{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:WGA3ZWTZOI6WELE5E5JBWRSQ4L","short_pith_number":"pith:WGA3ZWTZ","schema_version":"1.0","canonical_sha256":"b181bcda79723d622c9d27521b4650e2dd6e93b3f0f73c4dbbb19f851d4e6144","source":{"kind":"arxiv","id":"hep-th/0603122","version":2},"attestation_state":"computed","paper":{"title":"Double Scaling Limits in Gauge Theories and Matrix Models","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Gaetano Bertoldi, J. Luis Miramontes, Timothy J. Hollowood","submitted_at":"2006-03-15T19:54:54Z","abstract_excerpt":"We show that $\\N=1$ gauge theories with an adjoint chiral multiplet admit a wide class of large-N double-scaling limits where $N$ is taken to infinity in a way coordinated with a tuning of the bare superpotential. The tuning is such that the theory is near an Argyres-Douglas-type singularity where a set of non-local dibaryons becomes massless in conjunction with a set of confining strings becoming tensionless. The doubly-scaled theory consists of two decoupled sectors, one whose spectrum and interactions follow the usual large-N scaling whilst the other has light states of fixed mass in the la"},"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":"hep-th/0603122","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2006-03-15T19:54:54Z","cross_cats_sorted":[],"title_canon_sha256":"12160d22e79c1a4ef83ee3dd197cf95a18a5b1db39b1f2ecbc2c8edd5cb12c4f","abstract_canon_sha256":"848d9e74011e3d56afd05be3dcfc6270b7b71adfa5cd45ef81dc0178e29e96ec"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:34:10.364285Z","signature_b64":"DqVfEQFDbcraPURBgV3ZYN1lcUcTo5DD3W0feMXG2I3yPtbQ9Prfoa4acz17RA+hJlrl1PklVOKm92tw8pONDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b181bcda79723d622c9d27521b4650e2dd6e93b3f0f73c4dbbb19f851d4e6144","last_reissued_at":"2026-05-18T04:34:10.363787Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:34:10.363787Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Double Scaling Limits in Gauge Theories and Matrix Models","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Gaetano Bertoldi, J. Luis Miramontes, Timothy J. Hollowood","submitted_at":"2006-03-15T19:54:54Z","abstract_excerpt":"We show that $\\N=1$ gauge theories with an adjoint chiral multiplet admit a wide class of large-N double-scaling limits where $N$ is taken to infinity in a way coordinated with a tuning of the bare superpotential. The tuning is such that the theory is near an Argyres-Douglas-type singularity where a set of non-local dibaryons becomes massless in conjunction with a set of confining strings becoming tensionless. The doubly-scaled theory consists of two decoupled sectors, one whose spectrum and interactions follow the usual large-N scaling whilst the other has light states of fixed mass in the la"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0603122","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":"hep-th/0603122","created_at":"2026-05-18T04:34:10.363858+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0603122v2","created_at":"2026-05-18T04:34:10.363858+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0603122","created_at":"2026-05-18T04:34:10.363858+00:00"},{"alias_kind":"pith_short_12","alias_value":"WGA3ZWTZOI6W","created_at":"2026-05-18T12:25:54.717736+00:00"},{"alias_kind":"pith_short_16","alias_value":"WGA3ZWTZOI6WELE5","created_at":"2026-05-18T12:25:54.717736+00:00"},{"alias_kind":"pith_short_8","alias_value":"WGA3ZWTZ","created_at":"2026-05-18T12:25:54.717736+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/WGA3ZWTZOI6WELE5E5JBWRSQ4L","json":"https://pith.science/pith/WGA3ZWTZOI6WELE5E5JBWRSQ4L.json","graph_json":"https://pith.science/api/pith-number/WGA3ZWTZOI6WELE5E5JBWRSQ4L/graph.json","events_json":"https://pith.science/api/pith-number/WGA3ZWTZOI6WELE5E5JBWRSQ4L/events.json","paper":"https://pith.science/paper/WGA3ZWTZ"},"agent_actions":{"view_html":"https://pith.science/pith/WGA3ZWTZOI6WELE5E5JBWRSQ4L","download_json":"https://pith.science/pith/WGA3ZWTZOI6WELE5E5JBWRSQ4L.json","view_paper":"https://pith.science/paper/WGA3ZWTZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0603122&json=true","fetch_graph":"https://pith.science/api/pith-number/WGA3ZWTZOI6WELE5E5JBWRSQ4L/graph.json","fetch_events":"https://pith.science/api/pith-number/WGA3ZWTZOI6WELE5E5JBWRSQ4L/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WGA3ZWTZOI6WELE5E5JBWRSQ4L/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WGA3ZWTZOI6WELE5E5JBWRSQ4L/action/storage_attestation","attest_author":"https://pith.science/pith/WGA3ZWTZOI6WELE5E5JBWRSQ4L/action/author_attestation","sign_citation":"https://pith.science/pith/WGA3ZWTZOI6WELE5E5JBWRSQ4L/action/citation_signature","submit_replication":"https://pith.science/pith/WGA3ZWTZOI6WELE5E5JBWRSQ4L/action/replication_record"}},"created_at":"2026-05-18T04:34:10.363858+00:00","updated_at":"2026-05-18T04:34:10.363858+00:00"}