{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:N5ALIJDQGZ75ILMP6NQRH5PXVB","short_pith_number":"pith:N5ALIJDQ","canonical_record":{"source":{"id":"1206.6140","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-06-26T23:25:30Z","cross_cats_sorted":[],"title_canon_sha256":"06cf5cc843eca81c32089e44d0c68aab86bf49e7d90722740b29c9143db63f3f","abstract_canon_sha256":"caeeafb6ccd83ff1768c26d8617d006a62f3bfb886bf36a3f679f7f372e44ebb"},"schema_version":"1.0"},"canonical_sha256":"6f40b42470367fd42d8ff36113f5f7a8751ea055b8d3931a6dc3e6ca600ece62","source":{"kind":"arxiv","id":"1206.6140","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1206.6140","created_at":"2026-05-18T03:39:16Z"},{"alias_kind":"arxiv_version","alias_value":"1206.6140v3","created_at":"2026-05-18T03:39:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1206.6140","created_at":"2026-05-18T03:39:16Z"},{"alias_kind":"pith_short_12","alias_value":"N5ALIJDQGZ75","created_at":"2026-05-18T12:27:16Z"},{"alias_kind":"pith_short_16","alias_value":"N5ALIJDQGZ75ILMP","created_at":"2026-05-18T12:27:16Z"},{"alias_kind":"pith_short_8","alias_value":"N5ALIJDQ","created_at":"2026-05-18T12:27:16Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:N5ALIJDQGZ75ILMP6NQRH5PXVB","target":"record","payload":{"canonical_record":{"source":{"id":"1206.6140","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-06-26T23:25:30Z","cross_cats_sorted":[],"title_canon_sha256":"06cf5cc843eca81c32089e44d0c68aab86bf49e7d90722740b29c9143db63f3f","abstract_canon_sha256":"caeeafb6ccd83ff1768c26d8617d006a62f3bfb886bf36a3f679f7f372e44ebb"},"schema_version":"1.0"},"canonical_sha256":"6f40b42470367fd42d8ff36113f5f7a8751ea055b8d3931a6dc3e6ca600ece62","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:39:16.377249Z","signature_b64":"ogkkc9KyNLC22r5jAcS2nqeLUOA4aMlubxUdpkyfWC7vhinWLO2uTeQ5VX4FId3qEd5DjtIsAL1HUnXsu3ctAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6f40b42470367fd42d8ff36113f5f7a8751ea055b8d3931a6dc3e6ca600ece62","last_reissued_at":"2026-05-18T03:39:16.376667Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:39:16.376667Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1206.6140","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":"2026-05-18T03:39:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3ZDjfbqqII1bZep4HCxJPjNEg6WXyeebBgkaC2HXJST5/cAnVDGdVqkBWy70Xk/4zGDKmH6wEq28eERw7GF0AQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T05:36:00.278850Z"},"content_sha256":"11a1e7dbcbaf41c8dedaafd90d2cb03eb67e1602dd3fe101cdffc4d43d2d8022","schema_version":"1.0","event_id":"sha256:11a1e7dbcbaf41c8dedaafd90d2cb03eb67e1602dd3fe101cdffc4d43d2d8022"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:N5ALIJDQGZ75ILMP6NQRH5PXVB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Large, negative threshold contributions to light soft masses in models with Effective Supersymmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"C. Tamarit","submitted_at":"2012-06-26T23:25:30Z","abstract_excerpt":"Threshold contributions to light scalar soft masses due to heavy sparticles (possibly including a heavy Higgs mostly aligned with H_d) in Effective SUSY scenarios are dominated by two-loop diagrams involving gauge couplings. This is due to the fact that in the limit in which the heavy states are degenerate, their one-loop contributions to the light soft masses only depend on small Yukawas and the hypercharge coupling. The two-loop threshold corrections involving only gauge couplings are calculated accounting for nonzero gaugino and light squark masses and shown to be negative, and rather large"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1206.6140","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":"2026-05-18T03:39:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"C+1LAgsvq8la5hSfheILiCCsFHJEGCPrpRVA6giI7KZY9saW6MMMBWm0k0ajV0f866hhRpjlk3GLe5r8YyFBAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T05:36:00.279203Z"},"content_sha256":"5130792a889c14e8a310f779146f80b7148468ce9385cf653044b5e10f8b60cd","schema_version":"1.0","event_id":"sha256:5130792a889c14e8a310f779146f80b7148468ce9385cf653044b5e10f8b60cd"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/N5ALIJDQGZ75ILMP6NQRH5PXVB/bundle.json","state_url":"https://pith.science/pith/N5ALIJDQGZ75ILMP6NQRH5PXVB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/N5ALIJDQGZ75ILMP6NQRH5PXVB/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":"2026-06-09T05:36:00Z","links":{"resolver":"https://pith.science/pith/N5ALIJDQGZ75ILMP6NQRH5PXVB","bundle":"https://pith.science/pith/N5ALIJDQGZ75ILMP6NQRH5PXVB/bundle.json","state":"https://pith.science/pith/N5ALIJDQGZ75ILMP6NQRH5PXVB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/N5ALIJDQGZ75ILMP6NQRH5PXVB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:N5ALIJDQGZ75ILMP6NQRH5PXVB","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":"caeeafb6ccd83ff1768c26d8617d006a62f3bfb886bf36a3f679f7f372e44ebb","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-06-26T23:25:30Z","title_canon_sha256":"06cf5cc843eca81c32089e44d0c68aab86bf49e7d90722740b29c9143db63f3f"},"schema_version":"1.0","source":{"id":"1206.6140","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1206.6140","created_at":"2026-05-18T03:39:16Z"},{"alias_kind":"arxiv_version","alias_value":"1206.6140v3","created_at":"2026-05-18T03:39:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1206.6140","created_at":"2026-05-18T03:39:16Z"},{"alias_kind":"pith_short_12","alias_value":"N5ALIJDQGZ75","created_at":"2026-05-18T12:27:16Z"},{"alias_kind":"pith_short_16","alias_value":"N5ALIJDQGZ75ILMP","created_at":"2026-05-18T12:27:16Z"},{"alias_kind":"pith_short_8","alias_value":"N5ALIJDQ","created_at":"2026-05-18T12:27:16Z"}],"graph_snapshots":[{"event_id":"sha256:5130792a889c14e8a310f779146f80b7148468ce9385cf653044b5e10f8b60cd","target":"graph","created_at":"2026-05-18T03:39:16Z","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":"Threshold contributions to light scalar soft masses due to heavy sparticles (possibly including a heavy Higgs mostly aligned with H_d) in Effective SUSY scenarios are dominated by two-loop diagrams involving gauge couplings. This is due to the fact that in the limit in which the heavy states are degenerate, their one-loop contributions to the light soft masses only depend on small Yukawas and the hypercharge coupling. The two-loop threshold corrections involving only gauge couplings are calculated accounting for nonzero gaugino and light squark masses and shown to be negative, and rather large","authors_text":"C. Tamarit","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-06-26T23:25:30Z","title":"Large, negative threshold contributions to light soft masses in models with Effective Supersymmetry"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1206.6140","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":"sha256:11a1e7dbcbaf41c8dedaafd90d2cb03eb67e1602dd3fe101cdffc4d43d2d8022","target":"record","created_at":"2026-05-18T03:39:16Z","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":"caeeafb6ccd83ff1768c26d8617d006a62f3bfb886bf36a3f679f7f372e44ebb","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-06-26T23:25:30Z","title_canon_sha256":"06cf5cc843eca81c32089e44d0c68aab86bf49e7d90722740b29c9143db63f3f"},"schema_version":"1.0","source":{"id":"1206.6140","kind":"arxiv","version":3}},"canonical_sha256":"6f40b42470367fd42d8ff36113f5f7a8751ea055b8d3931a6dc3e6ca600ece62","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6f40b42470367fd42d8ff36113f5f7a8751ea055b8d3931a6dc3e6ca600ece62","first_computed_at":"2026-05-18T03:39:16.376667Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:39:16.376667Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ogkkc9KyNLC22r5jAcS2nqeLUOA4aMlubxUdpkyfWC7vhinWLO2uTeQ5VX4FId3qEd5DjtIsAL1HUnXsu3ctAA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:39:16.377249Z","signed_message":"canonical_sha256_bytes"},"source_id":"1206.6140","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:11a1e7dbcbaf41c8dedaafd90d2cb03eb67e1602dd3fe101cdffc4d43d2d8022","sha256:5130792a889c14e8a310f779146f80b7148468ce9385cf653044b5e10f8b60cd"],"state_sha256":"b7c144e3fa5b38d858ff83a70f80f8783d20e7cda78359b6ccc1c3054a33f5c4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JkFqaI3OK1gsX6fR5s8wOF+ECkjFm8enzEJReVxRmCXA1gZDaMo2lAA/kwifQ9NWSf1m94BJ2oHZfBuZwZ1dDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-09T05:36:00.281269Z","bundle_sha256":"0d085bc4b6797f2c3eab2911ee19ce4c00829c680b6f9f53561a93f93c5e9a3c"}}