{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:EVL6SBONINCW6CWQ72VRGXPRCH","short_pith_number":"pith:EVL6SBON","schema_version":"1.0","canonical_sha256":"2557e905cd43456f0ad0feab135df111db39fa31e77828ee5bfcc0489947d2c4","source":{"kind":"arxiv","id":"1311.3133","version":2},"attestation_state":"computed","paper":{"title":"Hadronic total cross sections at high energy and the QCD spectrum","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Enrico Meggiolaro, Matteo Giordano","submitted_at":"2013-11-13T14:04:21Z","abstract_excerpt":"We show how to obtain the leading energy dependence of hadronic total cross sections, in the framework of the nonperturbative approach to soft high-energy scattering based on Wilson-loop correlation functions, if certain nontrivial analyticity assumptions are satisfied. The total cross sections turn out to be of \"Froissart\" type, $\\sigma_{\\rm tot}^{(hh)}(s) \\mathop\\sim B\\log^2 s$ for ${s \\to\n  \\infty}$. We also discuss under which conditions the coefficient $B$ is universal, i.e., independent of the hadrons involved in the scattering process. In the most natural scenarios for universality, $B$"},"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":"1311.3133","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-11-13T14:04:21Z","cross_cats_sorted":[],"title_canon_sha256":"8f7e43a1b02ededd31f9fe199cf92a7028f0b508331249812e20632b7396f1df","abstract_canon_sha256":"b61e2d6a23c845382608b1b03b2ed0798b1560170e7f409586ad2bff8c219ca4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:56:05.035447Z","signature_b64":"gwLU+H9pJEBJCB2qUxMCfnGBMcwW5CxtS95+udAfgdR63UZhskREEk5qegfjLkG0fggcZzFPZRQjaySY0X5yCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2557e905cd43456f0ad0feab135df111db39fa31e77828ee5bfcc0489947d2c4","last_reissued_at":"2026-05-18T02:56:05.034991Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:56:05.034991Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hadronic total cross sections at high energy and the QCD spectrum","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Enrico Meggiolaro, Matteo Giordano","submitted_at":"2013-11-13T14:04:21Z","abstract_excerpt":"We show how to obtain the leading energy dependence of hadronic total cross sections, in the framework of the nonperturbative approach to soft high-energy scattering based on Wilson-loop correlation functions, if certain nontrivial analyticity assumptions are satisfied. The total cross sections turn out to be of \"Froissart\" type, $\\sigma_{\\rm tot}^{(hh)}(s) \\mathop\\sim B\\log^2 s$ for ${s \\to\n  \\infty}$. We also discuss under which conditions the coefficient $B$ is universal, i.e., independent of the hadrons involved in the scattering process. In the most natural scenarios for universality, $B$"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.3133","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":"1311.3133","created_at":"2026-05-18T02:56:05.035048+00:00"},{"alias_kind":"arxiv_version","alias_value":"1311.3133v2","created_at":"2026-05-18T02:56:05.035048+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.3133","created_at":"2026-05-18T02:56:05.035048+00:00"},{"alias_kind":"pith_short_12","alias_value":"EVL6SBONINCW","created_at":"2026-05-18T12:27:43.054852+00:00"},{"alias_kind":"pith_short_16","alias_value":"EVL6SBONINCW6CWQ","created_at":"2026-05-18T12:27:43.054852+00:00"},{"alias_kind":"pith_short_8","alias_value":"EVL6SBON","created_at":"2026-05-18T12:27:43.054852+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/EVL6SBONINCW6CWQ72VRGXPRCH","json":"https://pith.science/pith/EVL6SBONINCW6CWQ72VRGXPRCH.json","graph_json":"https://pith.science/api/pith-number/EVL6SBONINCW6CWQ72VRGXPRCH/graph.json","events_json":"https://pith.science/api/pith-number/EVL6SBONINCW6CWQ72VRGXPRCH/events.json","paper":"https://pith.science/paper/EVL6SBON"},"agent_actions":{"view_html":"https://pith.science/pith/EVL6SBONINCW6CWQ72VRGXPRCH","download_json":"https://pith.science/pith/EVL6SBONINCW6CWQ72VRGXPRCH.json","view_paper":"https://pith.science/paper/EVL6SBON","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1311.3133&json=true","fetch_graph":"https://pith.science/api/pith-number/EVL6SBONINCW6CWQ72VRGXPRCH/graph.json","fetch_events":"https://pith.science/api/pith-number/EVL6SBONINCW6CWQ72VRGXPRCH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EVL6SBONINCW6CWQ72VRGXPRCH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EVL6SBONINCW6CWQ72VRGXPRCH/action/storage_attestation","attest_author":"https://pith.science/pith/EVL6SBONINCW6CWQ72VRGXPRCH/action/author_attestation","sign_citation":"https://pith.science/pith/EVL6SBONINCW6CWQ72VRGXPRCH/action/citation_signature","submit_replication":"https://pith.science/pith/EVL6SBONINCW6CWQ72VRGXPRCH/action/replication_record"}},"created_at":"2026-05-18T02:56:05.035048+00:00","updated_at":"2026-05-18T02:56:05.035048+00:00"}