{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:24QHOFT57SYY4NUBIKO6F3DBRE","short_pith_number":"pith:24QHOFT5","canonical_record":{"source":{"id":"1310.6260","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-10-23T15:19:04Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"2c5cb8ffba4ae94f5e9c362288b175047555772b0c5e8d4704d453d871b94fe7","abstract_canon_sha256":"57618099baba234ebdd8931c9fa5ecbdbbf4f9ee7526e20d9cd131269d03a9c9"},"schema_version":"1.0"},"canonical_sha256":"d72077167dfcb18e3681429de2ec61891f66142489716ed79fe0bf85e49fc101","source":{"kind":"arxiv","id":"1310.6260","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1310.6260","created_at":"2026-05-18T03:09:20Z"},{"alias_kind":"arxiv_version","alias_value":"1310.6260v1","created_at":"2026-05-18T03:09:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.6260","created_at":"2026-05-18T03:09:20Z"},{"alias_kind":"pith_short_12","alias_value":"24QHOFT57SYY","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_16","alias_value":"24QHOFT57SYY4NUB","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_8","alias_value":"24QHOFT5","created_at":"2026-05-18T12:27:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:24QHOFT57SYY4NUBIKO6F3DBRE","target":"record","payload":{"canonical_record":{"source":{"id":"1310.6260","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-10-23T15:19:04Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"2c5cb8ffba4ae94f5e9c362288b175047555772b0c5e8d4704d453d871b94fe7","abstract_canon_sha256":"57618099baba234ebdd8931c9fa5ecbdbbf4f9ee7526e20d9cd131269d03a9c9"},"schema_version":"1.0"},"canonical_sha256":"d72077167dfcb18e3681429de2ec61891f66142489716ed79fe0bf85e49fc101","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:09:20.873449Z","signature_b64":"ZxNi/QZl7mBCTCf3FP0DS1SZ9EoOI2qlfKuWbB1lc/yu8fMAwdVlCFujVDJnRF63ZNqYN+BzqnTAhGiLIGfoAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d72077167dfcb18e3681429de2ec61891f66142489716ed79fe0bf85e49fc101","last_reissued_at":"2026-05-18T03:09:20.872594Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:09:20.872594Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1310.6260","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":"2026-05-18T03:09:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"j5klCGdIj10H/K0yQw+z7dE0Do8aJOSvrnX18EkCpvO9qPbYJe11NRICoYQAr0OWocSgzkYWSuYZ7d3+hB67CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T23:34:08.841067Z"},"content_sha256":"d35ad93bfe0ee0d0221f260ca9797440b37b7dfdaf7d3759a8e2a39900d785d9","schema_version":"1.0","event_id":"sha256:d35ad93bfe0ee0d0221f260ca9797440b37b7dfdaf7d3759a8e2a39900d785d9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:24QHOFT57SYY4NUBIKO6F3DBRE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Stabilizing the electroweak vacuum by higher dimensional operators in a Higgs-Yukawa model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Attila Nagy, C.-J. David Lin, Karl Jansen, Prasad Hegde","submitted_at":"2013-10-23T15:19:04Z","abstract_excerpt":"The Higgs boson discovery at the LHC with a mass of approximately 126 GeV suggests, that the electroweak vacuum of the standard model may be metastable at very high energies. However, any new physics beyond the standard model can change this picture. We want to address this important question within a lattice Higgs-Yukawa model as the limit of the standard model (SM). In this framework we will probe the effect of a higher dimensional operator for which we take a $(\\phi^{\\dagger}\\phi)^3$-term. Such a term could easily originate as a remnant of physics beyond the SM at very large scales.\n  As a "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.6260","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":"2026-05-18T03:09:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"P0+FMSlzIyx6jXRywZIA8S1sTOpJ0yw33pdR/gMU9gvFeqIRet9QXgj+vGaYc4T1LVVCOKyU6SFayaeIyMivDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T23:34:08.841433Z"},"content_sha256":"5017c9972b3341e817ef593e86a91ccc9046c16125812adbe8c631ece83aa8ea","schema_version":"1.0","event_id":"sha256:5017c9972b3341e817ef593e86a91ccc9046c16125812adbe8c631ece83aa8ea"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/24QHOFT57SYY4NUBIKO6F3DBRE/bundle.json","state_url":"https://pith.science/pith/24QHOFT57SYY4NUBIKO6F3DBRE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/24QHOFT57SYY4NUBIKO6F3DBRE/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":"2026-06-01T23:34:08Z","links":{"resolver":"https://pith.science/pith/24QHOFT57SYY4NUBIKO6F3DBRE","bundle":"https://pith.science/pith/24QHOFT57SYY4NUBIKO6F3DBRE/bundle.json","state":"https://pith.science/pith/24QHOFT57SYY4NUBIKO6F3DBRE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/24QHOFT57SYY4NUBIKO6F3DBRE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:24QHOFT57SYY4NUBIKO6F3DBRE","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":"57618099baba234ebdd8931c9fa5ecbdbbf4f9ee7526e20d9cd131269d03a9c9","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-10-23T15:19:04Z","title_canon_sha256":"2c5cb8ffba4ae94f5e9c362288b175047555772b0c5e8d4704d453d871b94fe7"},"schema_version":"1.0","source":{"id":"1310.6260","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1310.6260","created_at":"2026-05-18T03:09:20Z"},{"alias_kind":"arxiv_version","alias_value":"1310.6260v1","created_at":"2026-05-18T03:09:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.6260","created_at":"2026-05-18T03:09:20Z"},{"alias_kind":"pith_short_12","alias_value":"24QHOFT57SYY","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_16","alias_value":"24QHOFT57SYY4NUB","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_8","alias_value":"24QHOFT5","created_at":"2026-05-18T12:27:30Z"}],"graph_snapshots":[{"event_id":"sha256:5017c9972b3341e817ef593e86a91ccc9046c16125812adbe8c631ece83aa8ea","target":"graph","created_at":"2026-05-18T03:09:20Z","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 Higgs boson discovery at the LHC with a mass of approximately 126 GeV suggests, that the electroweak vacuum of the standard model may be metastable at very high energies. However, any new physics beyond the standard model can change this picture. We want to address this important question within a lattice Higgs-Yukawa model as the limit of the standard model (SM). In this framework we will probe the effect of a higher dimensional operator for which we take a $(\\phi^{\\dagger}\\phi)^3$-term. Such a term could easily originate as a remnant of physics beyond the SM at very large scales.\n  As a ","authors_text":"Attila Nagy, C.-J. David Lin, Karl Jansen, Prasad Hegde","cross_cats":["hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-10-23T15:19:04Z","title":"Stabilizing the electroweak vacuum by higher dimensional operators in a Higgs-Yukawa model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.6260","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:d35ad93bfe0ee0d0221f260ca9797440b37b7dfdaf7d3759a8e2a39900d785d9","target":"record","created_at":"2026-05-18T03:09:20Z","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":"57618099baba234ebdd8931c9fa5ecbdbbf4f9ee7526e20d9cd131269d03a9c9","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-10-23T15:19:04Z","title_canon_sha256":"2c5cb8ffba4ae94f5e9c362288b175047555772b0c5e8d4704d453d871b94fe7"},"schema_version":"1.0","source":{"id":"1310.6260","kind":"arxiv","version":1}},"canonical_sha256":"d72077167dfcb18e3681429de2ec61891f66142489716ed79fe0bf85e49fc101","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d72077167dfcb18e3681429de2ec61891f66142489716ed79fe0bf85e49fc101","first_computed_at":"2026-05-18T03:09:20.872594Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:09:20.872594Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ZxNi/QZl7mBCTCf3FP0DS1SZ9EoOI2qlfKuWbB1lc/yu8fMAwdVlCFujVDJnRF63ZNqYN+BzqnTAhGiLIGfoAA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:09:20.873449Z","signed_message":"canonical_sha256_bytes"},"source_id":"1310.6260","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d35ad93bfe0ee0d0221f260ca9797440b37b7dfdaf7d3759a8e2a39900d785d9","sha256:5017c9972b3341e817ef593e86a91ccc9046c16125812adbe8c631ece83aa8ea"],"state_sha256":"3508abc877d3954085fc8385e891abe412aa980920214745ce5284d317964563"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"o5ELYkcOUdGw1o4Ly+vRym+kGTlicWLmD+giizj8/1vupx8DdG1znKeb72vSz0nxNiePPabjPdDjLBJrn/QOCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T23:34:08.843271Z","bundle_sha256":"06dbb525556cbc551471161417e5e250a009523397168ce3e7a3ce36b33c7be6"}}