{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:AOLALX6I6Q6WIMAQOQNITXQ6EW","short_pith_number":"pith:AOLALX6I","canonical_record":{"source":{"id":"1301.5167","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-01-22T12:25:38Z","cross_cats_sorted":[],"title_canon_sha256":"c0d2535b936f16484ef6f28d53b845c8281ec9eb2f112c40554af7e0570c141a","abstract_canon_sha256":"427d148d7fff95bb683649aaa99a349ab8433ab9d51bcfa8b37cb9310c8fe519"},"schema_version":"1.0"},"canonical_sha256":"039605dfc8f43d643010741a89de1e25beae8ef590dd3099bbfd3daa1706adde","source":{"kind":"arxiv","id":"1301.5167","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1301.5167","created_at":"2026-05-18T01:52:04Z"},{"alias_kind":"arxiv_version","alias_value":"1301.5167v3","created_at":"2026-05-18T01:52:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1301.5167","created_at":"2026-05-18T01:52:04Z"},{"alias_kind":"pith_short_12","alias_value":"AOLALX6I6Q6W","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_16","alias_value":"AOLALX6I6Q6WIMAQ","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_8","alias_value":"AOLALX6I","created_at":"2026-05-18T12:27:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:AOLALX6I6Q6WIMAQOQNITXQ6EW","target":"record","payload":{"canonical_record":{"source":{"id":"1301.5167","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-01-22T12:25:38Z","cross_cats_sorted":[],"title_canon_sha256":"c0d2535b936f16484ef6f28d53b845c8281ec9eb2f112c40554af7e0570c141a","abstract_canon_sha256":"427d148d7fff95bb683649aaa99a349ab8433ab9d51bcfa8b37cb9310c8fe519"},"schema_version":"1.0"},"canonical_sha256":"039605dfc8f43d643010741a89de1e25beae8ef590dd3099bbfd3daa1706adde","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:52:04.731870Z","signature_b64":"klcc6AHMYOWUvSw2xRH2aQUNxtTY6d9gnzb53nhOK6A9nQVhZzA5D2FZ7pHgis1BO8HOXv5v5Xs65k2mjw/2Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"039605dfc8f43d643010741a89de1e25beae8ef590dd3099bbfd3daa1706adde","last_reissued_at":"2026-05-18T01:52:04.731475Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:52:04.731475Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1301.5167","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:52:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ozFvqHjoo/+AdnTvMA60913THSI8V+pFked5D4itidtN3vTqpbuTjF3EZDf54kEvMQOFh1FeBIbrlM+eBKU3DA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T18:29:14.958819Z"},"content_sha256":"ebffe8996ea87aeb46ae738559db87f2d4d8863ef33f6601ae2c12d787e7faed","schema_version":"1.0","event_id":"sha256:ebffe8996ea87aeb46ae738559db87f2d4d8863ef33f6601ae2c12d787e7faed"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:AOLALX6I6Q6WIMAQOQNITXQ6EW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The Higgs Mass as a Signature of Heavy SUSY","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Irene Valenzuela, Luis E. Ibanez","submitted_at":"2013-01-22T12:25:38Z","abstract_excerpt":"We compute the mass of the Higgs particle in a scheme in which SUSY is broken at a large scale M_{SS} well above the electroweak scale M_{EW}. Below M_{SS} one assumes one is just left with the SM with a fine-tuned Higgs potential. Under standard unification assumptions one can compute the mass of the Higgs particle as a function of the SUSY breaking scale M_{SS}. For M_{SS} > 10^{10} GeV one obtains m_H=126 \\pm 3 GeV, consistent with CMS and ATLAS results. For lower values of M_{SS} the values of the Higgs mass tend to those of a fine-tuned MSSM with m_H < 130 GeV. These results support the i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1301.5167","kind":"arxiv","version":3},"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":"2026-05-18T01:52:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dyLd65QxRCIZatfAwLC9IryV6cm3y0+ktykagB9Lw9VGPfvslyAz2KZUsY0czaWKuUxWlTzW4fcXmYNQlOBbBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T18:29:14.959167Z"},"content_sha256":"385f9a80224f4505bb39e327d0a0efb29ae3d1fb49ca6994834decebe7b739b1","schema_version":"1.0","event_id":"sha256:385f9a80224f4505bb39e327d0a0efb29ae3d1fb49ca6994834decebe7b739b1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/AOLALX6I6Q6WIMAQOQNITXQ6EW/bundle.json","state_url":"https://pith.science/pith/AOLALX6I6Q6WIMAQOQNITXQ6EW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/AOLALX6I6Q6WIMAQOQNITXQ6EW/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":"2026-06-03T18:29:14Z","links":{"resolver":"https://pith.science/pith/AOLALX6I6Q6WIMAQOQNITXQ6EW","bundle":"https://pith.science/pith/AOLALX6I6Q6WIMAQOQNITXQ6EW/bundle.json","state":"https://pith.science/pith/AOLALX6I6Q6WIMAQOQNITXQ6EW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/AOLALX6I6Q6WIMAQOQNITXQ6EW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:AOLALX6I6Q6WIMAQOQNITXQ6EW","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":"427d148d7fff95bb683649aaa99a349ab8433ab9d51bcfa8b37cb9310c8fe519","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-01-22T12:25:38Z","title_canon_sha256":"c0d2535b936f16484ef6f28d53b845c8281ec9eb2f112c40554af7e0570c141a"},"schema_version":"1.0","source":{"id":"1301.5167","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1301.5167","created_at":"2026-05-18T01:52:04Z"},{"alias_kind":"arxiv_version","alias_value":"1301.5167v3","created_at":"2026-05-18T01:52:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1301.5167","created_at":"2026-05-18T01:52:04Z"},{"alias_kind":"pith_short_12","alias_value":"AOLALX6I6Q6W","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_16","alias_value":"AOLALX6I6Q6WIMAQ","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_8","alias_value":"AOLALX6I","created_at":"2026-05-18T12:27:38Z"}],"graph_snapshots":[{"event_id":"sha256:385f9a80224f4505bb39e327d0a0efb29ae3d1fb49ca6994834decebe7b739b1","target":"graph","created_at":"2026-05-18T01:52:04Z","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":"We compute the mass of the Higgs particle in a scheme in which SUSY is broken at a large scale M_{SS} well above the electroweak scale M_{EW}. Below M_{SS} one assumes one is just left with the SM with a fine-tuned Higgs potential. Under standard unification assumptions one can compute the mass of the Higgs particle as a function of the SUSY breaking scale M_{SS}. For M_{SS} > 10^{10} GeV one obtains m_H=126 \\pm 3 GeV, consistent with CMS and ATLAS results. For lower values of M_{SS} the values of the Higgs mass tend to those of a fine-tuned MSSM with m_H < 130 GeV. These results support the i","authors_text":"Irene Valenzuela, Luis E. Ibanez","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-01-22T12:25:38Z","title":"The Higgs Mass as a Signature of Heavy SUSY"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1301.5167","kind":"arxiv","version":3},"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:ebffe8996ea87aeb46ae738559db87f2d4d8863ef33f6601ae2c12d787e7faed","target":"record","created_at":"2026-05-18T01:52:04Z","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":"427d148d7fff95bb683649aaa99a349ab8433ab9d51bcfa8b37cb9310c8fe519","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-01-22T12:25:38Z","title_canon_sha256":"c0d2535b936f16484ef6f28d53b845c8281ec9eb2f112c40554af7e0570c141a"},"schema_version":"1.0","source":{"id":"1301.5167","kind":"arxiv","version":3}},"canonical_sha256":"039605dfc8f43d643010741a89de1e25beae8ef590dd3099bbfd3daa1706adde","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"039605dfc8f43d643010741a89de1e25beae8ef590dd3099bbfd3daa1706adde","first_computed_at":"2026-05-18T01:52:04.731475Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:52:04.731475Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"klcc6AHMYOWUvSw2xRH2aQUNxtTY6d9gnzb53nhOK6A9nQVhZzA5D2FZ7pHgis1BO8HOXv5v5Xs65k2mjw/2Ag==","signature_status":"signed_v1","signed_at":"2026-05-18T01:52:04.731870Z","signed_message":"canonical_sha256_bytes"},"source_id":"1301.5167","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ebffe8996ea87aeb46ae738559db87f2d4d8863ef33f6601ae2c12d787e7faed","sha256:385f9a80224f4505bb39e327d0a0efb29ae3d1fb49ca6994834decebe7b739b1"],"state_sha256":"7924557c103af82c6dce221821aa934e7871b15e0b73185ec079b12983187c1c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gS/ddpxDQiNz2L4tqzUOl6h8iKeuZhDbPD00jzLFz/b1bmULT1xC4stF9BqecUhqCJv1bBaw1qZ7uFbiLUSqBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T18:29:14.961395Z","bundle_sha256":"7f24cfb658f504c54bf4c2eccadd426f774f417d0be1f3714255d7dc4f30e543"}}