{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:U2DFDVWM2XYYNQCR72BHJJQOQI","short_pith_number":"pith:U2DFDVWM","schema_version":"1.0","canonical_sha256":"a68651d6ccd5f186c051fe8274a60e8230b694eb2187bd614bcea2f810f245a6","source":{"kind":"arxiv","id":"2404.05491","version":2},"attestation_state":"computed","paper":{"title":"Rewording Theoretical Predictions at Colliders with Vacuum Amplitudes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-th"],"primary_cat":"hep-ph","authors_text":"German F.R. Sborlini, Germ\\'an Rodrigo, Prasanna K. Dhani, Selomit Ram\\'irez-Uribe","submitted_at":"2024-04-08T13:12:04Z","abstract_excerpt":"We propose multiloop vacuum amplitudes as the optimal building blocks for efficiently assembling theoretical predictions at high-energy colliders. This hypothesis is strongly supported by the manifestly causal properties of the loop-tree duality (LTD) representation of a vacuum amplitude. The vacuum amplitude, acting as a kernel, encodes all the final states contributing to a given scattering or decay process through residues in the on-shell energies of the internal propagators. It also naturally implements gauge invariance and the wave function renormalisation of the external legs. This metho"},"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":"2404.05491","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-04-08T13:12:04Z","cross_cats_sorted":["hep-ex","hep-th"],"title_canon_sha256":"d7e0eec97d4c18fa8faebc744ee8f5f7a21073b314842e52a296bce05b755f98","abstract_canon_sha256":"39e8ef3fde8269cf6a2bba5eea52f3d3da0a20ac8ffca7357ff68b762bf70cb7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:44:33.848249Z","signature_b64":"yIf0dUJKDNLhZYmCnQHjRYkij1wIwmOAjfc7tcYFNbNpUGGWQbHS88Bw6664sl0JfUSQdx3mqQrlEuztgH4ZCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a68651d6ccd5f186c051fe8274a60e8230b694eb2187bd614bcea2f810f245a6","last_reissued_at":"2026-07-05T09:44:33.847771Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:44:33.847771Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Rewording Theoretical Predictions at Colliders with Vacuum Amplitudes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-th"],"primary_cat":"hep-ph","authors_text":"German F.R. Sborlini, Germ\\'an Rodrigo, Prasanna K. Dhani, Selomit Ram\\'irez-Uribe","submitted_at":"2024-04-08T13:12:04Z","abstract_excerpt":"We propose multiloop vacuum amplitudes as the optimal building blocks for efficiently assembling theoretical predictions at high-energy colliders. This hypothesis is strongly supported by the manifestly causal properties of the loop-tree duality (LTD) representation of a vacuum amplitude. The vacuum amplitude, acting as a kernel, encodes all the final states contributing to a given scattering or decay process through residues in the on-shell energies of the internal propagators. It also naturally implements gauge invariance and the wave function renormalisation of the external legs. This metho"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2404.05491","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/2404.05491/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":"2404.05491","created_at":"2026-07-05T09:44:33.847828+00:00"},{"alias_kind":"arxiv_version","alias_value":"2404.05491v2","created_at":"2026-07-05T09:44:33.847828+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2404.05491","created_at":"2026-07-05T09:44:33.847828+00:00"},{"alias_kind":"pith_short_12","alias_value":"U2DFDVWM2XYY","created_at":"2026-07-05T09:44:33.847828+00:00"},{"alias_kind":"pith_short_16","alias_value":"U2DFDVWM2XYYNQCR","created_at":"2026-07-05T09:44:33.847828+00:00"},{"alias_kind":"pith_short_8","alias_value":"U2DFDVWM","created_at":"2026-07-05T09:44:33.847828+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.08169","citing_title":"Overview of Applications of Quantum Computing in QCD","ref_index":27,"is_internal_anchor":true},{"citing_arxiv_id":"2606.02702","citing_title":"Perturbative construction of amplitudes from on-shell trees with vacuum pairs: the all-plus four-gluon amplitude through order $\\boldsymbol{g}^{\\boldsymbol{6}}$","ref_index":32,"is_internal_anchor":false},{"citing_arxiv_id":"2504.06689","citing_title":"Les Houches 2023 -- Physics at TeV Colliders: Report on the Standard Model Precision Wishlist","ref_index":127,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/U2DFDVWM2XYYNQCR72BHJJQOQI","json":"https://pith.science/pith/U2DFDVWM2XYYNQCR72BHJJQOQI.json","graph_json":"https://pith.science/api/pith-number/U2DFDVWM2XYYNQCR72BHJJQOQI/graph.json","events_json":"https://pith.science/api/pith-number/U2DFDVWM2XYYNQCR72BHJJQOQI/events.json","paper":"https://pith.science/paper/U2DFDVWM"},"agent_actions":{"view_html":"https://pith.science/pith/U2DFDVWM2XYYNQCR72BHJJQOQI","download_json":"https://pith.science/pith/U2DFDVWM2XYYNQCR72BHJJQOQI.json","view_paper":"https://pith.science/paper/U2DFDVWM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2404.05491&json=true","fetch_graph":"https://pith.science/api/pith-number/U2DFDVWM2XYYNQCR72BHJJQOQI/graph.json","fetch_events":"https://pith.science/api/pith-number/U2DFDVWM2XYYNQCR72BHJJQOQI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/U2DFDVWM2XYYNQCR72BHJJQOQI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/U2DFDVWM2XYYNQCR72BHJJQOQI/action/storage_attestation","attest_author":"https://pith.science/pith/U2DFDVWM2XYYNQCR72BHJJQOQI/action/author_attestation","sign_citation":"https://pith.science/pith/U2DFDVWM2XYYNQCR72BHJJQOQI/action/citation_signature","submit_replication":"https://pith.science/pith/U2DFDVWM2XYYNQCR72BHJJQOQI/action/replication_record"}},"created_at":"2026-07-05T09:44:33.847828+00:00","updated_at":"2026-07-05T09:44:33.847828+00:00"}