{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:DBN6BEL4JQEMPUP6PTIRNLN34S","short_pith_number":"pith:DBN6BEL4","schema_version":"1.0","canonical_sha256":"185be0917c4c08c7d1fe7cd116adbbe49f866f16c6dfcbd765d5faff23fb70c8","source":{"kind":"arxiv","id":"1407.8431","version":3},"attestation_state":"computed","paper":{"title":"Mueller-Navelet jets in next-to-leading order BFKL: theory versus experiment","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alessandro Papa, Beatrice Murdaca, Dmitry Yu. Ivanov, Francesco Caporale","submitted_at":"2014-07-31T14:22:48Z","abstract_excerpt":"We study, within QCD collinear factorization and including BFKL resummation at the next-to-leading order, the production of Mueller-Navelet jets at LHC with center-of-mass energy of 7 TeV. The adopted jet vertices are calculated in the approximation of small aperture of the jet cone in the pseudorapidity-azimuthal angle plane. We consider several representations of the dijet cross section, differing only beyond the next-to-leading order, to calculate a few observables related with this process. We use various methods of optimization to fix the energy scales entering the perturbative calculatio"},"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":"1407.8431","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-31T14:22:48Z","cross_cats_sorted":[],"title_canon_sha256":"20078c6d86b2e2f55316bc971979553c11295cd56d3c6b07c21708d830305b32","abstract_canon_sha256":"bf2e6ca712e4ce6a886e90bdabaf0f9c472bec1788a0b8c0edc861febdf96920"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:22:43.462270Z","signature_b64":"+i2kEoPN1Iberff4mTgb2HLUZAlXFKiAHLfi7YdjZgEAa59Z7zvProiFRYcjdr9bkolYmXoOpqyMPTBMHncwCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"185be0917c4c08c7d1fe7cd116adbbe49f866f16c6dfcbd765d5faff23fb70c8","last_reissued_at":"2026-05-18T01:22:43.461747Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:22:43.461747Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Mueller-Navelet jets in next-to-leading order BFKL: theory versus experiment","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alessandro Papa, Beatrice Murdaca, Dmitry Yu. Ivanov, Francesco Caporale","submitted_at":"2014-07-31T14:22:48Z","abstract_excerpt":"We study, within QCD collinear factorization and including BFKL resummation at the next-to-leading order, the production of Mueller-Navelet jets at LHC with center-of-mass energy of 7 TeV. The adopted jet vertices are calculated in the approximation of small aperture of the jet cone in the pseudorapidity-azimuthal angle plane. We consider several representations of the dijet cross section, differing only beyond the next-to-leading order, to calculate a few observables related with this process. We use various methods of optimization to fix the energy scales entering the perturbative calculatio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.8431","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":""},"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":"1407.8431","created_at":"2026-05-18T01:22:43.461827+00:00"},{"alias_kind":"arxiv_version","alias_value":"1407.8431v3","created_at":"2026-05-18T01:22:43.461827+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.8431","created_at":"2026-05-18T01:22:43.461827+00:00"},{"alias_kind":"pith_short_12","alias_value":"DBN6BEL4JQEM","created_at":"2026-05-18T12:28:25.294606+00:00"},{"alias_kind":"pith_short_16","alias_value":"DBN6BEL4JQEMPUP6","created_at":"2026-05-18T12:28:25.294606+00:00"},{"alias_kind":"pith_short_8","alias_value":"DBN6BEL4","created_at":"2026-05-18T12:28:25.294606+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1906.11800","citing_title":"High-energy effects in forward inclusive dijet and hadron-jet production","ref_index":18,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/DBN6BEL4JQEMPUP6PTIRNLN34S","json":"https://pith.science/pith/DBN6BEL4JQEMPUP6PTIRNLN34S.json","graph_json":"https://pith.science/api/pith-number/DBN6BEL4JQEMPUP6PTIRNLN34S/graph.json","events_json":"https://pith.science/api/pith-number/DBN6BEL4JQEMPUP6PTIRNLN34S/events.json","paper":"https://pith.science/paper/DBN6BEL4"},"agent_actions":{"view_html":"https://pith.science/pith/DBN6BEL4JQEMPUP6PTIRNLN34S","download_json":"https://pith.science/pith/DBN6BEL4JQEMPUP6PTIRNLN34S.json","view_paper":"https://pith.science/paper/DBN6BEL4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1407.8431&json=true","fetch_graph":"https://pith.science/api/pith-number/DBN6BEL4JQEMPUP6PTIRNLN34S/graph.json","fetch_events":"https://pith.science/api/pith-number/DBN6BEL4JQEMPUP6PTIRNLN34S/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DBN6BEL4JQEMPUP6PTIRNLN34S/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DBN6BEL4JQEMPUP6PTIRNLN34S/action/storage_attestation","attest_author":"https://pith.science/pith/DBN6BEL4JQEMPUP6PTIRNLN34S/action/author_attestation","sign_citation":"https://pith.science/pith/DBN6BEL4JQEMPUP6PTIRNLN34S/action/citation_signature","submit_replication":"https://pith.science/pith/DBN6BEL4JQEMPUP6PTIRNLN34S/action/replication_record"}},"created_at":"2026-05-18T01:22:43.461827+00:00","updated_at":"2026-05-18T01:22:43.461827+00:00"}