_version":"1.0"},"canonical_sha256":"d7dd5f2ff1012296595d45e569474df5dfe43dfe0b3f69a4303f86cb4ce3310a","source":{"kind":"arxiv","id":"1303.0753","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.0753","created_at":"2026-05-18T03:04:06Z"},{"alias_kind":"arxiv_version","alias_value":"1303.0753v2","created_at":"2026-05-18T03:04:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.0753","created_at":"2026-05-18T03:04:06Z"},{"alias_kind":"pith_short_12","alias_value":"27OV6L7RAERJ","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_16","alias_value":"27OV6L7RAERJMWK5","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_8","alias_value":"27OV6L7R","created_at":"2026-05-18T12:27:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:27OV6L7RAERJMWK5IXSWSR2N6X","target":"record","payload":{"canonical_record":{"source":{"id":"1303.0753","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-03-04T16:55:56Z","cross_cats_sorted":["math-ph","math.MP","nlin.SI"],"title_canon_sha256":"6c03c692998b06e8c3d2694ac6f5947bf2ac8ec54dc068b5c1d31e573b49def1","abstract_canon_sha256":"7bef7fafaf3435709e7c558caea92bba61746791e357a2f561038d7b15d8e700"},"schema_version":"1.0"},"canonical_sha256":"d7dd5f2ff1012296595d45e569474df5dfe43dfe0b3f69a4303f86cb4ce3310a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:04:06.588411Z","signature_b64":"TARvIWhBTkcjDSEG8DctGkO2nhsH9Sin3t/mvPiVsMqFQxY2Tym8Fb/G7gAufLG76zlIkNbR3V+73oUeu5BSCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d7dd5f2ff1012296595d45e569474df5dfe43dfe0b3f69a4303f86cb4ce3310a","last_reissued_at":"2026-05-18T03:04:06.587930Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:04:06.587930Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1303.0753","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:04:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QHQcpkmP1ITd/p+CYSSV+tLXUbxdeXMP5g1xMH4Lo5+NZY9oUAsZ1V7NOzzJWA1eIzGwxZcMB/97dZEg0EbiDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T16:07:13.706519Z"},"content_sha256":"a4c3e686868569ab71facabfe5e9198b8268d10621fd1fdfd80e383798edfb59","schema_version":"1.0","event_id":"sha256:a4c3e686868569ab71facabfe5e9198b8268d10621fd1fdfd80e383798edfb59"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:27OV6L7RAERJMWK5IXSWSR2N6X","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Tau-functions for Quiver Gauge Theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP","nlin.SI"],"primary_cat":"hep-th","authors_text":"A.Marshakov","submitted_at":"2013-03-04T16:55:56Z","abstract_excerpt":"The prepotentials for the quiver supersymmetric gauge theories are defined as quasiclassical tau-functions, depending on two different sets of variables: the parameters of the UV gauge theory or the bare compexified couplings, and the vacuum condensates of the theory in IR. The bare couplings are introduced as periods on the UV base curve, and the consistency of corresponding gradient formulas for the tau-functions is proven using the Riemann bilinear relations. It is shown, that dependence of generalised prepotentials for the quiver gauge theories upon the bare couplings turns to coincide wit"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.0753","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:04:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oMCaW2S6ZFIujzimmP9mtQFZGDjqWlqNSKPF4nDoqcBkFRbsUdqZLK7d8EdDpOBo0qzcjAwF+PMdkHcG9YvdBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T16:07:13.707214Z"},"content_sha256":"7d4b872d1c25e6fef08b1596ad5810d6b6a5a1a700b069f6c31ef41a9bbde030","schema_version":"1.0","event_id":"sha256:7d4b872d1c25e6fef08b1596ad5810d6b6a5a1a700b069f6c31ef41a9bbde030"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/27OV6L7RAERJMWK5IXSWSR2N6X/bundle.json","state_url":"https://pith.science/pith/27OV6L7RAERJMWK5IXSWSR2N6X/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/27OV6L7RAERJMWK5IXSWSR2N6X/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-25T16:07:13Z","links":{"resolver":"https://pith.science/pith/27OV6L7RAERJMWK5IXSWSR2N6X","bundle":"https://pith.science/pith/27OV6L7RAERJMWK5IXSWSR2N6X/bundle.json","state":"https://pith.science/pith/27OV6L7RAERJMWK5IXSWSR2N6X/state.json","well_known_bundle":"https://pith.science/.well-known/pith/27OV6L7RAERJMWK5IXSWSR2N6X/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:27OV6L7RAERJMWK5IXSWSR2N6X","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"7bef7fafaf3435709e7c558caea92bba61746791e357a2f561038d7b15d8e700","cross_cats_sorted":["math-ph","math.MP","nlin.SI"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-03-04T16:55:56Z","title_canon_sha256":"6c03c692998b06e8c3d2694ac6f5947bf2ac8ec54dc068b5c1d31e573b49def1"},"schema_version":"1.0","source":{"id":"1303.0753","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.0753","created_at":"2026-05-18T03:04:06Z"},{"alias_kind":"arxiv_version","alias_value":"1303.0753v2","created_at":"2026-05-18T03:04:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.0753","created_at":"2026-05-18T03:04:06Z"},{"alias_kind":"pith_short_12","alias_value":"27OV6L7RAERJ","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_16","alias_value":"27OV6L7RAERJMWK5","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_8","alias_value":"27OV6L7R","created_at":"2026-05-18T12:27:30Z"}],"graph_snapshots":[{"event_id":"sha256:7d4b872d1c25e6fef08b1596ad5810d6b6a5a1a700b069f6c31ef41a9bbde030","target":"graph","created_at":"2026-05-18T03:04:06Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"The prepotentials for the quiver supersymmetric gauge theories are defined as quasiclassical tau-functions, depending on two different sets of variables: the parameters of the UV gauge theory or the bare compexified couplings, and the vacuum condensates of the theory in IR. The bare couplings are introduced as periods on the UV base curve, and the consistency of corresponding gradient formulas for the tau-functions is proven using the Riemann bilinear relations. It is shown, that dependence of generalised prepotentials for the quiver gauge theories upon the bare couplings turns to coincide wit","authors_text":"A.Marshakov","cross_cats":["math-ph","math.MP","nlin.SI"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-03-04T16:55:56Z","title":"Tau-functions for Quiver Gauge Theories"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.0753","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:a4c3e686868569ab71facabfe5e9198b8268d10621fd1fdfd80e383798edfb59","target":"record","created_at":"2026-05-18T03:04:06Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"7bef7fafaf3435709e7c558caea92bba61746791e357a2f561038d7b15d8e700","cross_cats_sorted":["math-ph","math.MP","nlin.SI"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-03-04T16:55:56Z","title_canon_sha256":"6c03c692998b06e8c3d2694ac6f5947bf2ac8ec54dc068b5c1d31e573b49def1"},"schema_version":"1.0","source":{"id":"1303.0753","kind":"arxiv","version":2}},"canonical_sha256":"d7dd5f2ff1012296595d45e569474df5dfe43dfe0b3f69a4303f86cb4ce3310a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d7dd5f2ff1012296595d45e569474df5dfe43dfe0b3f69a4303f86cb4ce3310a","first_computed_at":"2026-05-18T03:04:06.587930Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:04:06.587930Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"TARvIWhBTkcjDSEG8DctGkO2nhsH9Sin3t/mvPiVsMqFQxY2Tym8Fb/G7gAufLG76zlIkNbR3V+73oUeu5BSCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:04:06.588411Z","signed_message":"canonical_sha256_bytes"},"source_id":"1303.0753","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a4c3e686868569ab71facabfe5e9198b8268d10621fd1fdfd80e383798edfb59","sha256:7d4b872d1c25e6fef08b1596ad5810d6b6a5a1a700b069f6c31ef41a9bbde030"],"state_sha256":"b265ef6313ba58061889d59a1e27a93f3f7f9d4c57345e52d7f9df1e34462fa3"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SZmzIAr9ZvUhwLp2VoQ/tA4awZ9HXQG3W34ZjPyW14mXbMpLqxwlqITanpKKMNraSvyn8cItETKbbsbGDeM6DA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T16:07:13.711182Z","bundle_sha256":"52d8baa1dbafb657a6029d321e63a12fe841c7fc73ef070793d0b8f949984dbe"}}