{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2004:P3VGD7MVNWGQMOPHEXDJ5QQNIQ","short_pith_number":"pith:P3VGD7MV","canonical_record":{"source":{"id":"hep-th/0402146","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2004-02-19T11:40:41Z","cross_cats_sorted":[],"title_canon_sha256":"8534ad8dd100716ad3c63d1381d2581ae6911d7901819898282c792af59f707e","abstract_canon_sha256":"cf20c38a15ca2fbdcce0d5e8d6d1cff569ee8f8d9033a6b32f5dd7037bc02f00"},"schema_version":"1.0"},"canonical_sha256":"7eea61fd956d8d0639e725c69ec20d441309315ca8d81ac310f34fef4bd3725a","source":{"kind":"arxiv","id":"hep-th/0402146","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0402146","created_at":"2026-05-18T01:05:58Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0402146v1","created_at":"2026-05-18T01:05:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0402146","created_at":"2026-05-18T01:05:58Z"},{"alias_kind":"pith_short_12","alias_value":"P3VGD7MVNWGQ","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"P3VGD7MVNWGQMOPH","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"P3VGD7MV","created_at":"2026-05-18T12:25:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2004:P3VGD7MVNWGQMOPHEXDJ5QQNIQ","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/0402146","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2004-02-19T11:40:41Z","cross_cats_sorted":[],"title_canon_sha256":"8534ad8dd100716ad3c63d1381d2581ae6911d7901819898282c792af59f707e","abstract_canon_sha256":"cf20c38a15ca2fbdcce0d5e8d6d1cff569ee8f8d9033a6b32f5dd7037bc02f00"},"schema_version":"1.0"},"canonical_sha256":"7eea61fd956d8d0639e725c69ec20d441309315ca8d81ac310f34fef4bd3725a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:05:58.930586Z","signature_b64":"Kyb+/KH0Ldu9pPP3e3ZFcr/o3izPnVz9DsfxbT1CJMLqYQ2LutS+SeVMrgEiMjqiCFopzAEaPm8HicjUJAwHAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7eea61fd956d8d0639e725c69ec20d441309315ca8d81ac310f34fef4bd3725a","last_reissued_at":"2026-05-18T01:05:58.930110Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:05:58.930110Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/0402146","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":"2026-05-18T01:05:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HIqDkPVwZwOYfw9OyiBsOPBrAaA4CmNjOd6bkVn8pDX65lCs0IqW0V/jMfYnPcQm0YyzaV2oOOBdgVAdbkiHAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T01:38:10.369482Z"},"content_sha256":"0fcad3d814b3b1d82f4326fd0e575000a7f06ef50a331a28f13df85b451503ad","schema_version":"1.0","event_id":"sha256:0fcad3d814b3b1d82f4326fd0e575000a7f06ef50a331a28f13df85b451503ad"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2004:P3VGD7MVNWGQMOPHEXDJ5QQNIQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"4D equivalence theorem and gauge symmetry on orbifold","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"K. Hayakawa, K. Miyachi, M. Matsunaga, N. Haba, Y. Abe, Y. Matsumoto","submitted_at":"2004-02-19T11:40:41Z","abstract_excerpt":"We investigate the high-energy behavior of the scattering amplitudes in the extra dimensional gauge theory where the gauge symmetry is broken by the boundary condition. We study, in particular, the 5-dimensional SU(5) grand unified theory whose 5th-dimensional coordinate is compactified on S^1/Z_2. We pay attention to the gauge symmetry compatible with the boundary condition on the orbifold and give the BRST formalism of the 4D theory which is obtained through integration of the 5D theory along the extra dimension. We derive the 4D equivalence theorem on the basis of the Slavnov-Taylor identit"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0402146","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":"2026-05-18T01:05:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vVvusSCeOlvnENVrYvaf0a23R5dEar2h9ubmHXBsQInAKK87vWdOXmaiuKGQX+n1feiHjyijm5CY4E+RRmy2Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T01:38:10.370387Z"},"content_sha256":"c01ba971cc32c603cb2f0ee8f2a4125efb7abb7c32fff9c832badf2880a81315","schema_version":"1.0","event_id":"sha256:c01ba971cc32c603cb2f0ee8f2a4125efb7abb7c32fff9c832badf2880a81315"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/P3VGD7MVNWGQMOPHEXDJ5QQNIQ/bundle.json","state_url":"https://pith.science/pith/P3VGD7MVNWGQMOPHEXDJ5QQNIQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/P3VGD7MVNWGQMOPHEXDJ5QQNIQ/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":"2026-06-01T01:38:10Z","links":{"resolver":"https://pith.science/pith/P3VGD7MVNWGQMOPHEXDJ5QQNIQ","bundle":"https://pith.science/pith/P3VGD7MVNWGQMOPHEXDJ5QQNIQ/bundle.json","state":"https://pith.science/pith/P3VGD7MVNWGQMOPHEXDJ5QQNIQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/P3VGD7MVNWGQMOPHEXDJ5QQNIQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2004:P3VGD7MVNWGQMOPHEXDJ5QQNIQ","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":"cf20c38a15ca2fbdcce0d5e8d6d1cff569ee8f8d9033a6b32f5dd7037bc02f00","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"2004-02-19T11:40:41Z","title_canon_sha256":"8534ad8dd100716ad3c63d1381d2581ae6911d7901819898282c792af59f707e"},"schema_version":"1.0","source":{"id":"hep-th/0402146","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0402146","created_at":"2026-05-18T01:05:58Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0402146v1","created_at":"2026-05-18T01:05:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0402146","created_at":"2026-05-18T01:05:58Z"},{"alias_kind":"pith_short_12","alias_value":"P3VGD7MVNWGQ","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"P3VGD7MVNWGQMOPH","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"P3VGD7MV","created_at":"2026-05-18T12:25:52Z"}],"graph_snapshots":[{"event_id":"sha256:c01ba971cc32c603cb2f0ee8f2a4125efb7abb7c32fff9c832badf2880a81315","target":"graph","created_at":"2026-05-18T01:05:58Z","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 investigate the high-energy behavior of the scattering amplitudes in the extra dimensional gauge theory where the gauge symmetry is broken by the boundary condition. We study, in particular, the 5-dimensional SU(5) grand unified theory whose 5th-dimensional coordinate is compactified on S^1/Z_2. We pay attention to the gauge symmetry compatible with the boundary condition on the orbifold and give the BRST formalism of the 4D theory which is obtained through integration of the 5D theory along the extra dimension. We derive the 4D equivalence theorem on the basis of the Slavnov-Taylor identit","authors_text":"K. Hayakawa, K. Miyachi, M. Matsunaga, N. Haba, Y. Abe, Y. Matsumoto","cross_cats":[],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"2004-02-19T11:40:41Z","title":"4D equivalence theorem and gauge symmetry on orbifold"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0402146","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":"sha256:0fcad3d814b3b1d82f4326fd0e575000a7f06ef50a331a28f13df85b451503ad","target":"record","created_at":"2026-05-18T01:05:58Z","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":"cf20c38a15ca2fbdcce0d5e8d6d1cff569ee8f8d9033a6b32f5dd7037bc02f00","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"2004-02-19T11:40:41Z","title_canon_sha256":"8534ad8dd100716ad3c63d1381d2581ae6911d7901819898282c792af59f707e"},"schema_version":"1.0","source":{"id":"hep-th/0402146","kind":"arxiv","version":1}},"canonical_sha256":"7eea61fd956d8d0639e725c69ec20d441309315ca8d81ac310f34fef4bd3725a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7eea61fd956d8d0639e725c69ec20d441309315ca8d81ac310f34fef4bd3725a","first_computed_at":"2026-05-18T01:05:58.930110Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:05:58.930110Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Kyb+/KH0Ldu9pPP3e3ZFcr/o3izPnVz9DsfxbT1CJMLqYQ2LutS+SeVMrgEiMjqiCFopzAEaPm8HicjUJAwHAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:05:58.930586Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/0402146","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0fcad3d814b3b1d82f4326fd0e575000a7f06ef50a331a28f13df85b451503ad","sha256:c01ba971cc32c603cb2f0ee8f2a4125efb7abb7c32fff9c832badf2880a81315"],"state_sha256":"eeebaaaf3c984fea95975d3c8532c516b42e019a71608fdc298b478a513dd407"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"C7AEqRHhRi9krva/Ok6GqtmNnYFNkWP7/t7NM/79yumoBpS6hhMwN49/e+a131bMVrYgW5oNTJiW073HaDGcCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T01:38:10.376373Z","bundle_sha256":"622c336ef6a432cc54da340a67a8eb5bbbc172ac6678679954a6587c286a1821"}}