{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1998:HLHDIQWK6FFYXMP6HE23VJIYGE","short_pith_number":"pith:HLHDIQWK","canonical_record":{"source":{"id":"hep-ph/9808328","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1998-08-14T09:54:33Z","cross_cats_sorted":[],"title_canon_sha256":"c41273fc55aed6095d11befb146a2890d177581840d0dacada0af406abf8d962","abstract_canon_sha256":"46a5d67fdc54f4f04c28e68515fa5b7504890d9fc7b550bea4c4180492b8fa28"},"schema_version":"1.0"},"canonical_sha256":"3ace3442caf14b8bb1fe3935baa518313612e2b9d4ffb435ec4688f2ef3a093d","source":{"kind":"arxiv","id":"hep-ph/9808328","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9808328","created_at":"2026-07-04T16:09:22Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9808328v2","created_at":"2026-07-04T16:09:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9808328","created_at":"2026-07-04T16:09:22Z"},{"alias_kind":"pith_short_12","alias_value":"HLHDIQWK6FFY","created_at":"2026-07-04T16:09:22Z"},{"alias_kind":"pith_short_16","alias_value":"HLHDIQWK6FFYXMP6","created_at":"2026-07-04T16:09:22Z"},{"alias_kind":"pith_short_8","alias_value":"HLHDIQWK","created_at":"2026-07-04T16:09:22Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1998:HLHDIQWK6FFYXMP6HE23VJIYGE","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9808328","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1998-08-14T09:54:33Z","cross_cats_sorted":[],"title_canon_sha256":"c41273fc55aed6095d11befb146a2890d177581840d0dacada0af406abf8d962","abstract_canon_sha256":"46a5d67fdc54f4f04c28e68515fa5b7504890d9fc7b550bea4c4180492b8fa28"},"schema_version":"1.0"},"canonical_sha256":"3ace3442caf14b8bb1fe3935baa518313612e2b9d4ffb435ec4688f2ef3a093d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:09:22.408363Z","signature_b64":"YXD6oxfdGDeOJxuPxTcF/EoE5hN8S/Y5xQGQvuc6tjEjApIYSKOLhGnTw28ZL0EDB40gFG6Sg3EbVEx5iB6BCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3ace3442caf14b8bb1fe3935baa518313612e2b9d4ffb435ec4688f2ef3a093d","last_reissued_at":"2026-07-04T16:09:22.407948Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:09:22.407948Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9808328","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T16:09:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0nTUkDE6MOvCROIkFSW6pGOwjxQqNuw0BQa0OPHiEtLcAaba/CAl12HsNxUitf1Jo8jWRDrBkKY1rsN8EqRiBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-27T07:53:29.876836Z"},"content_sha256":"e49592f36816cecfb1741e6039c2f3c401d1e0f2af8f45e9c3d69474d3342cb9","schema_version":"1.0","event_id":"sha256:e49592f36816cecfb1741e6039c2f3c401d1e0f2af8f45e9c3d69474d3342cb9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1998:HLHDIQWK6FFYXMP6HE23VJIYGE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Delta M_K and epsilon_K in SUSY at the Next-to-Leading order","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Donini, A. Masiero, A. Vladikas, E. Franco, G. Martinelli, I. Scimemi, L. Conti, L. Giusti, L. Silvestrini, M. Ciuchini, M. Talevi, V. Gimenez, V. Lubicz","submitted_at":"1998-08-14T09:54:33Z","abstract_excerpt":"We perform a Next-to-Leading order analysis of Delta S=2 processes beyond the Standard Model. Combining the recently computed NLO anomalous dimensions and the B parameters of the most general Delta S=2 effective Hamiltonian, we give an analytic formula for Delta M_K and epsilon_K in terms of the Wilson coefficients at the high energy scale. This expression can be used for any extension of the Standard Model with new heavy particles. Using this result, we consider gluino-mediated contributions to Delta S=2 transitions in general SUSY models and provide an improved analysis of the constraints on"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9808328","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/hep-ph/9808328/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T16:09:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mYBrWDHZAdTXhPoyeguEcAorI7rwrPpo4nN2nV/yo28vafAk0EihuXchKtAlpsb0ZNsOpv0DWGwr5P1jLYcADw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-27T07:53:29.877210Z"},"content_sha256":"ffef3fec5d97dcdc5bba2879e6d45fd211559b55b92b4d542eccce7c7680f86e","schema_version":"1.0","event_id":"sha256:ffef3fec5d97dcdc5bba2879e6d45fd211559b55b92b4d542eccce7c7680f86e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HLHDIQWK6FFYXMP6HE23VJIYGE/bundle.json","state_url":"https://pith.science/pith/HLHDIQWK6FFYXMP6HE23VJIYGE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HLHDIQWK6FFYXMP6HE23VJIYGE/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-07-27T07:53:29Z","links":{"resolver":"https://pith.science/pith/HLHDIQWK6FFYXMP6HE23VJIYGE","bundle":"https://pith.science/pith/HLHDIQWK6FFYXMP6HE23VJIYGE/bundle.json","state":"https://pith.science/pith/HLHDIQWK6FFYXMP6HE23VJIYGE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HLHDIQWK6FFYXMP6HE23VJIYGE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1998:HLHDIQWK6FFYXMP6HE23VJIYGE","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"46a5d67fdc54f4f04c28e68515fa5b7504890d9fc7b550bea4c4180492b8fa28","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1998-08-14T09:54:33Z","title_canon_sha256":"c41273fc55aed6095d11befb146a2890d177581840d0dacada0af406abf8d962"},"schema_version":"1.0","source":{"id":"hep-ph/9808328","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9808328","created_at":"2026-07-04T16:09:22Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9808328v2","created_at":"2026-07-04T16:09:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9808328","created_at":"2026-07-04T16:09:22Z"},{"alias_kind":"pith_short_12","alias_value":"HLHDIQWK6FFY","created_at":"2026-07-04T16:09:22Z"},{"alias_kind":"pith_short_16","alias_value":"HLHDIQWK6FFYXMP6","created_at":"2026-07-04T16:09:22Z"},{"alias_kind":"pith_short_8","alias_value":"HLHDIQWK","created_at":"2026-07-04T16:09:22Z"}],"graph_snapshots":[{"event_id":"sha256:ffef3fec5d97dcdc5bba2879e6d45fd211559b55b92b4d542eccce7c7680f86e","target":"graph","created_at":"2026-07-04T16:09:22Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-ph/9808328/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We perform a Next-to-Leading order analysis of Delta S=2 processes beyond the Standard Model. Combining the recently computed NLO anomalous dimensions and the B parameters of the most general Delta S=2 effective Hamiltonian, we give an analytic formula for Delta M_K and epsilon_K in terms of the Wilson coefficients at the high energy scale. This expression can be used for any extension of the Standard Model with new heavy particles. Using this result, we consider gluino-mediated contributions to Delta S=2 transitions in general SUSY models and provide an improved analysis of the constraints on","authors_text":"A. Donini, A. Masiero, A. Vladikas, E. Franco, G. Martinelli, I. Scimemi, L. Conti, L. Giusti, L. Silvestrini, M. Ciuchini, M. Talevi, V. Gimenez, V. Lubicz","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1998-08-14T09:54:33Z","title":"Delta M_K and epsilon_K in SUSY at the Next-to-Leading order"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9808328","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:e49592f36816cecfb1741e6039c2f3c401d1e0f2af8f45e9c3d69474d3342cb9","target":"record","created_at":"2026-07-04T16:09:22Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"46a5d67fdc54f4f04c28e68515fa5b7504890d9fc7b550bea4c4180492b8fa28","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1998-08-14T09:54:33Z","title_canon_sha256":"c41273fc55aed6095d11befb146a2890d177581840d0dacada0af406abf8d962"},"schema_version":"1.0","source":{"id":"hep-ph/9808328","kind":"arxiv","version":2}},"canonical_sha256":"3ace3442caf14b8bb1fe3935baa518313612e2b9d4ffb435ec4688f2ef3a093d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3ace3442caf14b8bb1fe3935baa518313612e2b9d4ffb435ec4688f2ef3a093d","first_computed_at":"2026-07-04T16:09:22.407948Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:09:22.407948Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"YXD6oxfdGDeOJxuPxTcF/EoE5hN8S/Y5xQGQvuc6tjEjApIYSKOLhGnTw28ZL0EDB40gFG6Sg3EbVEx5iB6BCQ==","signature_status":"signed_v1","signed_at":"2026-07-04T16:09:22.408363Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9808328","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e49592f36816cecfb1741e6039c2f3c401d1e0f2af8f45e9c3d69474d3342cb9","sha256:ffef3fec5d97dcdc5bba2879e6d45fd211559b55b92b4d542eccce7c7680f86e"],"state_sha256":"a2b812d0d7efbc41b86b25080a6174e5824e8471683b71919941edb484bbcf5c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"haukJtVFwmNFzzX/GiXn9yKSSXI0iBko/qjtcDuzQCgrChX2bkOhVyzF+aycPBNuPdhxTF+CvY13wqlfO7hPDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-27T07:53:29.879622Z","bundle_sha256":"3c1f72a71c6442d1afca036df11f563775a3fd549e22d3329804727a0005f3fa"}}