{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:RJ6Z2O5RAWSRTVBDG2SQHCUGSZ","short_pith_number":"pith:RJ6Z2O5R","schema_version":"1.0","canonical_sha256":"8a7d9d3bb105a519d42336a5038a8696748945e2b8de34e2fbe25c44dcf0ffac","source":{"kind":"arxiv","id":"2304.11915","version":2},"attestation_state":"computed","paper":{"title":"Electroweak superpartner production at 13.6 TeV with Resummino","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Neuwirth, B. Fuks, J. Fiaschi, M. Klasen","submitted_at":"2023-04-24T08:46:13Z","abstract_excerpt":"Due to the greater experimental precision expected from the currently ongoing LHC Run 3, equally accurate theoretical predictions are essential. We update the documentation of the Resummino package, a program dedicated to precision cross section calculations for the production of a pair of sleptons, electroweakinos, and leptons in the presence of extra gauge bosons, and for the production of an associated electroweakino-squark or electroweakino-gluino pair. We detail different additions that have been released since the initial version of the program a decade ago, and then use the code to inve"},"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":"2304.11915","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2023-04-24T08:46:13Z","cross_cats_sorted":[],"title_canon_sha256":"869f9bb1ccf0a74e6a1cc5493b02966203caa7da956a7f99e5eb04d148f76d46","abstract_canon_sha256":"e7214a48f96de891c6d0c498ebb6b86cd44192425cddad2674cac7449efd6748"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:38:54.577922Z","signature_b64":"yHG0jPzUhtcW/UXcBeORLkKGIKGMFopvaQfgmDotl5ietnuS2s0+vMkzTf5+DSIBEJh6KPvBqc7Mjbya4AkpBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8a7d9d3bb105a519d42336a5038a8696748945e2b8de34e2fbe25c44dcf0ffac","last_reissued_at":"2026-07-05T06:38:54.577443Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:38:54.577443Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electroweak superpartner production at 13.6 TeV with Resummino","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Neuwirth, B. Fuks, J. Fiaschi, M. Klasen","submitted_at":"2023-04-24T08:46:13Z","abstract_excerpt":"Due to the greater experimental precision expected from the currently ongoing LHC Run 3, equally accurate theoretical predictions are essential. We update the documentation of the Resummino package, a program dedicated to precision cross section calculations for the production of a pair of sleptons, electroweakinos, and leptons in the presence of extra gauge bosons, and for the production of an associated electroweakino-squark or electroweakino-gluino pair. We detail different additions that have been released since the initial version of the program a decade ago, and then use the code to inve"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2304.11915","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/2304.11915/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":"2304.11915","created_at":"2026-07-05T06:38:54.577501+00:00"},{"alias_kind":"arxiv_version","alias_value":"2304.11915v2","created_at":"2026-07-05T06:38:54.577501+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2304.11915","created_at":"2026-07-05T06:38:54.577501+00:00"},{"alias_kind":"pith_short_12","alias_value":"RJ6Z2O5RAWSR","created_at":"2026-07-05T06:38:54.577501+00:00"},{"alias_kind":"pith_short_16","alias_value":"RJ6Z2O5RAWSRTVBD","created_at":"2026-07-05T06:38:54.577501+00:00"},{"alias_kind":"pith_short_8","alias_value":"RJ6Z2O5R","created_at":"2026-07-05T06:38:54.577501+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2507.08927","citing_title":"Deciphering compressed electroweakino excesses with MadAnalysis 5","ref_index":81,"is_internal_anchor":false},{"citing_arxiv_id":"2510.07397","citing_title":"Slepton pair production at next-to-leading power","ref_index":18,"is_internal_anchor":false},{"citing_arxiv_id":"2605.13819","citing_title":"Search for charginos and neutralinos with $B-L$ $R$-parity violating decays in $\\sqrt{s}=13$ TeV and $13.6$ TeV $pp$ collisions with the ATLAS detector","ref_index":38,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RJ6Z2O5RAWSRTVBDG2SQHCUGSZ","json":"https://pith.science/pith/RJ6Z2O5RAWSRTVBDG2SQHCUGSZ.json","graph_json":"https://pith.science/api/pith-number/RJ6Z2O5RAWSRTVBDG2SQHCUGSZ/graph.json","events_json":"https://pith.science/api/pith-number/RJ6Z2O5RAWSRTVBDG2SQHCUGSZ/events.json","paper":"https://pith.science/paper/RJ6Z2O5R"},"agent_actions":{"view_html":"https://pith.science/pith/RJ6Z2O5RAWSRTVBDG2SQHCUGSZ","download_json":"https://pith.science/pith/RJ6Z2O5RAWSRTVBDG2SQHCUGSZ.json","view_paper":"https://pith.science/paper/RJ6Z2O5R","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2304.11915&json=true","fetch_graph":"https://pith.science/api/pith-number/RJ6Z2O5RAWSRTVBDG2SQHCUGSZ/graph.json","fetch_events":"https://pith.science/api/pith-number/RJ6Z2O5RAWSRTVBDG2SQHCUGSZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RJ6Z2O5RAWSRTVBDG2SQHCUGSZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RJ6Z2O5RAWSRTVBDG2SQHCUGSZ/action/storage_attestation","attest_author":"https://pith.science/pith/RJ6Z2O5RAWSRTVBDG2SQHCUGSZ/action/author_attestation","sign_citation":"https://pith.science/pith/RJ6Z2O5RAWSRTVBDG2SQHCUGSZ/action/citation_signature","submit_replication":"https://pith.science/pith/RJ6Z2O5RAWSRTVBDG2SQHCUGSZ/action/replication_record"}},"created_at":"2026-07-05T06:38:54.577501+00:00","updated_at":"2026-07-05T06:38:54.577501+00:00"}