{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:GMYZF7OWA5J3UPIIPNSIOK6DSO","short_pith_number":"pith:GMYZF7OW","canonical_record":{"source":{"id":"1212.5652","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-12-22T03:35:34Z","cross_cats_sorted":[],"title_canon_sha256":"57dddb35f9759dbfcf4f50441edf5e608ce2052dad4d4224371197eacc405339","abstract_canon_sha256":"6b964479134b02c3a3350258e935913e44ba7cd041f344eb01f534aaf746ac79"},"schema_version":"1.0"},"canonical_sha256":"333192fdd60753ba3d087b64872bc393bd8f8f607df1bbfc6937947923e0b300","source":{"kind":"arxiv","id":"1212.5652","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1212.5652","created_at":"2026-05-18T02:54:14Z"},{"alias_kind":"arxiv_version","alias_value":"1212.5652v2","created_at":"2026-05-18T02:54:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1212.5652","created_at":"2026-05-18T02:54:14Z"},{"alias_kind":"pith_short_12","alias_value":"GMYZF7OWA5J3","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_16","alias_value":"GMYZF7OWA5J3UPII","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_8","alias_value":"GMYZF7OW","created_at":"2026-05-18T12:27:06Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:GMYZF7OWA5J3UPIIPNSIOK6DSO","target":"record","payload":{"canonical_record":{"source":{"id":"1212.5652","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-12-22T03:35:34Z","cross_cats_sorted":[],"title_canon_sha256":"57dddb35f9759dbfcf4f50441edf5e608ce2052dad4d4224371197eacc405339","abstract_canon_sha256":"6b964479134b02c3a3350258e935913e44ba7cd041f344eb01f534aaf746ac79"},"schema_version":"1.0"},"canonical_sha256":"333192fdd60753ba3d087b64872bc393bd8f8f607df1bbfc6937947923e0b300","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:54:14.353040Z","signature_b64":"GVEr6gVPUyugjDY2yJTLsZYeceeoxGzKkBLQ8TwLS+/SSkh14It7ddqa+Jm8BI1KTZeAY6MWuRDguAVww2IZCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"333192fdd60753ba3d087b64872bc393bd8f8f607df1bbfc6937947923e0b300","last_reissued_at":"2026-05-18T02:54:14.352490Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:54:14.352490Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1212.5652","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":"2026-05-18T02:54:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/1PNHRCRTwSWodKmm/2XxDpjVB1YOAPMTkhKTSw7pdS+Z8gu364QE7voVv3A+5VCJ1jpPlGaJMx2myxaD8fTCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-23T19:32:36.062051Z"},"content_sha256":"9b210f1f0a8549a4fc94186aaab2a455dad789e0500a6678bde2d27a00170d3c","schema_version":"1.0","event_id":"sha256:9b210f1f0a8549a4fc94186aaab2a455dad789e0500a6678bde2d27a00170d3c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:GMYZF7OWA5J3UPIIPNSIOK6DSO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Stepping Into Electroweak Symmetry Breaking: Phase Transitions and Higgs Phenomenology","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hiren H. Patel, Michael J. Ramsey-Musolf","submitted_at":"2012-12-22T03:35:34Z","abstract_excerpt":"We study the dynamics of electroweak symmetry-breaking in an extension of the Standard Model where the Higgs sector is augmented by the addition of a real (Y = 0) isospin triplet. We show that this scenario exhibits a novel, two-step electroweak phase transition, wherein the first step provides the strongly first order transition as required for electroweak baryogenesis followed by a second step to the Standard Model Higgs phase that also admits a cold dark matter candidate. We analyze the constraints on this scenario from recent results obtained at the Large Hadron Collider for the Higgs diph"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1212.5652","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":"2026-05-18T02:54:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"O3fsoU7QsWlwpcuDe9JfM+5KgYm0QxQ2zZe+dAUu2d43XCjDaTHSXum389gPs8yOeEHr74GG0Kks2VQ9mjp+DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-23T19:32:36.062715Z"},"content_sha256":"7730d4cc6019e3d7692bb396b72504476e1105f10ef70b7ca6d2e68e9ef277dc","schema_version":"1.0","event_id":"sha256:7730d4cc6019e3d7692bb396b72504476e1105f10ef70b7ca6d2e68e9ef277dc"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GMYZF7OWA5J3UPIIPNSIOK6DSO/bundle.json","state_url":"https://pith.science/pith/GMYZF7OWA5J3UPIIPNSIOK6DSO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GMYZF7OWA5J3UPIIPNSIOK6DSO/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":"2026-05-23T19:32:36Z","links":{"resolver":"https://pith.science/pith/GMYZF7OWA5J3UPIIPNSIOK6DSO","bundle":"https://pith.science/pith/GMYZF7OWA5J3UPIIPNSIOK6DSO/bundle.json","state":"https://pith.science/pith/GMYZF7OWA5J3UPIIPNSIOK6DSO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GMYZF7OWA5J3UPIIPNSIOK6DSO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:GMYZF7OWA5J3UPIIPNSIOK6DSO","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":"6b964479134b02c3a3350258e935913e44ba7cd041f344eb01f534aaf746ac79","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-12-22T03:35:34Z","title_canon_sha256":"57dddb35f9759dbfcf4f50441edf5e608ce2052dad4d4224371197eacc405339"},"schema_version":"1.0","source":{"id":"1212.5652","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1212.5652","created_at":"2026-05-18T02:54:14Z"},{"alias_kind":"arxiv_version","alias_value":"1212.5652v2","created_at":"2026-05-18T02:54:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1212.5652","created_at":"2026-05-18T02:54:14Z"},{"alias_kind":"pith_short_12","alias_value":"GMYZF7OWA5J3","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_16","alias_value":"GMYZF7OWA5J3UPII","created_at":"2026-05-18T12:27:06Z"},{"alias_kind":"pith_short_8","alias_value":"GMYZF7OW","created_at":"2026-05-18T12:27:06Z"}],"graph_snapshots":[{"event_id":"sha256:7730d4cc6019e3d7692bb396b72504476e1105f10ef70b7ca6d2e68e9ef277dc","target":"graph","created_at":"2026-05-18T02:54:14Z","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 study the dynamics of electroweak symmetry-breaking in an extension of the Standard Model where the Higgs sector is augmented by the addition of a real (Y = 0) isospin triplet. We show that this scenario exhibits a novel, two-step electroweak phase transition, wherein the first step provides the strongly first order transition as required for electroweak baryogenesis followed by a second step to the Standard Model Higgs phase that also admits a cold dark matter candidate. We analyze the constraints on this scenario from recent results obtained at the Large Hadron Collider for the Higgs diph","authors_text":"Hiren H. Patel, Michael J. Ramsey-Musolf","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-12-22T03:35:34Z","title":"Stepping Into Electroweak Symmetry Breaking: Phase Transitions and Higgs Phenomenology"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1212.5652","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":"sha256:9b210f1f0a8549a4fc94186aaab2a455dad789e0500a6678bde2d27a00170d3c","target":"record","created_at":"2026-05-18T02:54:14Z","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":"6b964479134b02c3a3350258e935913e44ba7cd041f344eb01f534aaf746ac79","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-12-22T03:35:34Z","title_canon_sha256":"57dddb35f9759dbfcf4f50441edf5e608ce2052dad4d4224371197eacc405339"},"schema_version":"1.0","source":{"id":"1212.5652","kind":"arxiv","version":2}},"canonical_sha256":"333192fdd60753ba3d087b64872bc393bd8f8f607df1bbfc6937947923e0b300","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"333192fdd60753ba3d087b64872bc393bd8f8f607df1bbfc6937947923e0b300","first_computed_at":"2026-05-18T02:54:14.352490Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:54:14.352490Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"GVEr6gVPUyugjDY2yJTLsZYeceeoxGzKkBLQ8TwLS+/SSkh14It7ddqa+Jm8BI1KTZeAY6MWuRDguAVww2IZCg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:54:14.353040Z","signed_message":"canonical_sha256_bytes"},"source_id":"1212.5652","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9b210f1f0a8549a4fc94186aaab2a455dad789e0500a6678bde2d27a00170d3c","sha256:7730d4cc6019e3d7692bb396b72504476e1105f10ef70b7ca6d2e68e9ef277dc"],"state_sha256":"e51fc59820be1eed5195687e5b574361b98103a678d6301d53d57772aa5700f9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pF/l3RBY5NyHAE9VlDFDbb4egXtSOKD1e9FOa3TSTbIfTmslXPth4sA1DT7q82SS15NJWVpojpu6XbQp4mXOBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-23T19:32:36.066179Z","bundle_sha256":"7e6efc44c389122573e97aec2464dd4af1f02ea2a0e75738ea9ff4cc8261cbe5"}}