{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:EPYJPJZ44EDDPGYMJDMLECIFJJ","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":"0f0e0905a357820223b565532cb8024033fa75e6b254512f73f4217715d310b0","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2021-03-12T08:27:03Z","title_canon_sha256":"4867209e1e75a1312218f98657e9153c8303c2de931ee1af3c215d91a0c690c3"},"schema_version":"1.0","source":{"id":"2103.08343","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2103.08343","created_at":"2026-07-05T02:59:36Z"},{"alias_kind":"arxiv_version","alias_value":"2103.08343v1","created_at":"2026-07-05T02:59:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2103.08343","created_at":"2026-07-05T02:59:36Z"},{"alias_kind":"pith_short_12","alias_value":"EPYJPJZ44EDD","created_at":"2026-07-05T02:59:36Z"},{"alias_kind":"pith_short_16","alias_value":"EPYJPJZ44EDDPGYM","created_at":"2026-07-05T02:59:36Z"},{"alias_kind":"pith_short_8","alias_value":"EPYJPJZ4","created_at":"2026-07-05T02:59:36Z"}],"graph_snapshots":[{"event_id":"sha256:b8172cfdccb57563f22d077cf1ada78af75d980948d22de6419c3c62b4110fac","target":"graph","created_at":"2026-07-05T02:59:36Z","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/2103.08343/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"YES! We introduce a variable power Maxwell nonlinear electrodynamics theory which can remove the singularity of electric field of point-like charges at their locations. One of the main problems of Maxwell's electromagnetic field theory is related to the existence of singularity for electric field of point-like charges at their locations. In other words, the electric field of a point-like charge diverges at the charge location which leads to an infinite self-energy. In order to remove this singularity a few nonlinear electrodynamics (NED) theories have been introduced. Born-Infeld (BI) NED theo","authors_text":"Behzad Eslam Panah","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2021-03-12T08:27:03Z","title":"Can the power Maxwell nonlinear electrodynamics theory remove the singularity of electric field of point-like charges at their locations?"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2103.08343","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":"sha256:521ed316a545ed9c89dc2029f1fff0d7cca2af8510a9a1e7cd94b12c9327d1e6","target":"record","created_at":"2026-07-05T02:59:36Z","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":"0f0e0905a357820223b565532cb8024033fa75e6b254512f73f4217715d310b0","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2021-03-12T08:27:03Z","title_canon_sha256":"4867209e1e75a1312218f98657e9153c8303c2de931ee1af3c215d91a0c690c3"},"schema_version":"1.0","source":{"id":"2103.08343","kind":"arxiv","version":1}},"canonical_sha256":"23f097a73ce106379b0c48d8b209054a61e6adbe85ce848f80f1f203fbaddf1f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"23f097a73ce106379b0c48d8b209054a61e6adbe85ce848f80f1f203fbaddf1f","first_computed_at":"2026-07-05T02:59:36.797672Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T02:59:36.797672Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"FJAU6bdG5neZTXkKlN3Y5aA4iRQd0lty6omiV0Rc0mAMX6iARglZBhx61gXzF7ccclxnwFm4O1RQgBlHrJ/eBg==","signature_status":"signed_v1","signed_at":"2026-07-05T02:59:36.798034Z","signed_message":"canonical_sha256_bytes"},"source_id":"2103.08343","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:521ed316a545ed9c89dc2029f1fff0d7cca2af8510a9a1e7cd94b12c9327d1e6","sha256:b8172cfdccb57563f22d077cf1ada78af75d980948d22de6419c3c62b4110fac"],"state_sha256":"5283dfb80d32c42feb97e9bce2877257be40532ab1f22bf56522fd9636c63a49"}