{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:PMSS7255IV5Y4AN4S53DOSRHFR","short_pith_number":"pith:PMSS7255","schema_version":"1.0","canonical_sha256":"7b252febbd457b8e01bc9776374a272c460520ff8659d1ba3dab0183e9a688c6","source":{"kind":"arxiv","id":"hep-ph/0510031","version":2},"attestation_state":"computed","paper":{"title":"Analytic Properties of Hard Exclusive Amplitudes","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"O.V. Teryaev","submitted_at":"2005-10-03T17:45:41Z","abstract_excerpt":"Analytic properties of hard exclusive processes described by Generalized Parton Distributions (GPD's) are considered. The analytic continuation of GPD is provided by Generalized Distribution Amplitudes (GDA). The GDA's for the production of two $\\rho-$mesons may give an access to four-quark exotic states. The crucial role in the proof of analyticity is played by the Cavalieri conditions (polynomiality), resulting in the \"holographic\" property of GPD, when the full information about various hard processes is contained in the one dimensional sections ($x=\\pm \\xi$)of GPD. The applicability of ana"},"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/0510031","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2005-10-03T17:45:41Z","cross_cats_sorted":[],"title_canon_sha256":"02f7c163329faa47bd6b15c134993dc31f6a1b07c311f83bee306f1da3ae1ee9","abstract_canon_sha256":"57d61064c4ec4cb5ce9c2801090b5c9dff3c86cd86e64217348c7ae443964794"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:51:08.048741Z","signature_b64":"0IYjRNcSUExmnW/OfM0S++90IOnW/4KEEH3qcBeL0Uy4KjGo9jrtctPJpWJ38jrkyPMhJVCKy7OhKrAXWZZeAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7b252febbd457b8e01bc9776374a272c460520ff8659d1ba3dab0183e9a688c6","last_reissued_at":"2026-07-04T14:51:08.048404Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:51:08.048404Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Analytic Properties of Hard Exclusive Amplitudes","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"O.V. Teryaev","submitted_at":"2005-10-03T17:45:41Z","abstract_excerpt":"Analytic properties of hard exclusive processes described by Generalized Parton Distributions (GPD's) are considered. The analytic continuation of GPD is provided by Generalized Distribution Amplitudes (GDA). The GDA's for the production of two $\\rho-$mesons may give an access to four-quark exotic states. The crucial role in the proof of analyticity is played by the Cavalieri conditions (polynomiality), resulting in the \"holographic\" property of GPD, when the full information about various hard processes is contained in the one dimensional sections ($x=\\pm \\xi$)of GPD. The applicability of ana"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0510031","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-ph/0510031/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/0510031","created_at":"2026-07-04T14:51:08.048453+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0510031v2","created_at":"2026-07-04T14:51:08.048453+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0510031","created_at":"2026-07-04T14:51:08.048453+00:00"},{"alias_kind":"pith_short_12","alias_value":"PMSS7255IV5Y","created_at":"2026-07-04T14:51:08.048453+00:00"},{"alias_kind":"pith_short_16","alias_value":"PMSS7255IV5Y4AN4","created_at":"2026-07-04T14:51:08.048453+00:00"},{"alias_kind":"pith_short_8","alias_value":"PMSS7255","created_at":"2026-07-04T14:51:08.048453+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2606.09152","citing_title":"Constraining DVCS Compton Form Factors Using Lattice QCD informed Neural Network","ref_index":27,"is_internal_anchor":true},{"citing_arxiv_id":"1906.09419","citing_title":"Physics with Positron Beams at Jefferson Lab 12 GeV","ref_index":58,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PMSS7255IV5Y4AN4S53DOSRHFR","json":"https://pith.science/pith/PMSS7255IV5Y4AN4S53DOSRHFR.json","graph_json":"https://pith.science/api/pith-number/PMSS7255IV5Y4AN4S53DOSRHFR/graph.json","events_json":"https://pith.science/api/pith-number/PMSS7255IV5Y4AN4S53DOSRHFR/events.json","paper":"https://pith.science/paper/PMSS7255"},"agent_actions":{"view_html":"https://pith.science/pith/PMSS7255IV5Y4AN4S53DOSRHFR","download_json":"https://pith.science/pith/PMSS7255IV5Y4AN4S53DOSRHFR.json","view_paper":"https://pith.science/paper/PMSS7255","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0510031&json=true","fetch_graph":"https://pith.science/api/pith-number/PMSS7255IV5Y4AN4S53DOSRHFR/graph.json","fetch_events":"https://pith.science/api/pith-number/PMSS7255IV5Y4AN4S53DOSRHFR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PMSS7255IV5Y4AN4S53DOSRHFR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PMSS7255IV5Y4AN4S53DOSRHFR/action/storage_attestation","attest_author":"https://pith.science/pith/PMSS7255IV5Y4AN4S53DOSRHFR/action/author_attestation","sign_citation":"https://pith.science/pith/PMSS7255IV5Y4AN4S53DOSRHFR/action/citation_signature","submit_replication":"https://pith.science/pith/PMSS7255IV5Y4AN4S53DOSRHFR/action/replication_record"}},"created_at":"2026-07-04T14:51:08.048453+00:00","updated_at":"2026-07-04T14:51:08.048453+00:00"}