{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2003:AD7QJ46Q6AKW7E75NFKGBLHLIH","short_pith_number":"pith:AD7QJ46Q","canonical_record":{"source":{"id":"hep-th/0305085","kind":"arxiv","version":4},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2003-05-10T13:27:18Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"269bb9d1d9e291735984c10043911b0d8b843b6d7795649fb1335f5338e759ab","abstract_canon_sha256":"2808c44107eb33cdefa325e9756f82fdb508d50b11c1b35af1cd671bb8cc697b"},"schema_version":"1.0"},"canonical_sha256":"00ff04f3d0f0156f93fd695460aceb41f35085e80be141ea691af97d1c9e1c06","source":{"kind":"arxiv","id":"hep-th/0305085","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0305085","created_at":"2026-05-18T01:38:48Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0305085v4","created_at":"2026-05-18T01:38:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0305085","created_at":"2026-05-18T01:38:48Z"},{"alias_kind":"pith_short_12","alias_value":"AD7QJ46Q6AKW","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_16","alias_value":"AD7QJ46Q6AKW7E75","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_8","alias_value":"AD7QJ46Q","created_at":"2026-05-18T12:25:51Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2003:AD7QJ46Q6AKW7E75NFKGBLHLIH","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/0305085","kind":"arxiv","version":4},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2003-05-10T13:27:18Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"269bb9d1d9e291735984c10043911b0d8b843b6d7795649fb1335f5338e759ab","abstract_canon_sha256":"2808c44107eb33cdefa325e9756f82fdb508d50b11c1b35af1cd671bb8cc697b"},"schema_version":"1.0"},"canonical_sha256":"00ff04f3d0f0156f93fd695460aceb41f35085e80be141ea691af97d1c9e1c06","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:38:48.633349Z","signature_b64":"0bCQbM20xXtkwb5CMRteQQy39Ei1nhit6dwSOMiazCab+FB5ug1YGrk5OAnDth4Noy92QM64/nIqptXaWgVeBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"00ff04f3d0f0156f93fd695460aceb41f35085e80be141ea691af97d1c9e1c06","last_reissued_at":"2026-05-18T01:38:48.632848Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:38:48.632848Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/0305085","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:38:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bqK6QMgFSk7tO+o+Tjik6Q5zh2cWcFMXD331kRzjUncixRfn7ucSvvHZ/jDc+uMcFHabV2WO1LSqD0ZFJlw5CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T17:23:11.358377Z"},"content_sha256":"feacf3950d56aa509dc6a85827cc1d0fd8a9a9bf6364d812681f1bc3bd9d46db","schema_version":"1.0","event_id":"sha256:feacf3950d56aa509dc6a85827cc1d0fd8a9a9bf6364d812681f1bc3bd9d46db"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2003:AD7QJ46Q6AKW7E75NFKGBLHLIH","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Wilson lines corrections to gauge couplings from a field theory approach","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"D.M. Ghilencea","submitted_at":"2003-05-10T13:27:18Z","abstract_excerpt":"Using an effective field theory approach, we address the effects on the gauge couplings of one and two additional compact dimensions in the presence of a constant background (gauge) field. Such background fields are a generic presence in models with extra dimensions and can be employed for gauge symmetry breaking mechanisms in the context of 4D N=1 supersymmetric models. The structure of the ultraviolet (UV) and infrared (IR) divergences that the gauge couplings develop in the presence of Wilson line vev's is investigated. One-loop radiative corrections to the gauge couplings due to overlappin"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0305085","kind":"arxiv","version":4},"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":"2026-05-18T01:38:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tY2+i1o7DM/0r5DnsXXhpmwvWlyZUfPrzAklrftw8LncUgBihT93zcUNUsHu1CqoLO26bUUh2RExhMzrI2VSCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T17:23:11.359037Z"},"content_sha256":"24de0968114246a38d6e2eea9e44700c7304557642ade8d46edb698990c4b84f","schema_version":"1.0","event_id":"sha256:24de0968114246a38d6e2eea9e44700c7304557642ade8d46edb698990c4b84f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/AD7QJ46Q6AKW7E75NFKGBLHLIH/bundle.json","state_url":"https://pith.science/pith/AD7QJ46Q6AKW7E75NFKGBLHLIH/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/AD7QJ46Q6AKW7E75NFKGBLHLIH/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":"2026-06-10T17:23:11Z","links":{"resolver":"https://pith.science/pith/AD7QJ46Q6AKW7E75NFKGBLHLIH","bundle":"https://pith.science/pith/AD7QJ46Q6AKW7E75NFKGBLHLIH/bundle.json","state":"https://pith.science/pith/AD7QJ46Q6AKW7E75NFKGBLHLIH/state.json","well_known_bundle":"https://pith.science/.well-known/pith/AD7QJ46Q6AKW7E75NFKGBLHLIH/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2003:AD7QJ46Q6AKW7E75NFKGBLHLIH","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":"2808c44107eb33cdefa325e9756f82fdb508d50b11c1b35af1cd671bb8cc697b","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"hep-th","submitted_at":"2003-05-10T13:27:18Z","title_canon_sha256":"269bb9d1d9e291735984c10043911b0d8b843b6d7795649fb1335f5338e759ab"},"schema_version":"1.0","source":{"id":"hep-th/0305085","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0305085","created_at":"2026-05-18T01:38:48Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0305085v4","created_at":"2026-05-18T01:38:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0305085","created_at":"2026-05-18T01:38:48Z"},{"alias_kind":"pith_short_12","alias_value":"AD7QJ46Q6AKW","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_16","alias_value":"AD7QJ46Q6AKW7E75","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_8","alias_value":"AD7QJ46Q","created_at":"2026-05-18T12:25:51Z"}],"graph_snapshots":[{"event_id":"sha256:24de0968114246a38d6e2eea9e44700c7304557642ade8d46edb698990c4b84f","target":"graph","created_at":"2026-05-18T01:38:48Z","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":"Using an effective field theory approach, we address the effects on the gauge couplings of one and two additional compact dimensions in the presence of a constant background (gauge) field. Such background fields are a generic presence in models with extra dimensions and can be employed for gauge symmetry breaking mechanisms in the context of 4D N=1 supersymmetric models. The structure of the ultraviolet (UV) and infrared (IR) divergences that the gauge couplings develop in the presence of Wilson line vev's is investigated. One-loop radiative corrections to the gauge couplings due to overlappin","authors_text":"D.M. Ghilencea","cross_cats":["hep-ph"],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"2003-05-10T13:27:18Z","title":"Wilson lines corrections to gauge couplings from a field theory approach"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0305085","kind":"arxiv","version":4},"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:feacf3950d56aa509dc6a85827cc1d0fd8a9a9bf6364d812681f1bc3bd9d46db","target":"record","created_at":"2026-05-18T01:38:48Z","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":"2808c44107eb33cdefa325e9756f82fdb508d50b11c1b35af1cd671bb8cc697b","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"hep-th","submitted_at":"2003-05-10T13:27:18Z","title_canon_sha256":"269bb9d1d9e291735984c10043911b0d8b843b6d7795649fb1335f5338e759ab"},"schema_version":"1.0","source":{"id":"hep-th/0305085","kind":"arxiv","version":4}},"canonical_sha256":"00ff04f3d0f0156f93fd695460aceb41f35085e80be141ea691af97d1c9e1c06","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"00ff04f3d0f0156f93fd695460aceb41f35085e80be141ea691af97d1c9e1c06","first_computed_at":"2026-05-18T01:38:48.632848Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:38:48.632848Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"0bCQbM20xXtkwb5CMRteQQy39Ei1nhit6dwSOMiazCab+FB5ug1YGrk5OAnDth4Noy92QM64/nIqptXaWgVeBg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:38:48.633349Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/0305085","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:feacf3950d56aa509dc6a85827cc1d0fd8a9a9bf6364d812681f1bc3bd9d46db","sha256:24de0968114246a38d6e2eea9e44700c7304557642ade8d46edb698990c4b84f"],"state_sha256":"fcc7dce849de27b828af99c53211d70ecba968d1c710d3a86a63a24fecf9f83a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CiU2LZOEfzXx9oqqibL8ePuttkKbT2oWwqugjc3ACJGLSWGkvno6/RZjc/glnGzWaAYhbwTgAEMriTNLJ5B+Dw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-10T17:23:11.363034Z","bundle_sha256":"1a14d70c43a59cd7ffd8aed99eb979729a9a72504486eec67f994ec5739e8bb7"}}