{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:AUVHHNMQDKSOENVFZZWC5LFZ3W","short_pith_number":"pith:AUVHHNMQ","canonical_record":{"source":{"id":"2411.13514","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-11-20T18:07:30Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"e14e70340bb6fd9996fb81414acd9d67d8de050ff3b31351062925d230b87d7b","abstract_canon_sha256":"177305e94136efbb1eb04b98140ad7dc63dca4f63513364f5a76f1b0cd114e44"},"schema_version":"1.0"},"canonical_sha256":"052a73b5901aa4e236a5ce6c2eacb9ddb6c74d4f3bdfdcdfad8e2232f18a118f","source":{"kind":"arxiv","id":"2411.13514","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2411.13514","created_at":"2026-07-05T09:38:18Z"},{"alias_kind":"arxiv_version","alias_value":"2411.13514v1","created_at":"2026-07-05T09:38:18Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.13514","created_at":"2026-07-05T09:38:18Z"},{"alias_kind":"pith_short_12","alias_value":"AUVHHNMQDKSO","created_at":"2026-07-05T09:38:18Z"},{"alias_kind":"pith_short_16","alias_value":"AUVHHNMQDKSOENVF","created_at":"2026-07-05T09:38:18Z"},{"alias_kind":"pith_short_8","alias_value":"AUVHHNMQ","created_at":"2026-07-05T09:38:18Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:AUVHHNMQDKSOENVFZZWC5LFZ3W","target":"record","payload":{"canonical_record":{"source":{"id":"2411.13514","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-11-20T18:07:30Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"e14e70340bb6fd9996fb81414acd9d67d8de050ff3b31351062925d230b87d7b","abstract_canon_sha256":"177305e94136efbb1eb04b98140ad7dc63dca4f63513364f5a76f1b0cd114e44"},"schema_version":"1.0"},"canonical_sha256":"052a73b5901aa4e236a5ce6c2eacb9ddb6c74d4f3bdfdcdfad8e2232f18a118f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:38:18.477547Z","signature_b64":"++PZPwvOPLE45YglQcH48CtK1XohOkujycznL1sjXeIxrGQi2RiZ/yhN2lwjLcaCJVZr0cU5Qy8YXRGZVjVHCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"052a73b5901aa4e236a5ce6c2eacb9ddb6c74d4f3bdfdcdfad8e2232f18a118f","last_reissued_at":"2026-07-05T09:38:18.477075Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:38:18.477075Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2411.13514","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":"2026-07-05T09:38:18Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YhO1r0ox7+qCbVkhemwdsFF+Axn60HkkxlWF5YZOeVGbW0PmXdY2GysWotcV9/fI9e7u59FcfQDpGw1ujKlSDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-14T19:07:13.397311Z"},"content_sha256":"8cf82cb5a1e253f22d4049c1f8dce754f829cbdae4c2351d87a69a31755c652f","schema_version":"1.0","event_id":"sha256:8cf82cb5a1e253f22d4049c1f8dce754f829cbdae4c2351d87a69a31755c652f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:AUVHHNMQDKSOENVFZZWC5LFZ3W","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Localized Electromagnetic Perturbations on Vector Solitons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Eduard Kim, Emin Nugaev, Yakov Shnir, Yulia Galushkina","submitted_at":"2024-11-20T18:07:30Z","abstract_excerpt":"Using effective field theory approach one can describe localization of electromagnetic field on a non-topological soliton. Pursuing this aim we consider the U(1) gauge theory with gauge kinetic coupling to a self-interacting complex neutral Proca field. The model possesses single energy scale given by the vector boson mass. Considering spherically symmetric stationary configurations, we study vibrational modes of the Proca field on the background of the soliton and discuss their properties."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.13514","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2411.13514/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":"2026-07-05T09:38:18Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"iJ/wT4ocaHOe7OKeLs+f+fqom1gFTPccNx9XVzTUoARSpF5NLF5GxaZlITgukHKVsakxCy7CJPTwr8qB40ZHBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-14T19:07:13.397837Z"},"content_sha256":"00a25d0f2710030e3b7143bc54eb9772eff6862434661825f09f06199cfc7f0e","schema_version":"1.0","event_id":"sha256:00a25d0f2710030e3b7143bc54eb9772eff6862434661825f09f06199cfc7f0e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/AUVHHNMQDKSOENVFZZWC5LFZ3W/bundle.json","state_url":"https://pith.science/pith/AUVHHNMQDKSOENVFZZWC5LFZ3W/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/AUVHHNMQDKSOENVFZZWC5LFZ3W/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":"2026-08-14T19:07:13Z","links":{"resolver":"https://pith.science/pith/AUVHHNMQDKSOENVFZZWC5LFZ3W","bundle":"https://pith.science/pith/AUVHHNMQDKSOENVFZZWC5LFZ3W/bundle.json","state":"https://pith.science/pith/AUVHHNMQDKSOENVFZZWC5LFZ3W/state.json","well_known_bundle":"https://pith.science/.well-known/pith/AUVHHNMQDKSOENVFZZWC5LFZ3W/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:AUVHHNMQDKSOENVFZZWC5LFZ3W","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":"177305e94136efbb1eb04b98140ad7dc63dca4f63513364f5a76f1b0cd114e44","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-11-20T18:07:30Z","title_canon_sha256":"e14e70340bb6fd9996fb81414acd9d67d8de050ff3b31351062925d230b87d7b"},"schema_version":"1.0","source":{"id":"2411.13514","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2411.13514","created_at":"2026-07-05T09:38:18Z"},{"alias_kind":"arxiv_version","alias_value":"2411.13514v1","created_at":"2026-07-05T09:38:18Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.13514","created_at":"2026-07-05T09:38:18Z"},{"alias_kind":"pith_short_12","alias_value":"AUVHHNMQDKSO","created_at":"2026-07-05T09:38:18Z"},{"alias_kind":"pith_short_16","alias_value":"AUVHHNMQDKSOENVF","created_at":"2026-07-05T09:38:18Z"},{"alias_kind":"pith_short_8","alias_value":"AUVHHNMQ","created_at":"2026-07-05T09:38:18Z"}],"graph_snapshots":[{"event_id":"sha256:00a25d0f2710030e3b7143bc54eb9772eff6862434661825f09f06199cfc7f0e","target":"graph","created_at":"2026-07-05T09:38:18Z","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/2411.13514/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Using effective field theory approach one can describe localization of electromagnetic field on a non-topological soliton. Pursuing this aim we consider the U(1) gauge theory with gauge kinetic coupling to a self-interacting complex neutral Proca field. The model possesses single energy scale given by the vector boson mass. Considering spherically symmetric stationary configurations, we study vibrational modes of the Proca field on the background of the soliton and discuss their properties.","authors_text":"Eduard Kim, Emin Nugaev, Yakov Shnir, Yulia Galushkina","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-11-20T18:07:30Z","title":"Localized Electromagnetic Perturbations on Vector Solitons"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.13514","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":"sha256:8cf82cb5a1e253f22d4049c1f8dce754f829cbdae4c2351d87a69a31755c652f","target":"record","created_at":"2026-07-05T09:38:18Z","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":"177305e94136efbb1eb04b98140ad7dc63dca4f63513364f5a76f1b0cd114e44","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-11-20T18:07:30Z","title_canon_sha256":"e14e70340bb6fd9996fb81414acd9d67d8de050ff3b31351062925d230b87d7b"},"schema_version":"1.0","source":{"id":"2411.13514","kind":"arxiv","version":1}},"canonical_sha256":"052a73b5901aa4e236a5ce6c2eacb9ddb6c74d4f3bdfdcdfad8e2232f18a118f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"052a73b5901aa4e236a5ce6c2eacb9ddb6c74d4f3bdfdcdfad8e2232f18a118f","first_computed_at":"2026-07-05T09:38:18.477075Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T09:38:18.477075Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"++PZPwvOPLE45YglQcH48CtK1XohOkujycznL1sjXeIxrGQi2RiZ/yhN2lwjLcaCJVZr0cU5Qy8YXRGZVjVHCg==","signature_status":"signed_v1","signed_at":"2026-07-05T09:38:18.477547Z","signed_message":"canonical_sha256_bytes"},"source_id":"2411.13514","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8cf82cb5a1e253f22d4049c1f8dce754f829cbdae4c2351d87a69a31755c652f","sha256:00a25d0f2710030e3b7143bc54eb9772eff6862434661825f09f06199cfc7f0e"],"state_sha256":"eb72dd1a124e1cbb247a5d39bd5e85505b6d3cce776d88c10a607eba63c29ff2"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LRV+sVFc9wZjScNXYJ4mxz3KiksMOSKvL4pWcj+dX7MQfMZE1Ztywog2fODN/KLrTC/FKcgaTJ/n4eMQ8wL4Aw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-14T19:07:13.402564Z","bundle_sha256":"8c11e14aa95c0a877c9012290a9334721531b5c6c4eaa5e3356e55571761aba0"}}