{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:7YL2RRSCCFFD32DQDIT6TDYQBP","short_pith_number":"pith:7YL2RRSC","schema_version":"1.0","canonical_sha256":"fe17a8c642114a3de8701a27e98f100beaec185f34d0134704f7fc45c1f92abb","source":{"kind":"arxiv","id":"1105.3487","version":1},"attestation_state":"computed","paper":{"title":"From N=4 gauge theory to N=2 conformal QCD: three-loop mixing of scalar composite operators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Christoph Sieg, Elli Pomoni","submitted_at":"2011-05-17T20:49:41Z","abstract_excerpt":"We derive the planar dilatation operator in the closed subsector of scalar composite operators of an N=2 superconformal quiver gauge theory to three loops. By tuning the ratio of its two gauge couplings we interpolate between a Z_2 orbifold of N=4 SYM theory and N=2 superconformal QCD. We find zeta(3) contributions at three loops that disappear when the theory is at the orbifold point. They are responsible for imaginary contributions to the dispersion relation of a single scalar excitation in the spin-chain picture. This points towards an interpretation of the individual scalar excitations as "},"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":"1105.3487","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-05-17T20:49:41Z","cross_cats_sorted":[],"title_canon_sha256":"54d1b02b6f77e3f6aaeb3b4c8410f2e7f81e01cdec007966ef1d0c5840e3bc6a","abstract_canon_sha256":"c71f1b60d17e102e3902f7938bdd32c84d1ad0ea2e51e2b93cb57242d85cc480"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:21:52.483148Z","signature_b64":"j5YwkOFyc1kV+rYW+KXdcJnLXtdElRovT7Vxhqkmey9ztF1rxtri/czqVlOXmkj3TbTg84b9mhyNdri05ATxAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fe17a8c642114a3de8701a27e98f100beaec185f34d0134704f7fc45c1f92abb","last_reissued_at":"2026-05-18T04:21:52.482488Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:21:52.482488Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"From N=4 gauge theory to N=2 conformal QCD: three-loop mixing of scalar composite operators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Christoph Sieg, Elli Pomoni","submitted_at":"2011-05-17T20:49:41Z","abstract_excerpt":"We derive the planar dilatation operator in the closed subsector of scalar composite operators of an N=2 superconformal quiver gauge theory to three loops. By tuning the ratio of its two gauge couplings we interpolate between a Z_2 orbifold of N=4 SYM theory and N=2 superconformal QCD. We find zeta(3) contributions at three loops that disappear when the theory is at the orbifold point. They are responsible for imaginary contributions to the dispersion relation of a single scalar excitation in the spin-chain picture. This points towards an interpretation of the individual scalar excitations as "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.3487","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":""},"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":"1105.3487","created_at":"2026-05-18T04:21:52.482592+00:00"},{"alias_kind":"arxiv_version","alias_value":"1105.3487v1","created_at":"2026-05-18T04:21:52.482592+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.3487","created_at":"2026-05-18T04:21:52.482592+00:00"},{"alias_kind":"pith_short_12","alias_value":"7YL2RRSCCFFD","created_at":"2026-05-18T12:26:22.705136+00:00"},{"alias_kind":"pith_short_16","alias_value":"7YL2RRSCCFFD32DQ","created_at":"2026-05-18T12:26:22.705136+00:00"},{"alias_kind":"pith_short_8","alias_value":"7YL2RRSC","created_at":"2026-05-18T12:26:22.705136+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.08934","citing_title":"Long-range to the Rescue of Yang-Baxter II","ref_index":13,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7YL2RRSCCFFD32DQDIT6TDYQBP","json":"https://pith.science/pith/7YL2RRSCCFFD32DQDIT6TDYQBP.json","graph_json":"https://pith.science/api/pith-number/7YL2RRSCCFFD32DQDIT6TDYQBP/graph.json","events_json":"https://pith.science/api/pith-number/7YL2RRSCCFFD32DQDIT6TDYQBP/events.json","paper":"https://pith.science/paper/7YL2RRSC"},"agent_actions":{"view_html":"https://pith.science/pith/7YL2RRSCCFFD32DQDIT6TDYQBP","download_json":"https://pith.science/pith/7YL2RRSCCFFD32DQDIT6TDYQBP.json","view_paper":"https://pith.science/paper/7YL2RRSC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1105.3487&json=true","fetch_graph":"https://pith.science/api/pith-number/7YL2RRSCCFFD32DQDIT6TDYQBP/graph.json","fetch_events":"https://pith.science/api/pith-number/7YL2RRSCCFFD32DQDIT6TDYQBP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7YL2RRSCCFFD32DQDIT6TDYQBP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7YL2RRSCCFFD32DQDIT6TDYQBP/action/storage_attestation","attest_author":"https://pith.science/pith/7YL2RRSCCFFD32DQDIT6TDYQBP/action/author_attestation","sign_citation":"https://pith.science/pith/7YL2RRSCCFFD32DQDIT6TDYQBP/action/citation_signature","submit_replication":"https://pith.science/pith/7YL2RRSCCFFD32DQDIT6TDYQBP/action/replication_record"}},"created_at":"2026-05-18T04:21:52.482592+00:00","updated_at":"2026-05-18T04:21:52.482592+00:00"}