{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:M6TR77W3ZJ3B7ZNQ7ETPJWERLC","short_pith_number":"pith:M6TR77W3","canonical_record":{"source":{"id":"1405.3841","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-05-15T13:25:12Z","cross_cats_sorted":[],"title_canon_sha256":"29072525d4d675135b5a914eb7b7b940a694aef2cf682c090249363a32771877","abstract_canon_sha256":"348a2dfa1e922f8b114640e9cc52889ae4b8eb6a17d9e43508603201a151d196"},"schema_version":"1.0"},"canonical_sha256":"67a71ffedbca761fe5b0f926f4d891588d34e6b3dd6e6d3bf846702ea05bde46","source":{"kind":"arxiv","id":"1405.3841","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1405.3841","created_at":"2026-05-18T02:51:49Z"},{"alias_kind":"arxiv_version","alias_value":"1405.3841v1","created_at":"2026-05-18T02:51:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1405.3841","created_at":"2026-05-18T02:51:49Z"},{"alias_kind":"pith_short_12","alias_value":"M6TR77W3ZJ3B","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"M6TR77W3ZJ3B7ZNQ","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"M6TR77W3","created_at":"2026-05-18T12:28:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:M6TR77W3ZJ3B7ZNQ7ETPJWERLC","target":"record","payload":{"canonical_record":{"source":{"id":"1405.3841","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-05-15T13:25:12Z","cross_cats_sorted":[],"title_canon_sha256":"29072525d4d675135b5a914eb7b7b940a694aef2cf682c090249363a32771877","abstract_canon_sha256":"348a2dfa1e922f8b114640e9cc52889ae4b8eb6a17d9e43508603201a151d196"},"schema_version":"1.0"},"canonical_sha256":"67a71ffedbca761fe5b0f926f4d891588d34e6b3dd6e6d3bf846702ea05bde46","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:51:49.195461Z","signature_b64":"6yf5/CcuJAQynL50k+w/0NH5ZKn5eWkENq5WN2uBwbYYvU2EJYgM8j0+g5Gv/G49XSmKQHC80+8yV/dWqhbcBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"67a71ffedbca761fe5b0f926f4d891588d34e6b3dd6e6d3bf846702ea05bde46","last_reissued_at":"2026-05-18T02:51:49.195074Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:51:49.195074Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1405.3841","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:51:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LpKSXpNssZpvgPLQDeP+83IFkpt54e0l/uocpWntqigH1kK1njM5aExOIqoApklnkY3RcIhEWb4OJ79QgOQoAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T18:23:41.452469Z"},"content_sha256":"2fa09ab6fb2fa6d9354c084a8bafdcd13e6b0b4b38ba3fa817218cf89a6ec283","schema_version":"1.0","event_id":"sha256:2fa09ab6fb2fa6d9354c084a8bafdcd13e6b0b4b38ba3fa817218cf89a6ec283"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:M6TR77W3ZJ3B7ZNQ7ETPJWERLC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Prospects for bounds on electroweak and Higgs observables via scaling effects","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"David Marzocca","submitted_at":"2014-05-15T13:25:12Z","abstract_excerpt":"In these proceedings we briefly review the basic concepts underlying indirect bounds on the Wilson coefficients of some Standard Model dimension-6 operators, relevant to electroweak and Higgs observables, obtained via renormalization group (RG) mixing to strongly constrained observables. With the present data we derive RG-induced bounds, stronger than the direct constraints, on some Higgs couplings and anomalous triple gauge couplings. Any deviation from these bounds would suggest a particular pattern of correlations among the Wilson coefficients, thus offering a new window on the new physics "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1405.3841","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":""},"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":"2026-05-18T02:51:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"e9mzdkdjctqwoIaqBZBINCC84COzPsU+wzRRZTjL79ENMWyexmEc8cJqUpQop0bgb7v3DNiBtX9iMWee8Wc3BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T18:23:41.453172Z"},"content_sha256":"6c1e9ecbd7737160e8869691240baf652383e6013e0d982936ddce0633448003","schema_version":"1.0","event_id":"sha256:6c1e9ecbd7737160e8869691240baf652383e6013e0d982936ddce0633448003"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/M6TR77W3ZJ3B7ZNQ7ETPJWERLC/bundle.json","state_url":"https://pith.science/pith/M6TR77W3ZJ3B7ZNQ7ETPJWERLC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/M6TR77W3ZJ3B7ZNQ7ETPJWERLC/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":"2026-06-08T18:23:41Z","links":{"resolver":"https://pith.science/pith/M6TR77W3ZJ3B7ZNQ7ETPJWERLC","bundle":"https://pith.science/pith/M6TR77W3ZJ3B7ZNQ7ETPJWERLC/bundle.json","state":"https://pith.science/pith/M6TR77W3ZJ3B7ZNQ7ETPJWERLC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/M6TR77W3ZJ3B7ZNQ7ETPJWERLC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:M6TR77W3ZJ3B7ZNQ7ETPJWERLC","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":"348a2dfa1e922f8b114640e9cc52889ae4b8eb6a17d9e43508603201a151d196","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-05-15T13:25:12Z","title_canon_sha256":"29072525d4d675135b5a914eb7b7b940a694aef2cf682c090249363a32771877"},"schema_version":"1.0","source":{"id":"1405.3841","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1405.3841","created_at":"2026-05-18T02:51:49Z"},{"alias_kind":"arxiv_version","alias_value":"1405.3841v1","created_at":"2026-05-18T02:51:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1405.3841","created_at":"2026-05-18T02:51:49Z"},{"alias_kind":"pith_short_12","alias_value":"M6TR77W3ZJ3B","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"M6TR77W3ZJ3B7ZNQ","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"M6TR77W3","created_at":"2026-05-18T12:28:38Z"}],"graph_snapshots":[{"event_id":"sha256:6c1e9ecbd7737160e8869691240baf652383e6013e0d982936ddce0633448003","target":"graph","created_at":"2026-05-18T02:51:49Z","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"},"paper":{"abstract_excerpt":"In these proceedings we briefly review the basic concepts underlying indirect bounds on the Wilson coefficients of some Standard Model dimension-6 operators, relevant to electroweak and Higgs observables, obtained via renormalization group (RG) mixing to strongly constrained observables. With the present data we derive RG-induced bounds, stronger than the direct constraints, on some Higgs couplings and anomalous triple gauge couplings. Any deviation from these bounds would suggest a particular pattern of correlations among the Wilson coefficients, thus offering a new window on the new physics ","authors_text":"David Marzocca","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-05-15T13:25:12Z","title":"Prospects for bounds on electroweak and Higgs observables via scaling effects"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1405.3841","kind":"arxiv","version":1},"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":"sha256:2fa09ab6fb2fa6d9354c084a8bafdcd13e6b0b4b38ba3fa817218cf89a6ec283","target":"record","created_at":"2026-05-18T02:51:49Z","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":"348a2dfa1e922f8b114640e9cc52889ae4b8eb6a17d9e43508603201a151d196","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-05-15T13:25:12Z","title_canon_sha256":"29072525d4d675135b5a914eb7b7b940a694aef2cf682c090249363a32771877"},"schema_version":"1.0","source":{"id":"1405.3841","kind":"arxiv","version":1}},"canonical_sha256":"67a71ffedbca761fe5b0f926f4d891588d34e6b3dd6e6d3bf846702ea05bde46","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"67a71ffedbca761fe5b0f926f4d891588d34e6b3dd6e6d3bf846702ea05bde46","first_computed_at":"2026-05-18T02:51:49.195074Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:51:49.195074Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"6yf5/CcuJAQynL50k+w/0NH5ZKn5eWkENq5WN2uBwbYYvU2EJYgM8j0+g5Gv/G49XSmKQHC80+8yV/dWqhbcBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:51:49.195461Z","signed_message":"canonical_sha256_bytes"},"source_id":"1405.3841","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2fa09ab6fb2fa6d9354c084a8bafdcd13e6b0b4b38ba3fa817218cf89a6ec283","sha256:6c1e9ecbd7737160e8869691240baf652383e6013e0d982936ddce0633448003"],"state_sha256":"5e71c21dd55a9789702adcaf0895a5a47c2ed234d9886694872f7fcfb793f67e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jIuhvV1w56zsx/c8dE3SSLSRlzOQiltk16Lu1RINlwnoWFUvXU1f/wRRJo8KX9GtLANDbEzajAr5Qj2x0rc+DA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-08T18:23:41.456822Z","bundle_sha256":"dca7f72b3e14a15a1f1f5b2443cfd88908af7b97fc2d5c98e028fd0c849b7fb5"}}