{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:CLH2XMFDZLWSX5FMYXWABLUDFG","short_pith_number":"pith:CLH2XMFD","schema_version":"1.0","canonical_sha256":"12cfabb0a3caed2bf4acc5ec00ae8329abd765b934235608651a4df6019dac70","source":{"kind":"arxiv","id":"1604.08013","version":2},"attestation_state":"computed","paper":{"title":"High-Energy Resummation in Di-hadron Production at the LHC","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 G. Celiberto","submitted_at":"2016-04-27T10:46:05Z","abstract_excerpt":"We propose to study at the Large Hadron Collider (LHC) the inclusive production of a pair of hadrons (a \"di-hadron\" system) in a kinematics where two detected hadrons with high transverse momenta are separated by a large interval of rapidity. This process has much in common with the widely discussed Mueller-Navelet jet production and can also be used to access the dynamics of hard proton-parton interactions in the Regge limit. For both processes large contributions enhanced by logarithms of energy can be resummed in perturbation theory within the Balitsky-Fadin-Kuraev-Lipatov (BFKL) formalism "},"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":"1604.08013","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-04-27T10:46:05Z","cross_cats_sorted":[],"title_canon_sha256":"da643828f61fe9a04344844367c471fcad093c14db75a3b83701174786f0ee98","abstract_canon_sha256":"8c5ebacf602af4983b6e5765ad2a37e436326681084eec550c1e7586329ff8c0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:09:31.991930Z","signature_b64":"83vDTqSEaSJVHA1IGr980uR2OdHh95FHJxjumWSaGyY+sJpNEcg0s2LRoUWPvoa5zHfjlUv7iX+4ygdpjLcWCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"12cfabb0a3caed2bf4acc5ec00ae8329abd765b934235608651a4df6019dac70","last_reissued_at":"2026-05-18T01:09:31.991583Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:09:31.991583Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"High-Energy Resummation in Di-hadron Production at the LHC","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 G. Celiberto","submitted_at":"2016-04-27T10:46:05Z","abstract_excerpt":"We propose to study at the Large Hadron Collider (LHC) the inclusive production of a pair of hadrons (a \"di-hadron\" system) in a kinematics where two detected hadrons with high transverse momenta are separated by a large interval of rapidity. This process has much in common with the widely discussed Mueller-Navelet jet production and can also be used to access the dynamics of hard proton-parton interactions in the Regge limit. For both processes large contributions enhanced by logarithms of energy can be resummed in perturbation theory within the Balitsky-Fadin-Kuraev-Lipatov (BFKL) formalism "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.08013","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":"1604.08013","created_at":"2026-05-18T01:09:31.991641+00:00"},{"alias_kind":"arxiv_version","alias_value":"1604.08013v2","created_at":"2026-05-18T01:09:31.991641+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.08013","created_at":"2026-05-18T01:09:31.991641+00:00"},{"alias_kind":"pith_short_12","alias_value":"CLH2XMFDZLWS","created_at":"2026-05-18T12:30:09.641336+00:00"},{"alias_kind":"pith_short_16","alias_value":"CLH2XMFDZLWSX5FM","created_at":"2026-05-18T12:30:09.641336+00:00"},{"alias_kind":"pith_short_8","alias_value":"CLH2XMFD","created_at":"2026-05-18T12:30:09.641336+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"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":27,"is_internal_anchor":true},{"citing_arxiv_id":"2605.01539","citing_title":"Multimodal Fragmentation of All-Heavy Pentaquarks: Uncertainty-Aware Predictions for Hadron Colliders","ref_index":168,"is_internal_anchor":false},{"citing_arxiv_id":"2604.11646","citing_title":"All-charm tetraquarks at hadron colliders: A high-precision fragmentation perspective","ref_index":242,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CLH2XMFDZLWSX5FMYXWABLUDFG","json":"https://pith.science/pith/CLH2XMFDZLWSX5FMYXWABLUDFG.json","graph_json":"https://pith.science/api/pith-number/CLH2XMFDZLWSX5FMYXWABLUDFG/graph.json","events_json":"https://pith.science/api/pith-number/CLH2XMFDZLWSX5FMYXWABLUDFG/events.json","paper":"https://pith.science/paper/CLH2XMFD"},"agent_actions":{"view_html":"https://pith.science/pith/CLH2XMFDZLWSX5FMYXWABLUDFG","download_json":"https://pith.science/pith/CLH2XMFDZLWSX5FMYXWABLUDFG.json","view_paper":"https://pith.science/paper/CLH2XMFD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1604.08013&json=true","fetch_graph":"https://pith.science/api/pith-number/CLH2XMFDZLWSX5FMYXWABLUDFG/graph.json","fetch_events":"https://pith.science/api/pith-number/CLH2XMFDZLWSX5FMYXWABLUDFG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CLH2XMFDZLWSX5FMYXWABLUDFG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CLH2XMFDZLWSX5FMYXWABLUDFG/action/storage_attestation","attest_author":"https://pith.science/pith/CLH2XMFDZLWSX5FMYXWABLUDFG/action/author_attestation","sign_citation":"https://pith.science/pith/CLH2XMFDZLWSX5FMYXWABLUDFG/action/citation_signature","submit_replication":"https://pith.science/pith/CLH2XMFDZLWSX5FMYXWABLUDFG/action/replication_record"}},"created_at":"2026-05-18T01:09:31.991641+00:00","updated_at":"2026-05-18T01:09:31.991641+00:00"}