{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:NGFXK4BDSRAL3U6MU7ZKKRJ673","short_pith_number":"pith:NGFXK4BD","schema_version":"1.0","canonical_sha256":"698b7570239440bdd3cca7f2a5453efecbdd52f6246b9891339ae0a66050b30c","source":{"kind":"arxiv","id":"2506.17127","version":1},"attestation_state":"computed","paper":{"title":"Soft and semihard components of multiplicity distributions in the $k_T$ factorization approach","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"F. S. Navarra, H. R. Martins-Fontes","submitted_at":"2025-06-20T16:28:45Z","abstract_excerpt":"Particle production in hadronic collisions can be studied in the low-momentum (soft) and high-momentum (hard) transfer regimes. While the latter can be well understood with in perturbative QCD the former contains non-perturbative effects which cannot be calculated from first principles. There is also an intermediate regime called semihard, in which the momentum transfer runs typically from $~1$ to $~10$ GeV. As the hadron-hadron collision energy increases, we expect to see a relative growth of the number of semihard events. It has been conjectured that this growth would be the cause of some ch"},"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":"2506.17127","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-06-20T16:28:45Z","cross_cats_sorted":[],"title_canon_sha256":"60fa9abce29b0f653b525cbcfb1e00373d64bb8cd7a73c9446c7badb41b20791","abstract_canon_sha256":"126b1a7d5ece302dea71e36fb52668e4007763a5c24896ec1168529bd504c9dc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:24:56.747502Z","signature_b64":"2XwKN0euw2JZ4kIrVBWecy1W4jQlLervOKF8krAdl8taKDOV8P+K856gGrhJ52o6178nzKNsYzfD7/6WazuVDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"698b7570239440bdd3cca7f2a5453efecbdd52f6246b9891339ae0a66050b30c","last_reissued_at":"2026-07-05T11:24:56.747069Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:24:56.747069Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Soft and semihard components of multiplicity distributions in the $k_T$ factorization approach","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"F. S. Navarra, H. R. Martins-Fontes","submitted_at":"2025-06-20T16:28:45Z","abstract_excerpt":"Particle production in hadronic collisions can be studied in the low-momentum (soft) and high-momentum (hard) transfer regimes. While the latter can be well understood with in perturbative QCD the former contains non-perturbative effects which cannot be calculated from first principles. There is also an intermediate regime called semihard, in which the momentum transfer runs typically from $~1$ to $~10$ GeV. As the hadron-hadron collision energy increases, we expect to see a relative growth of the number of semihard events. It has been conjectured that this growth would be the cause of some ch"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2506.17127","kind":"arxiv","version":1},"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/2506.17127/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":"2506.17127","created_at":"2026-07-05T11:24:56.747125+00:00"},{"alias_kind":"arxiv_version","alias_value":"2506.17127v1","created_at":"2026-07-05T11:24:56.747125+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2506.17127","created_at":"2026-07-05T11:24:56.747125+00:00"},{"alias_kind":"pith_short_12","alias_value":"NGFXK4BDSRAL","created_at":"2026-07-05T11:24:56.747125+00:00"},{"alias_kind":"pith_short_16","alias_value":"NGFXK4BDSRAL3U6M","created_at":"2026-07-05T11:24:56.747125+00:00"},{"alias_kind":"pith_short_8","alias_value":"NGFXK4BD","created_at":"2026-07-05T11:24:56.747125+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/NGFXK4BDSRAL3U6MU7ZKKRJ673","json":"https://pith.science/pith/NGFXK4BDSRAL3U6MU7ZKKRJ673.json","graph_json":"https://pith.science/api/pith-number/NGFXK4BDSRAL3U6MU7ZKKRJ673/graph.json","events_json":"https://pith.science/api/pith-number/NGFXK4BDSRAL3U6MU7ZKKRJ673/events.json","paper":"https://pith.science/paper/NGFXK4BD"},"agent_actions":{"view_html":"https://pith.science/pith/NGFXK4BDSRAL3U6MU7ZKKRJ673","download_json":"https://pith.science/pith/NGFXK4BDSRAL3U6MU7ZKKRJ673.json","view_paper":"https://pith.science/paper/NGFXK4BD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2506.17127&json=true","fetch_graph":"https://pith.science/api/pith-number/NGFXK4BDSRAL3U6MU7ZKKRJ673/graph.json","fetch_events":"https://pith.science/api/pith-number/NGFXK4BDSRAL3U6MU7ZKKRJ673/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NGFXK4BDSRAL3U6MU7ZKKRJ673/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NGFXK4BDSRAL3U6MU7ZKKRJ673/action/storage_attestation","attest_author":"https://pith.science/pith/NGFXK4BDSRAL3U6MU7ZKKRJ673/action/author_attestation","sign_citation":"https://pith.science/pith/NGFXK4BDSRAL3U6MU7ZKKRJ673/action/citation_signature","submit_replication":"https://pith.science/pith/NGFXK4BDSRAL3U6MU7ZKKRJ673/action/replication_record"}},"created_at":"2026-07-05T11:24:56.747125+00:00","updated_at":"2026-07-05T11:24:56.747125+00:00"}