{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:3774FMI4BW2X64UEZOWAFQG2JA","short_pith_number":"pith:3774FMI4","canonical_record":{"source":{"id":"1112.3112","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-12-14T04:12:15Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"c7a6a943041af00dd92fab506b2191ca069b46c19fb59e243f89b9c4adba694d","abstract_canon_sha256":"0574bb6b68d4c7d8dfd7d4fcc9e8c29f768d83528aec84ebe8936f797f9e3c59"},"schema_version":"1.0"},"canonical_sha256":"dfffc2b11c0db57f7284cbac02c0da481d95ddb4d3a8c534b31832dcec9a6a9b","source":{"kind":"arxiv","id":"1112.3112","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1112.3112","created_at":"2026-05-18T01:59:10Z"},{"alias_kind":"arxiv_version","alias_value":"1112.3112v2","created_at":"2026-05-18T01:59:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.3112","created_at":"2026-05-18T01:59:10Z"},{"alias_kind":"pith_short_12","alias_value":"3774FMI4BW2X","created_at":"2026-05-18T12:26:18Z"},{"alias_kind":"pith_short_16","alias_value":"3774FMI4BW2X64UE","created_at":"2026-05-18T12:26:18Z"},{"alias_kind":"pith_short_8","alias_value":"3774FMI4","created_at":"2026-05-18T12:26:18Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:3774FMI4BW2X64UEZOWAFQG2JA","target":"record","payload":{"canonical_record":{"source":{"id":"1112.3112","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-12-14T04:12:15Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"c7a6a943041af00dd92fab506b2191ca069b46c19fb59e243f89b9c4adba694d","abstract_canon_sha256":"0574bb6b68d4c7d8dfd7d4fcc9e8c29f768d83528aec84ebe8936f797f9e3c59"},"schema_version":"1.0"},"canonical_sha256":"dfffc2b11c0db57f7284cbac02c0da481d95ddb4d3a8c534b31832dcec9a6a9b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:59:10.380633Z","signature_b64":"UIiGRBoeO6LLunewxk7+CHEn7PimwmXF+EIoVtmwLUsNPKG4i201+XJzEyZJrhGntQ3NoEQmeGX9/EfPh54mDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dfffc2b11c0db57f7284cbac02c0da481d95ddb4d3a8c534b31832dcec9a6a9b","last_reissued_at":"2026-05-18T01:59:10.380115Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:59:10.380115Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1112.3112","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":"2026-05-18T01:59:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wA/jyh8Ct9h+ty73w6z08m2yFYt2ygENdqeJOa4tW0/WY0+s29KBFAZicfHQ+lKmeFzkJ9v2/G1QEt3qMNd5DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-24T03:05:31.107909Z"},"content_sha256":"21145345fc306cce6c46c2caf6554b9208c604a5b050e5319d500143e6972e08","schema_version":"1.0","event_id":"sha256:21145345fc306cce6c46c2caf6554b9208c604a5b050e5319d500143e6972e08"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:3774FMI4BW2X64UEZOWAFQG2JA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Impacts of the Higgs mass on vacuum stability, running fermion masses and two-body Higgs decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"He Zhang, Shun Zhou, Zhi-zhong Xing","submitted_at":"2011-12-14T04:12:15Z","abstract_excerpt":"The latest results of the ATLAS and CMS experiments indicate 116 GeV \\lesssim M_H \\lesssim 131 GeV and 115 GeV \\lesssim M_H \\lesssim 127 GeV, respectively, for the mass of the Higgs boson in the standard model (SM) at the 95% confidence level. In particular, both experiments point to a preferred narrow mass range M_H \\simeq (124 ... 126) GeV. We examine the impact of this preliminary result of M_H on the SM vacuum stability by using the two-loop renormalization-group equations (RGEs), and arrive at the cutoff scale \\Lambda_VS \\sim 4 \\times 10^{12} GeV (for M_H = 125 GeV, M_t = 172.9 GeV and \\a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.3112","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":""},"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":"2026-05-18T01:59:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PJhSQPXOfuDt6WnvbYiRH7Jfq1+AlNBH6yc9EKUN20DyVa6jd9LEwb/wK/pwxlsxzapL5L2xGmekk3k5F1c+BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-24T03:05:31.108264Z"},"content_sha256":"3c11a7e6d64091ec5953eab95744860bc7ddc34f96d91d02efd4183f12ae26c2","schema_version":"1.0","event_id":"sha256:3c11a7e6d64091ec5953eab95744860bc7ddc34f96d91d02efd4183f12ae26c2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3774FMI4BW2X64UEZOWAFQG2JA/bundle.json","state_url":"https://pith.science/pith/3774FMI4BW2X64UEZOWAFQG2JA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3774FMI4BW2X64UEZOWAFQG2JA/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":"2026-05-24T03:05:31Z","links":{"resolver":"https://pith.science/pith/3774FMI4BW2X64UEZOWAFQG2JA","bundle":"https://pith.science/pith/3774FMI4BW2X64UEZOWAFQG2JA/bundle.json","state":"https://pith.science/pith/3774FMI4BW2X64UEZOWAFQG2JA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3774FMI4BW2X64UEZOWAFQG2JA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:3774FMI4BW2X64UEZOWAFQG2JA","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":"0574bb6b68d4c7d8dfd7d4fcc9e8c29f768d83528aec84ebe8936f797f9e3c59","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-12-14T04:12:15Z","title_canon_sha256":"c7a6a943041af00dd92fab506b2191ca069b46c19fb59e243f89b9c4adba694d"},"schema_version":"1.0","source":{"id":"1112.3112","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1112.3112","created_at":"2026-05-18T01:59:10Z"},{"alias_kind":"arxiv_version","alias_value":"1112.3112v2","created_at":"2026-05-18T01:59:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.3112","created_at":"2026-05-18T01:59:10Z"},{"alias_kind":"pith_short_12","alias_value":"3774FMI4BW2X","created_at":"2026-05-18T12:26:18Z"},{"alias_kind":"pith_short_16","alias_value":"3774FMI4BW2X64UE","created_at":"2026-05-18T12:26:18Z"},{"alias_kind":"pith_short_8","alias_value":"3774FMI4","created_at":"2026-05-18T12:26:18Z"}],"graph_snapshots":[{"event_id":"sha256:3c11a7e6d64091ec5953eab95744860bc7ddc34f96d91d02efd4183f12ae26c2","target":"graph","created_at":"2026-05-18T01:59:10Z","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":"The latest results of the ATLAS and CMS experiments indicate 116 GeV \\lesssim M_H \\lesssim 131 GeV and 115 GeV \\lesssim M_H \\lesssim 127 GeV, respectively, for the mass of the Higgs boson in the standard model (SM) at the 95% confidence level. In particular, both experiments point to a preferred narrow mass range M_H \\simeq (124 ... 126) GeV. We examine the impact of this preliminary result of M_H on the SM vacuum stability by using the two-loop renormalization-group equations (RGEs), and arrive at the cutoff scale \\Lambda_VS \\sim 4 \\times 10^{12} GeV (for M_H = 125 GeV, M_t = 172.9 GeV and \\a","authors_text":"He Zhang, Shun Zhou, Zhi-zhong Xing","cross_cats":["hep-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-12-14T04:12:15Z","title":"Impacts of the Higgs mass on vacuum stability, running fermion masses and two-body Higgs decays"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.3112","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":"sha256:21145345fc306cce6c46c2caf6554b9208c604a5b050e5319d500143e6972e08","target":"record","created_at":"2026-05-18T01:59:10Z","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":"0574bb6b68d4c7d8dfd7d4fcc9e8c29f768d83528aec84ebe8936f797f9e3c59","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-12-14T04:12:15Z","title_canon_sha256":"c7a6a943041af00dd92fab506b2191ca069b46c19fb59e243f89b9c4adba694d"},"schema_version":"1.0","source":{"id":"1112.3112","kind":"arxiv","version":2}},"canonical_sha256":"dfffc2b11c0db57f7284cbac02c0da481d95ddb4d3a8c534b31832dcec9a6a9b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"dfffc2b11c0db57f7284cbac02c0da481d95ddb4d3a8c534b31832dcec9a6a9b","first_computed_at":"2026-05-18T01:59:10.380115Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:59:10.380115Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"UIiGRBoeO6LLunewxk7+CHEn7PimwmXF+EIoVtmwLUsNPKG4i201+XJzEyZJrhGntQ3NoEQmeGX9/EfPh54mDg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:59:10.380633Z","signed_message":"canonical_sha256_bytes"},"source_id":"1112.3112","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:21145345fc306cce6c46c2caf6554b9208c604a5b050e5319d500143e6972e08","sha256:3c11a7e6d64091ec5953eab95744860bc7ddc34f96d91d02efd4183f12ae26c2"],"state_sha256":"01bd0c734a77c4c5846247dcd28693801a7d084896eb14b6eed4dcdddae04fd9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5nQ2nhk9WpYF/M36I5RqaPcYf1MTHPdU8omWFNKAqKmLLaRmOXeUEnrHWqJLxDM9y9v8hrj4MCITJIdAdywDDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-24T03:05:31.112509Z","bundle_sha256":"8078da2062272711fddac8770b4778272c36863c5c28b6b60fe4a0c94e7ef590"}}