{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2003:D75NKDJYQVM4XBJTBAI7K23OT7","short_pith_number":"pith:D75NKDJY","canonical_record":{"source":{"id":"hep-th/0310130","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2003-10-14T12:17:04Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"2401b3850bc9757f529fb7160da47313807d9ddee2637813803c8ab8f406fa56","abstract_canon_sha256":"4fed8f4c3f24cec39488570dff35de38bd87e319e8c34913ba963ca048440273"},"schema_version":"1.0"},"canonical_sha256":"1ffad50d388559cb85330811f56b6e9fec17dff748de69d0b986dd6bbc914549","source":{"kind":"arxiv","id":"hep-th/0310130","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0310130","created_at":"2026-07-04T16:41:25Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0310130v2","created_at":"2026-07-04T16:41:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0310130","created_at":"2026-07-04T16:41:25Z"},{"alias_kind":"pith_short_12","alias_value":"D75NKDJYQVM4","created_at":"2026-07-04T16:41:25Z"},{"alias_kind":"pith_short_16","alias_value":"D75NKDJYQVM4XBJT","created_at":"2026-07-04T16:41:25Z"},{"alias_kind":"pith_short_8","alias_value":"D75NKDJY","created_at":"2026-07-04T16:41:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2003:D75NKDJYQVM4XBJTBAI7K23OT7","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/0310130","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2003-10-14T12:17:04Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"2401b3850bc9757f529fb7160da47313807d9ddee2637813803c8ab8f406fa56","abstract_canon_sha256":"4fed8f4c3f24cec39488570dff35de38bd87e319e8c34913ba963ca048440273"},"schema_version":"1.0"},"canonical_sha256":"1ffad50d388559cb85330811f56b6e9fec17dff748de69d0b986dd6bbc914549","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:41:25.701623Z","signature_b64":"3EL/xM1Onezn8zJd0YLw7l5k61iBz13YWgxo5PZaWCoNUXgfudXWlKH0Mkk72vr2S7JqJrpPUemCTml3y9RqBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1ffad50d388559cb85330811f56b6e9fec17dff748de69d0b986dd6bbc914549","last_reissued_at":"2026-07-04T16:41:25.701217Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:41:25.701217Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/0310130","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":"2026-07-04T16:41:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"f+f6Se0O1nkgfgpn/R5qHehZosGKgS7msqDRgwnGVeHxF/pZWuSPLHVrVwOZi+iRFB44jgeEYVLsJUFEuBAbCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-13T04:27:23.406479Z"},"content_sha256":"dc44ba8a2020b0d81c4e87f8f01d95ce8877bcc6f546050e34d997f5c276be10","schema_version":"1.0","event_id":"sha256:dc44ba8a2020b0d81c4e87f8f01d95ce8877bcc6f546050e34d997f5c276be10"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2003:D75NKDJYQVM4XBJTBAI7K23OT7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Massless Localized Vector Field on a Wall in D=5 SQED with Tensor Multiplets","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Keisuke Ohashi, Norisuke Sakai, Youichi Isozumi","submitted_at":"2003-10-14T12:17:04Z","abstract_excerpt":"Massless localized vector field is obtained in five-dimensional supersymmetric (SUSY) QED coupled to tensor multiplets as a half BPS solution. The four-dimensional gauge coupling is obtained as a topological charge. We also find all the (bosonic) massive modes exactly for a particular value of a parameter, demonstrating explicitly the existence of a mass gap. The four-dimensional Coulomb law is shown to hold for sources placed on the wall."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0310130","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/0310130/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-04T16:41:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OLB1VHu0CqnK40Zr/LjuY+YX5qd316ueYuTkeQELF3J+H/I2Mt0CFYTo7k9aLtTqX8XoZ5dmxFWGfx2DbOSVDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-13T04:27:23.407081Z"},"content_sha256":"0122d6444af1daa27f84adbd277f0dbac2842f6e151e3ae157014f16732dc00e","schema_version":"1.0","event_id":"sha256:0122d6444af1daa27f84adbd277f0dbac2842f6e151e3ae157014f16732dc00e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/D75NKDJYQVM4XBJTBAI7K23OT7/bundle.json","state_url":"https://pith.science/pith/D75NKDJYQVM4XBJTBAI7K23OT7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/D75NKDJYQVM4XBJTBAI7K23OT7/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":"2026-08-13T04:27:23Z","links":{"resolver":"https://pith.science/pith/D75NKDJYQVM4XBJTBAI7K23OT7","bundle":"https://pith.science/pith/D75NKDJYQVM4XBJTBAI7K23OT7/bundle.json","state":"https://pith.science/pith/D75NKDJYQVM4XBJTBAI7K23OT7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/D75NKDJYQVM4XBJTBAI7K23OT7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2003:D75NKDJYQVM4XBJTBAI7K23OT7","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":"4fed8f4c3f24cec39488570dff35de38bd87e319e8c34913ba963ca048440273","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"hep-th","submitted_at":"2003-10-14T12:17:04Z","title_canon_sha256":"2401b3850bc9757f529fb7160da47313807d9ddee2637813803c8ab8f406fa56"},"schema_version":"1.0","source":{"id":"hep-th/0310130","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0310130","created_at":"2026-07-04T16:41:25Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0310130v2","created_at":"2026-07-04T16:41:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0310130","created_at":"2026-07-04T16:41:25Z"},{"alias_kind":"pith_short_12","alias_value":"D75NKDJYQVM4","created_at":"2026-07-04T16:41:25Z"},{"alias_kind":"pith_short_16","alias_value":"D75NKDJYQVM4XBJT","created_at":"2026-07-04T16:41:25Z"},{"alias_kind":"pith_short_8","alias_value":"D75NKDJY","created_at":"2026-07-04T16:41:25Z"}],"graph_snapshots":[{"event_id":"sha256:0122d6444af1daa27f84adbd277f0dbac2842f6e151e3ae157014f16732dc00e","target":"graph","created_at":"2026-07-04T16:41:25Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-th/0310130/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Massless localized vector field is obtained in five-dimensional supersymmetric (SUSY) QED coupled to tensor multiplets as a half BPS solution. The four-dimensional gauge coupling is obtained as a topological charge. We also find all the (bosonic) massive modes exactly for a particular value of a parameter, demonstrating explicitly the existence of a mass gap. The four-dimensional Coulomb law is shown to hold for sources placed on the wall.","authors_text":"Keisuke Ohashi, Norisuke Sakai, Youichi Isozumi","cross_cats":["hep-ph"],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"2003-10-14T12:17:04Z","title":"Massless Localized Vector Field on a Wall in D=5 SQED with Tensor Multiplets"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0310130","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:dc44ba8a2020b0d81c4e87f8f01d95ce8877bcc6f546050e34d997f5c276be10","target":"record","created_at":"2026-07-04T16:41:25Z","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":"4fed8f4c3f24cec39488570dff35de38bd87e319e8c34913ba963ca048440273","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"hep-th","submitted_at":"2003-10-14T12:17:04Z","title_canon_sha256":"2401b3850bc9757f529fb7160da47313807d9ddee2637813803c8ab8f406fa56"},"schema_version":"1.0","source":{"id":"hep-th/0310130","kind":"arxiv","version":2}},"canonical_sha256":"1ffad50d388559cb85330811f56b6e9fec17dff748de69d0b986dd6bbc914549","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1ffad50d388559cb85330811f56b6e9fec17dff748de69d0b986dd6bbc914549","first_computed_at":"2026-07-04T16:41:25.701217Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:41:25.701217Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"3EL/xM1Onezn8zJd0YLw7l5k61iBz13YWgxo5PZaWCoNUXgfudXWlKH0Mkk72vr2S7JqJrpPUemCTml3y9RqBA==","signature_status":"signed_v1","signed_at":"2026-07-04T16:41:25.701623Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/0310130","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:dc44ba8a2020b0d81c4e87f8f01d95ce8877bcc6f546050e34d997f5c276be10","sha256:0122d6444af1daa27f84adbd277f0dbac2842f6e151e3ae157014f16732dc00e"],"state_sha256":"18500d903b2dbbe6e8f43269ad2a101fa3588723c795332e6b9c6689ba12d175"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WaeOcsS9UB9AcFAxG3umjnh5Ua6HxOc9S2tXxDJh+VuzLWMkZ4d72eHQ6OfQf1wbsep/ANf87jKlSrvVtGTbBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-13T04:27:23.417850Z","bundle_sha256":"34651a17862fad7659e022408f94857c53371138b37b1dcf167d57859181633a"}}