{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1997:4I4ZL34YZBUXHOOHZQ2WFYZ5EE","short_pith_number":"pith:4I4ZL34Y","canonical_record":{"source":{"id":"hep-th/9712054","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1997-12-05T07:02:05Z","cross_cats_sorted":[],"title_canon_sha256":"fe075df7b769376871f2cb5a2d1096775a3fac12235ef134d683c0199efdb826","abstract_canon_sha256":"daf4552545e57ec52f837a2b17ffc4860a4bc1f21219efa9bf7d02bcbedcf169"},"schema_version":"1.0"},"canonical_sha256":"e23995ef98c86973b9c7cc3562e33d2132dad637a88e68a8b820071ea9cfb56a","source":{"kind":"arxiv","id":"hep-th/9712054","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9712054","created_at":"2026-07-04T16:05:47Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9712054v2","created_at":"2026-07-04T16:05:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9712054","created_at":"2026-07-04T16:05:47Z"},{"alias_kind":"pith_short_12","alias_value":"4I4ZL34YZBUX","created_at":"2026-07-04T16:05:47Z"},{"alias_kind":"pith_short_16","alias_value":"4I4ZL34YZBUXHOOH","created_at":"2026-07-04T16:05:47Z"},{"alias_kind":"pith_short_8","alias_value":"4I4ZL34Y","created_at":"2026-07-04T16:05:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1997:4I4ZL34YZBUXHOOHZQ2WFYZ5EE","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/9712054","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1997-12-05T07:02:05Z","cross_cats_sorted":[],"title_canon_sha256":"fe075df7b769376871f2cb5a2d1096775a3fac12235ef134d683c0199efdb826","abstract_canon_sha256":"daf4552545e57ec52f837a2b17ffc4860a4bc1f21219efa9bf7d02bcbedcf169"},"schema_version":"1.0"},"canonical_sha256":"e23995ef98c86973b9c7cc3562e33d2132dad637a88e68a8b820071ea9cfb56a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:05:47.954876Z","signature_b64":"Cgy9AHZa1qd3IR+dlf6i67A7K3ktVrIoCRHJDisHvihWoQ65H3AScHZUBgjKaYSqjI7sPEg7jMb0bYVdo48QBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e23995ef98c86973b9c7cc3562e33d2132dad637a88e68a8b820071ea9cfb56a","last_reissued_at":"2026-07-04T16:05:47.954509Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:05:47.954509Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/9712054","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":"2026-07-04T16:05:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dD2IAbPnLiOO/yNgI9dJ0EvfnbXjoQLDngMOPQyee+uBjEerMGG2BvJx6OIxC6/GnAPCvSg2zPEX/e6L37dKAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-09T23:18:45.138328Z"},"content_sha256":"bed6c5eb2dc9294451d26106cbc33c2511b1f7eb2c5eb52ec9d48c7f81f01211","schema_version":"1.0","event_id":"sha256:bed6c5eb2dc9294451d26106cbc33c2511b1f7eb2c5eb52ec9d48c7f81f01211"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1997:4I4ZL34YZBUXHOOHZQ2WFYZ5EE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Renormalization Group Flow near the Superconformal Points in N=2 Supersymmetric Gauge Theories","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Naoto Yokoi, Takahiro Kubota","submitted_at":"1997-12-05T07:02:05Z","abstract_excerpt":"The behavior of the beta-function of the low-energy effective coupling in the N=2 supersymmetric SU(2) QCD with several massive matter hypermultiplets and in the SU(3) Yang-Mills theory is determined near the superconformal points in the moduli space. The renormalization group flow is unambiguously fixed by looking at limited types of deformation near the superconformal points. It is pointed out that the scaling dimension of the beta-function is controlled by the scaling behavior of moduli parameters and the relation between them is explicitly worked out. Our scaling dimensions of the beta-fun"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9712054","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/hep-th/9712054/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T16:05:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DvTbu3iHAIxuHcNUJtdzYbV/neMDAT8uq38zJj61HTIiDUBseSF7iYy1+Q0pqNkOI49u1uYAOFCAb/O2mbtIDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-09T23:18:45.139084Z"},"content_sha256":"cc70bfb39adfa30df48a1b523cdb88f06fc8730a50a00d22cc8cdd9609af3728","schema_version":"1.0","event_id":"sha256:cc70bfb39adfa30df48a1b523cdb88f06fc8730a50a00d22cc8cdd9609af3728"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4I4ZL34YZBUXHOOHZQ2WFYZ5EE/bundle.json","state_url":"https://pith.science/pith/4I4ZL34YZBUXHOOHZQ2WFYZ5EE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4I4ZL34YZBUXHOOHZQ2WFYZ5EE/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":"2026-08-09T23:18:45Z","links":{"resolver":"https://pith.science/pith/4I4ZL34YZBUXHOOHZQ2WFYZ5EE","bundle":"https://pith.science/pith/4I4ZL34YZBUXHOOHZQ2WFYZ5EE/bundle.json","state":"https://pith.science/pith/4I4ZL34YZBUXHOOHZQ2WFYZ5EE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4I4ZL34YZBUXHOOHZQ2WFYZ5EE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1997:4I4ZL34YZBUXHOOHZQ2WFYZ5EE","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":"daf4552545e57ec52f837a2b17ffc4860a4bc1f21219efa9bf7d02bcbedcf169","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"1997-12-05T07:02:05Z","title_canon_sha256":"fe075df7b769376871f2cb5a2d1096775a3fac12235ef134d683c0199efdb826"},"schema_version":"1.0","source":{"id":"hep-th/9712054","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9712054","created_at":"2026-07-04T16:05:47Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9712054v2","created_at":"2026-07-04T16:05:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9712054","created_at":"2026-07-04T16:05:47Z"},{"alias_kind":"pith_short_12","alias_value":"4I4ZL34YZBUX","created_at":"2026-07-04T16:05:47Z"},{"alias_kind":"pith_short_16","alias_value":"4I4ZL34YZBUXHOOH","created_at":"2026-07-04T16:05:47Z"},{"alias_kind":"pith_short_8","alias_value":"4I4ZL34Y","created_at":"2026-07-04T16:05:47Z"}],"graph_snapshots":[{"event_id":"sha256:cc70bfb39adfa30df48a1b523cdb88f06fc8730a50a00d22cc8cdd9609af3728","target":"graph","created_at":"2026-07-04T16:05:47Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-th/9712054/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The behavior of the beta-function of the low-energy effective coupling in the N=2 supersymmetric SU(2) QCD with several massive matter hypermultiplets and in the SU(3) Yang-Mills theory is determined near the superconformal points in the moduli space. The renormalization group flow is unambiguously fixed by looking at limited types of deformation near the superconformal points. It is pointed out that the scaling dimension of the beta-function is controlled by the scaling behavior of moduli parameters and the relation between them is explicitly worked out. Our scaling dimensions of the beta-fun","authors_text":"Naoto Yokoi, Takahiro Kubota","cross_cats":[],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"1997-12-05T07:02:05Z","title":"Renormalization Group Flow near the Superconformal Points in N=2 Supersymmetric Gauge Theories"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9712054","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:bed6c5eb2dc9294451d26106cbc33c2511b1f7eb2c5eb52ec9d48c7f81f01211","target":"record","created_at":"2026-07-04T16:05:47Z","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":"daf4552545e57ec52f837a2b17ffc4860a4bc1f21219efa9bf7d02bcbedcf169","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"1997-12-05T07:02:05Z","title_canon_sha256":"fe075df7b769376871f2cb5a2d1096775a3fac12235ef134d683c0199efdb826"},"schema_version":"1.0","source":{"id":"hep-th/9712054","kind":"arxiv","version":2}},"canonical_sha256":"e23995ef98c86973b9c7cc3562e33d2132dad637a88e68a8b820071ea9cfb56a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e23995ef98c86973b9c7cc3562e33d2132dad637a88e68a8b820071ea9cfb56a","first_computed_at":"2026-07-04T16:05:47.954509Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:05:47.954509Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Cgy9AHZa1qd3IR+dlf6i67A7K3ktVrIoCRHJDisHvihWoQ65H3AScHZUBgjKaYSqjI7sPEg7jMb0bYVdo48QBA==","signature_status":"signed_v1","signed_at":"2026-07-04T16:05:47.954876Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/9712054","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:bed6c5eb2dc9294451d26106cbc33c2511b1f7eb2c5eb52ec9d48c7f81f01211","sha256:cc70bfb39adfa30df48a1b523cdb88f06fc8730a50a00d22cc8cdd9609af3728"],"state_sha256":"f447644cdda562fa116b0ba35e1da860b6a7cb1e81905d9bf415195293fe6042"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GpIhfUNZoJngfhHiNXLvkIkSSkDSoV3uQODvhvDr0+Y7DU6BdZlMZ19ayaDIKM9dlk1lMP3reCISnoqrXGuCBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-09T23:18:45.145240Z","bundle_sha256":"5f0868e34fcdcef7fb2482f9f9db98df98b6ac9b8fa3e5c1c048176a31cbd5f5"}}