{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:OZF3JRLS5PT6A6YU5XDMEFVXX6","short_pith_number":"pith:OZF3JRLS","schema_version":"1.0","canonical_sha256":"764bb4c572ebe7e07b14edc6c216b7bfb09237a15670939ed3a4dc8d81a1e516","source":{"kind":"arxiv","id":"2606.26450","version":1},"attestation_state":"computed","paper":{"title":"An Ultraviolet Finite Theory of Scalars","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Clifford Cheung, Francesco Calisto","submitted_at":"2026-06-24T23:23:49Z","abstract_excerpt":"We construct a theory of scalars that is free of short-distance infinities to all orders in perturbation theory. Loop divergences are neutralized by momentum-dependent interactions that are ghost free and polynomially bounded. The finite counterparts of the usual one-loop scalar self-energy and beta function are straightforwardly computed. In a variant of this model, the one-loop mass renormalization is zero due to an inversion that swaps the ultraviolet and the infrared."},"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":"2606.26450","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2026-06-24T23:23:49Z","cross_cats_sorted":[],"title_canon_sha256":"05512cc62ed27a69fd7f1a6e110f94ee260b3ba91c1896ed891ffaea7d42104a","abstract_canon_sha256":"452d7d6a88dd68ed6c962751d5d8751afc5ae7a0998fd9e27dca70a1fc371282"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-26T00:15:41.563102Z","signature_b64":"LClfRaXNIUZFqXIumb5CEIahY0GwGwN1COZJanwydEtGqxYY3ZTR45hufmOaLBp1br/YTylvSpXsnp4fgnXDAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"764bb4c572ebe7e07b14edc6c216b7bfb09237a15670939ed3a4dc8d81a1e516","last_reissued_at":"2026-06-26T00:15:41.562772Z","signature_status":"signed_v1","first_computed_at":"2026-06-26T00:15:41.562772Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"An Ultraviolet Finite Theory of Scalars","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Clifford Cheung, Francesco Calisto","submitted_at":"2026-06-24T23:23:49Z","abstract_excerpt":"We construct a theory of scalars that is free of short-distance infinities to all orders in perturbation theory. Loop divergences are neutralized by momentum-dependent interactions that are ghost free and polynomially bounded. The finite counterparts of the usual one-loop scalar self-energy and beta function are straightforwardly computed. In a variant of this model, the one-loop mass renormalization is zero due to an inversion that swaps the ultraviolet and the infrared."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.26450","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/2606.26450/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":"2606.26450","created_at":"2026-06-26T00:15:41.562824+00:00"},{"alias_kind":"arxiv_version","alias_value":"2606.26450v1","created_at":"2026-06-26T00:15:41.562824+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.26450","created_at":"2026-06-26T00:15:41.562824+00:00"},{"alias_kind":"pith_short_12","alias_value":"OZF3JRLS5PT6","created_at":"2026-06-26T00:15:41.562824+00:00"},{"alias_kind":"pith_short_16","alias_value":"OZF3JRLS5PT6A6YU","created_at":"2026-06-26T00:15:41.562824+00:00"},{"alias_kind":"pith_short_8","alias_value":"OZF3JRLS","created_at":"2026-06-26T00:15:41.562824+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/OZF3JRLS5PT6A6YU5XDMEFVXX6","json":"https://pith.science/pith/OZF3JRLS5PT6A6YU5XDMEFVXX6.json","graph_json":"https://pith.science/api/pith-number/OZF3JRLS5PT6A6YU5XDMEFVXX6/graph.json","events_json":"https://pith.science/api/pith-number/OZF3JRLS5PT6A6YU5XDMEFVXX6/events.json","paper":"https://pith.science/paper/OZF3JRLS"},"agent_actions":{"view_html":"https://pith.science/pith/OZF3JRLS5PT6A6YU5XDMEFVXX6","download_json":"https://pith.science/pith/OZF3JRLS5PT6A6YU5XDMEFVXX6.json","view_paper":"https://pith.science/paper/OZF3JRLS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2606.26450&json=true","fetch_graph":"https://pith.science/api/pith-number/OZF3JRLS5PT6A6YU5XDMEFVXX6/graph.json","fetch_events":"https://pith.science/api/pith-number/OZF3JRLS5PT6A6YU5XDMEFVXX6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OZF3JRLS5PT6A6YU5XDMEFVXX6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OZF3JRLS5PT6A6YU5XDMEFVXX6/action/storage_attestation","attest_author":"https://pith.science/pith/OZF3JRLS5PT6A6YU5XDMEFVXX6/action/author_attestation","sign_citation":"https://pith.science/pith/OZF3JRLS5PT6A6YU5XDMEFVXX6/action/citation_signature","submit_replication":"https://pith.science/pith/OZF3JRLS5PT6A6YU5XDMEFVXX6/action/replication_record"}},"created_at":"2026-06-26T00:15:41.562824+00:00","updated_at":"2026-06-26T00:15:41.562824+00:00"}