{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:RAGT4TL6CJ4J2Q3XCU5F4M4KEV","short_pith_number":"pith:RAGT4TL6","canonical_record":{"source":{"id":"1004.2953","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-04-17T11:17:51Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"e4b91a7e53eaa18879b9254da8249d8600ab3c9952d03e3f7138f50937e44b7a","abstract_canon_sha256":"adeac0b494dae65a232e4295bc3abc8e1cc63a63ad0aa5c488f06bc52d50eb7b"},"schema_version":"1.0"},"canonical_sha256":"880d3e4d7e12789d4377153a5e338a25568a205e985bdb76f0c4c6b875e87a0c","source":{"kind":"arxiv","id":"1004.2953","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1004.2953","created_at":"2026-05-18T04:31:22Z"},{"alias_kind":"arxiv_version","alias_value":"1004.2953v1","created_at":"2026-05-18T04:31:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1004.2953","created_at":"2026-05-18T04:31:22Z"},{"alias_kind":"pith_short_12","alias_value":"RAGT4TL6CJ4J","created_at":"2026-05-18T12:26:13Z"},{"alias_kind":"pith_short_16","alias_value":"RAGT4TL6CJ4J2Q3X","created_at":"2026-05-18T12:26:13Z"},{"alias_kind":"pith_short_8","alias_value":"RAGT4TL6","created_at":"2026-05-18T12:26:13Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:RAGT4TL6CJ4J2Q3XCU5F4M4KEV","target":"record","payload":{"canonical_record":{"source":{"id":"1004.2953","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-04-17T11:17:51Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"e4b91a7e53eaa18879b9254da8249d8600ab3c9952d03e3f7138f50937e44b7a","abstract_canon_sha256":"adeac0b494dae65a232e4295bc3abc8e1cc63a63ad0aa5c488f06bc52d50eb7b"},"schema_version":"1.0"},"canonical_sha256":"880d3e4d7e12789d4377153a5e338a25568a205e985bdb76f0c4c6b875e87a0c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:31:22.537344Z","signature_b64":"EDKfLL7DIp8fZuX40O8HCGD2FrwmQJYhXpRsQFBpTNH6mlJdrO1ukT1FlL5FOkbom6uhuqYdIXZtwuBstVPAAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"880d3e4d7e12789d4377153a5e338a25568a205e985bdb76f0c4c6b875e87a0c","last_reissued_at":"2026-05-18T04:31:22.536823Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:31:22.536823Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1004.2953","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":"2026-05-18T04:31:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pmn/ab7h15UP1IDPG58zNPeHGTi5VZTZd5CNhHbhd0Bh3hF7m83m04aEVHk4zjXxMh+BMyH5zvXKrwAke985Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-02T15:59:12.246479Z"},"content_sha256":"6a88418ecec30c023f54a6b5d700b23cccf4194d301e86f9091f63828abd2ae0","schema_version":"1.0","event_id":"sha256:6a88418ecec30c023f54a6b5d700b23cccf4194d301e86f9091f63828abd2ae0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:RAGT4TL6CJ4J2Q3XCU5F4M4KEV","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"An Unusual Two Higgs Doublet Model from Warped Space","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"A.P. Spray (TRIUMF), John N. Ng, We-Fu Chang (National Tsing Hua University)","submitted_at":"2010-04-17T11:17:51Z","abstract_excerpt":"We study a simple two Higgs doublet model (2HDM) in the Randall-Sundrum scenario, with an IR brane localized Higgs field and a second doublet arising from a $t\\bar{t}$ condensate due to strong Kaluza-Klein gluon effects.\n The effective 2HDM predicts that the ratio of the brane to condensate vacuum expectation values $\\tan \\beta \\sim 3$. It also predicts a standard model like Higgs boson of mass ${\\mathcal{O}}(100)$ GeV and a heavier scalar at the scale of the lowest KK gluon mass, which we take to be $M_{KK} \\gtrsim 1.5$ TeV.  The pseudoscalar and the charged scalars are degenerate in mass at "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1004.2953","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":"2026-05-18T04:31:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"EuD61i11zak4CE5CiOu2liQzO88vWomxIOleWbX/JtKxG4iIgCwEsJGuJXxBm1yxllNggEccyE60BlywRD0oCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-02T15:59:12.246838Z"},"content_sha256":"4ba3d18d35355850d182327b1b91ee94d2922c646fb7cef56f383bd9e3515264","schema_version":"1.0","event_id":"sha256:4ba3d18d35355850d182327b1b91ee94d2922c646fb7cef56f383bd9e3515264"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RAGT4TL6CJ4J2Q3XCU5F4M4KEV/bundle.json","state_url":"https://pith.science/pith/RAGT4TL6CJ4J2Q3XCU5F4M4KEV/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RAGT4TL6CJ4J2Q3XCU5F4M4KEV/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":"2026-07-02T15:59:12Z","links":{"resolver":"https://pith.science/pith/RAGT4TL6CJ4J2Q3XCU5F4M4KEV","bundle":"https://pith.science/pith/RAGT4TL6CJ4J2Q3XCU5F4M4KEV/bundle.json","state":"https://pith.science/pith/RAGT4TL6CJ4J2Q3XCU5F4M4KEV/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RAGT4TL6CJ4J2Q3XCU5F4M4KEV/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:RAGT4TL6CJ4J2Q3XCU5F4M4KEV","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":"adeac0b494dae65a232e4295bc3abc8e1cc63a63ad0aa5c488f06bc52d50eb7b","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-04-17T11:17:51Z","title_canon_sha256":"e4b91a7e53eaa18879b9254da8249d8600ab3c9952d03e3f7138f50937e44b7a"},"schema_version":"1.0","source":{"id":"1004.2953","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1004.2953","created_at":"2026-05-18T04:31:22Z"},{"alias_kind":"arxiv_version","alias_value":"1004.2953v1","created_at":"2026-05-18T04:31:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1004.2953","created_at":"2026-05-18T04:31:22Z"},{"alias_kind":"pith_short_12","alias_value":"RAGT4TL6CJ4J","created_at":"2026-05-18T12:26:13Z"},{"alias_kind":"pith_short_16","alias_value":"RAGT4TL6CJ4J2Q3X","created_at":"2026-05-18T12:26:13Z"},{"alias_kind":"pith_short_8","alias_value":"RAGT4TL6","created_at":"2026-05-18T12:26:13Z"}],"graph_snapshots":[{"event_id":"sha256:4ba3d18d35355850d182327b1b91ee94d2922c646fb7cef56f383bd9e3515264","target":"graph","created_at":"2026-05-18T04:31:22Z","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 a simple two Higgs doublet model (2HDM) in the Randall-Sundrum scenario, with an IR brane localized Higgs field and a second doublet arising from a $t\\bar{t}$ condensate due to strong Kaluza-Klein gluon effects.\n The effective 2HDM predicts that the ratio of the brane to condensate vacuum expectation values $\\tan \\beta \\sim 3$. It also predicts a standard model like Higgs boson of mass ${\\mathcal{O}}(100)$ GeV and a heavier scalar at the scale of the lowest KK gluon mass, which we take to be $M_{KK} \\gtrsim 1.5$ TeV.  The pseudoscalar and the charged scalars are degenerate in mass at ","authors_text":"A.P. Spray (TRIUMF), John N. Ng, We-Fu Chang (National Tsing Hua University)","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-04-17T11:17:51Z","title":"An Unusual Two Higgs Doublet Model from Warped Space"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1004.2953","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":"sha256:6a88418ecec30c023f54a6b5d700b23cccf4194d301e86f9091f63828abd2ae0","target":"record","created_at":"2026-05-18T04:31:22Z","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":"adeac0b494dae65a232e4295bc3abc8e1cc63a63ad0aa5c488f06bc52d50eb7b","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-04-17T11:17:51Z","title_canon_sha256":"e4b91a7e53eaa18879b9254da8249d8600ab3c9952d03e3f7138f50937e44b7a"},"schema_version":"1.0","source":{"id":"1004.2953","kind":"arxiv","version":1}},"canonical_sha256":"880d3e4d7e12789d4377153a5e338a25568a205e985bdb76f0c4c6b875e87a0c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"880d3e4d7e12789d4377153a5e338a25568a205e985bdb76f0c4c6b875e87a0c","first_computed_at":"2026-05-18T04:31:22.536823Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:31:22.536823Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"EDKfLL7DIp8fZuX40O8HCGD2FrwmQJYhXpRsQFBpTNH6mlJdrO1ukT1FlL5FOkbom6uhuqYdIXZtwuBstVPAAA==","signature_status":"signed_v1","signed_at":"2026-05-18T04:31:22.537344Z","signed_message":"canonical_sha256_bytes"},"source_id":"1004.2953","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6a88418ecec30c023f54a6b5d700b23cccf4194d301e86f9091f63828abd2ae0","sha256:4ba3d18d35355850d182327b1b91ee94d2922c646fb7cef56f383bd9e3515264"],"state_sha256":"8b117b14e2be2dfe4a40f91623af0d116b5cc64c4f4a734d74b933380d96be21"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fVvmzj4fyxevybFHFCQSHYuCOlCKoavYPl6gmwt+y34UsGA9ITtPpjQ08nU7uEGLDBCUHcMQlF+i3x+v/mfwCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-02T15:59:12.248805Z","bundle_sha256":"6c90b581041edd70c7ba3d6f971a342a1c60922d8c4c44a2943c6242f621443c"}}