{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2003:7SLT5VNRWICCGVX66GOEL253D7","short_pith_number":"pith:7SLT5VNR","schema_version":"1.0","canonical_sha256":"fc973ed5b1b2042356fef19c45ebbb1fdde3dbffea5af170f559bc5dbb1a8ac6","source":{"kind":"arxiv","id":"hep-ph/0305132","version":3},"attestation_state":"computed","paper":{"title":"One-Loop Helicity Amplitudes for Parton Level Virtual Compton Scattering","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"H. W. Huang, T. Morii","submitted_at":"2003-05-13T03:40:10Z","abstract_excerpt":"We calculate the one-loop QCD virtual corrections to all helicity amplitudes for parton level virtual Compton scattering processes. We include the amplitudes both on quark target process $\\gamma^* q\\to\\gamma q$ and on gluon target process $\\gamma^*g\\to\\gamma g$. The infrared pole structure of the amplitudes is in agreement with the prediction of Catani's general formalism for the singularities of one-loop amplitudes, while expressions for the finite remainder are given in terms of logarithms and dilogarithms that are real in the physical region."},"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/0305132","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2003-05-13T03:40:10Z","cross_cats_sorted":[],"title_canon_sha256":"d1d02969947238166077d5b64f7c6958b5fd1c5d8eb75322cb02b43f1475a415","abstract_canon_sha256":"2fbd970d1b06c0ae72974edff3a1c89874e2a5a0c184d29ae68b77a7faf213c0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:40:44.319383Z","signature_b64":"jsoSDtVYFiohyTv1xdZKA0npsIoDHzl59uctoKISw8eOu6KRTupyMOkw3p7gDWeJ1SD0pSiAu1b5I+125HRyDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fc973ed5b1b2042356fef19c45ebbb1fdde3dbffea5af170f559bc5dbb1a8ac6","last_reissued_at":"2026-07-04T16:40:44.318974Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:40:44.318974Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"One-Loop Helicity Amplitudes for Parton Level Virtual Compton Scattering","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"H. W. Huang, T. Morii","submitted_at":"2003-05-13T03:40:10Z","abstract_excerpt":"We calculate the one-loop QCD virtual corrections to all helicity amplitudes for parton level virtual Compton scattering processes. We include the amplitudes both on quark target process $\\gamma^* q\\to\\gamma q$ and on gluon target process $\\gamma^*g\\to\\gamma g$. The infrared pole structure of the amplitudes is in agreement with the prediction of Catani's general formalism for the singularities of one-loop amplitudes, while expressions for the finite remainder are given in terms of logarithms and dilogarithms that are real in the physical region."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0305132","kind":"arxiv","version":3},"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/0305132/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/0305132","created_at":"2026-07-04T16:40:44.319025+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0305132v3","created_at":"2026-07-04T16:40:44.319025+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0305132","created_at":"2026-07-04T16:40:44.319025+00:00"},{"alias_kind":"pith_short_12","alias_value":"7SLT5VNRWICC","created_at":"2026-07-04T16:40:44.319025+00:00"},{"alias_kind":"pith_short_16","alias_value":"7SLT5VNRWICCGVX6","created_at":"2026-07-04T16:40:44.319025+00:00"},{"alias_kind":"pith_short_8","alias_value":"7SLT5VNR","created_at":"2026-07-04T16:40:44.319025+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2608.05330","citing_title":"Photon-nucleon entanglement in Compton scattering at low and high energies","ref_index":71,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7SLT5VNRWICCGVX66GOEL253D7","json":"https://pith.science/pith/7SLT5VNRWICCGVX66GOEL253D7.json","graph_json":"https://pith.science/api/pith-number/7SLT5VNRWICCGVX66GOEL253D7/graph.json","events_json":"https://pith.science/api/pith-number/7SLT5VNRWICCGVX66GOEL253D7/events.json","paper":"https://pith.science/paper/7SLT5VNR"},"agent_actions":{"view_html":"https://pith.science/pith/7SLT5VNRWICCGVX66GOEL253D7","download_json":"https://pith.science/pith/7SLT5VNRWICCGVX66GOEL253D7.json","view_paper":"https://pith.science/paper/7SLT5VNR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0305132&json=true","fetch_graph":"https://pith.science/api/pith-number/7SLT5VNRWICCGVX66GOEL253D7/graph.json","fetch_events":"https://pith.science/api/pith-number/7SLT5VNRWICCGVX66GOEL253D7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7SLT5VNRWICCGVX66GOEL253D7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7SLT5VNRWICCGVX66GOEL253D7/action/storage_attestation","attest_author":"https://pith.science/pith/7SLT5VNRWICCGVX66GOEL253D7/action/author_attestation","sign_citation":"https://pith.science/pith/7SLT5VNRWICCGVX66GOEL253D7/action/citation_signature","submit_replication":"https://pith.science/pith/7SLT5VNRWICCGVX66GOEL253D7/action/replication_record"}},"created_at":"2026-07-04T16:40:44.319025+00:00","updated_at":"2026-07-04T16:40:44.319025+00:00"}