{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:UZRWVV5ERXX7AHY7VGMEKMRW6N","short_pith_number":"pith:UZRWVV5E","schema_version":"1.0","canonical_sha256":"a6636ad7a48deff01f1fa998453236f37fa87a267982901e8756e63d211fd82f","source":{"kind":"arxiv","id":"hep-ph/9909305","version":1},"attestation_state":"computed","paper":{"title":"Analytic Approach in Quantum Chromodynamics","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"D.V. Shirkov, I.L. Solovtsov","submitted_at":"1999-09-09T12:14:03Z","abstract_excerpt":"We investigate a new ``renormalization invariant analytic formulation'' of calculations in quantum chromodynamics, where the renormalization group summation is correlated with the analyticity with respect to the square of the transferred momentum $Q^2$. The expressions for the invariant charge and matrix elements are then modified such that the unphysical singularities of the ghost pole type do not appear at all, being by construction compensated by additional nonperturbative contributions. Using the new scheme, we show that the results of calculations for a number of physical processes are st"},"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-ph/9909305","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1999-09-09T12:14:03Z","cross_cats_sorted":[],"title_canon_sha256":"80294251e7adead6242a5b9987d342a5eba5dad1ac2b003fb0b11f85fc249b41","abstract_canon_sha256":"57a61522f9609ecf716967194601993394f0c44fa152d7743626e89742507290"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:14:28.384221Z","signature_b64":"optmvlHH1S9JiTLh6lZ6DQCdqKpVEIcNGPWPnTD+xBC6RXzdrBwqvwk1ghhLcLAeEnsjOgdi1cUNbXaALweSDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a6636ad7a48deff01f1fa998453236f37fa87a267982901e8756e63d211fd82f","last_reissued_at":"2026-07-04T16:14:28.383844Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:14:28.383844Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Analytic Approach in Quantum Chromodynamics","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"D.V. Shirkov, I.L. Solovtsov","submitted_at":"1999-09-09T12:14:03Z","abstract_excerpt":"We investigate a new ``renormalization invariant analytic formulation'' of calculations in quantum chromodynamics, where the renormalization group summation is correlated with the analyticity with respect to the square of the transferred momentum $Q^2$. The expressions for the invariant charge and matrix elements are then modified such that the unphysical singularities of the ghost pole type do not appear at all, being by construction compensated by additional nonperturbative contributions. Using the new scheme, we show that the results of calculations for a number of physical processes are st"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9909305","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/hep-ph/9909305/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":"hep-ph/9909305","created_at":"2026-07-04T16:14:28.383896+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9909305v1","created_at":"2026-07-04T16:14:28.383896+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9909305","created_at":"2026-07-04T16:14:28.383896+00:00"},{"alias_kind":"pith_short_12","alias_value":"UZRWVV5ERXX7","created_at":"2026-07-04T16:14:28.383896+00:00"},{"alias_kind":"pith_short_16","alias_value":"UZRWVV5ERXX7AHY7","created_at":"2026-07-04T16:14:28.383896+00:00"},{"alias_kind":"pith_short_8","alias_value":"UZRWVV5E","created_at":"2026-07-04T16:14:28.383896+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/UZRWVV5ERXX7AHY7VGMEKMRW6N","json":"https://pith.science/pith/UZRWVV5ERXX7AHY7VGMEKMRW6N.json","graph_json":"https://pith.science/api/pith-number/UZRWVV5ERXX7AHY7VGMEKMRW6N/graph.json","events_json":"https://pith.science/api/pith-number/UZRWVV5ERXX7AHY7VGMEKMRW6N/events.json","paper":"https://pith.science/paper/UZRWVV5E"},"agent_actions":{"view_html":"https://pith.science/pith/UZRWVV5ERXX7AHY7VGMEKMRW6N","download_json":"https://pith.science/pith/UZRWVV5ERXX7AHY7VGMEKMRW6N.json","view_paper":"https://pith.science/paper/UZRWVV5E","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9909305&json=true","fetch_graph":"https://pith.science/api/pith-number/UZRWVV5ERXX7AHY7VGMEKMRW6N/graph.json","fetch_events":"https://pith.science/api/pith-number/UZRWVV5ERXX7AHY7VGMEKMRW6N/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UZRWVV5ERXX7AHY7VGMEKMRW6N/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UZRWVV5ERXX7AHY7VGMEKMRW6N/action/storage_attestation","attest_author":"https://pith.science/pith/UZRWVV5ERXX7AHY7VGMEKMRW6N/action/author_attestation","sign_citation":"https://pith.science/pith/UZRWVV5ERXX7AHY7VGMEKMRW6N/action/citation_signature","submit_replication":"https://pith.science/pith/UZRWVV5ERXX7AHY7VGMEKMRW6N/action/replication_record"}},"created_at":"2026-07-04T16:14:28.383896+00:00","updated_at":"2026-07-04T16:14:28.383896+00:00"}