{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2003:7HEHXBPTDXY4H5QA4WZGDAXSRW","short_pith_number":"pith:7HEHXBPT","canonical_record":{"source":{"id":"hep-ph/0304109","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2003-04-11T09:44:06Z","cross_cats_sorted":[],"title_canon_sha256":"b9bfa61d0958eba28dbe2ac91651a6bae7c954cd23ba2e9cca66cccb9ddf2209","abstract_canon_sha256":"adf2e9f6d58fb6a5e85ee9824786d117f4c3dbb6c5c744ffe9fec1a5b0d13fa0"},"schema_version":"1.0"},"canonical_sha256":"f9c87b85f31df1c3f600e5b26182f28d8a1749d4d47392d0898e24cdcc07c5a7","source":{"kind":"arxiv","id":"hep-ph/0304109","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0304109","created_at":"2026-05-18T00:36:56Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0304109v1","created_at":"2026-05-18T00:36:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0304109","created_at":"2026-05-18T00:36:56Z"},{"alias_kind":"pith_short_12","alias_value":"7HEHXBPTDXY4","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_16","alias_value":"7HEHXBPTDXY4H5QA","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_8","alias_value":"7HEHXBPT","created_at":"2026-05-18T12:25:51Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2003:7HEHXBPTDXY4H5QA4WZGDAXSRW","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0304109","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2003-04-11T09:44:06Z","cross_cats_sorted":[],"title_canon_sha256":"b9bfa61d0958eba28dbe2ac91651a6bae7c954cd23ba2e9cca66cccb9ddf2209","abstract_canon_sha256":"adf2e9f6d58fb6a5e85ee9824786d117f4c3dbb6c5c744ffe9fec1a5b0d13fa0"},"schema_version":"1.0"},"canonical_sha256":"f9c87b85f31df1c3f600e5b26182f28d8a1749d4d47392d0898e24cdcc07c5a7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:36:56.512474Z","signature_b64":"HRKZ/Lcz5u3+RKrZwmD3JgFvuxyeTor5KM9PBG70Hm02tDv8mfdLUvwaiLoy7ZPTjIBXxFas8owP3Dc4WIzCAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f9c87b85f31df1c3f600e5b26182f28d8a1749d4d47392d0898e24cdcc07c5a7","last_reissued_at":"2026-05-18T00:36:56.512026Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:36:56.512026Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0304109","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":"2026-05-18T00:36:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4UYcT5cQv2AiQX/JYVoU32WNJrQLEM37p6zcKsVONJbGoPBtghSXJKILNozsR2p1mzcgGDVASfgrMDzgMc7BCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T11:17:14.388771Z"},"content_sha256":"b63936018729fc76f439e390eb89344c56c43f712eaef49430c2d528f15e9d2c","schema_version":"1.0","event_id":"sha256:b63936018729fc76f439e390eb89344c56c43f712eaef49430c2d528f15e9d2c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2003:7HEHXBPTDXY4H5QA4WZGDAXSRW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dynamical Electroweak Symmetry Breaking from Extra Dimensions","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Koichi Yamawaki, Masaharu Tanabashi, Michio Hashimoto","submitted_at":"2003-04-11T09:44:06Z","abstract_excerpt":"We study the dynamical electroweak symmetry breaking (DEWSB) in the $D (=6,8,...)$-dimensional bulk with compactified extra dimensions. We identify the critical binding strength for triggering the DEWSB, based on the ladder Schwinger-Dyson equation. In the top mode standard model with extra dimensions, where the standard model gauge bosons and the third generation of quarks and leptons are put in the bulk, we analyze the most attractive channel (MAC) by using renormalization group equations (RGEs) of (dimensionless) bulk gauge couplings and determine the effective cutoff where the MAC coupling"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0304109","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":"2026-05-18T00:36:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"K8qhRmixAVZY7lqTPywOXmhLKMcbaI3td/vZRUNL5UCjED7SxupcZHnE87TYRmkrLJyMs7KG3alqcAg5Z2nPCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T11:17:14.389127Z"},"content_sha256":"70a607ee0cd9ee1fb23f76405adb47f2bba6f99d6c29eda1af1c1b6c0fc464ef","schema_version":"1.0","event_id":"sha256:70a607ee0cd9ee1fb23f76405adb47f2bba6f99d6c29eda1af1c1b6c0fc464ef"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/7HEHXBPTDXY4H5QA4WZGDAXSRW/bundle.json","state_url":"https://pith.science/pith/7HEHXBPTDXY4H5QA4WZGDAXSRW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/7HEHXBPTDXY4H5QA4WZGDAXSRW/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":"2026-05-30T11:17:14Z","links":{"resolver":"https://pith.science/pith/7HEHXBPTDXY4H5QA4WZGDAXSRW","bundle":"https://pith.science/pith/7HEHXBPTDXY4H5QA4WZGDAXSRW/bundle.json","state":"https://pith.science/pith/7HEHXBPTDXY4H5QA4WZGDAXSRW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/7HEHXBPTDXY4H5QA4WZGDAXSRW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2003:7HEHXBPTDXY4H5QA4WZGDAXSRW","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":"adf2e9f6d58fb6a5e85ee9824786d117f4c3dbb6c5c744ffe9fec1a5b0d13fa0","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2003-04-11T09:44:06Z","title_canon_sha256":"b9bfa61d0958eba28dbe2ac91651a6bae7c954cd23ba2e9cca66cccb9ddf2209"},"schema_version":"1.0","source":{"id":"hep-ph/0304109","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0304109","created_at":"2026-05-18T00:36:56Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0304109v1","created_at":"2026-05-18T00:36:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0304109","created_at":"2026-05-18T00:36:56Z"},{"alias_kind":"pith_short_12","alias_value":"7HEHXBPTDXY4","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_16","alias_value":"7HEHXBPTDXY4H5QA","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_8","alias_value":"7HEHXBPT","created_at":"2026-05-18T12:25:51Z"}],"graph_snapshots":[{"event_id":"sha256:70a607ee0cd9ee1fb23f76405adb47f2bba6f99d6c29eda1af1c1b6c0fc464ef","target":"graph","created_at":"2026-05-18T00:36:56Z","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 dynamical electroweak symmetry breaking (DEWSB) in the $D (=6,8,...)$-dimensional bulk with compactified extra dimensions. We identify the critical binding strength for triggering the DEWSB, based on the ladder Schwinger-Dyson equation. In the top mode standard model with extra dimensions, where the standard model gauge bosons and the third generation of quarks and leptons are put in the bulk, we analyze the most attractive channel (MAC) by using renormalization group equations (RGEs) of (dimensionless) bulk gauge couplings and determine the effective cutoff where the MAC coupling","authors_text":"Koichi Yamawaki, Masaharu Tanabashi, Michio Hashimoto","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2003-04-11T09:44:06Z","title":"Dynamical Electroweak Symmetry Breaking from Extra Dimensions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0304109","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:b63936018729fc76f439e390eb89344c56c43f712eaef49430c2d528f15e9d2c","target":"record","created_at":"2026-05-18T00:36:56Z","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":"adf2e9f6d58fb6a5e85ee9824786d117f4c3dbb6c5c744ffe9fec1a5b0d13fa0","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2003-04-11T09:44:06Z","title_canon_sha256":"b9bfa61d0958eba28dbe2ac91651a6bae7c954cd23ba2e9cca66cccb9ddf2209"},"schema_version":"1.0","source":{"id":"hep-ph/0304109","kind":"arxiv","version":1}},"canonical_sha256":"f9c87b85f31df1c3f600e5b26182f28d8a1749d4d47392d0898e24cdcc07c5a7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f9c87b85f31df1c3f600e5b26182f28d8a1749d4d47392d0898e24cdcc07c5a7","first_computed_at":"2026-05-18T00:36:56.512026Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:36:56.512026Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"HRKZ/Lcz5u3+RKrZwmD3JgFvuxyeTor5KM9PBG70Hm02tDv8mfdLUvwaiLoy7ZPTjIBXxFas8owP3Dc4WIzCAg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:36:56.512474Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0304109","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b63936018729fc76f439e390eb89344c56c43f712eaef49430c2d528f15e9d2c","sha256:70a607ee0cd9ee1fb23f76405adb47f2bba6f99d6c29eda1af1c1b6c0fc464ef"],"state_sha256":"10fc1062dc000a2e568e4f2b32c4543461676b0417698e3275ea8d14af75fa6d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"O431DRbRVC9L8x5p6FoFZP6Ex5UM5i04pfOazpKx6GE1XPylkNc0wcSeXwsKwgGgdNZ9MQVrMv/+4Yby9ewWBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T11:17:14.391266Z","bundle_sha256":"2e4adcad88199a3da243577e40d10a219f7ee067b7a35bf570fb321f4d9d9733"}}