{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:JRUJMKIIOH6IT7LGRXYQOCBVTH","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":"665b3d1fee050781e95a0f6a9e5700a3cfc7b38daa4adeb5f960fc5ae43f448a","cross_cats_sorted":["astro-ph.CO","cond-mat.mes-hall","hep-ph","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-06-10T18:00:00Z","title_canon_sha256":"f19afba515b63b3873b4593e1ab545899f8ecc5473d2bdd78e71015ed5ad85bb"},"schema_version":"1.0","source":{"id":"2606.12513","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2606.12513","created_at":"2026-06-12T00:07:52Z"},{"alias_kind":"arxiv_version","alias_value":"2606.12513v1","created_at":"2026-06-12T00:07:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.12513","created_at":"2026-06-12T00:07:52Z"},{"alias_kind":"pith_short_12","alias_value":"JRUJMKIIOH6I","created_at":"2026-06-12T00:07:52Z"},{"alias_kind":"pith_short_16","alias_value":"JRUJMKIIOH6IT7LG","created_at":"2026-06-12T00:07:52Z"},{"alias_kind":"pith_short_8","alias_value":"JRUJMKII","created_at":"2026-06-12T00:07:52Z"}],"graph_snapshots":[{"event_id":"sha256:6b9eddc5e34e7ed7cbda723ad051d7df57a0cd03e8b9792a86b3a70c7e182f1b","target":"graph","created_at":"2026-06-12T00:07:52Z","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/2606.12513/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We analyze Maxwell theory coupled to an axion domain wall as a spectral boundary value problem. We find that a finite-width axion domain wall generically supports a localized normalizable chiral electromagnetic mode with linear, gapless dispersion. This mode arises from helicity-dependent coupling sourced by the axion gradient: one polarization experiences an effective attractive potential and forms a bound state, while the opposite polarization is repelled. The existence of this chiral surface photon is robust over a wide regime of wall structures and axion masses. Our result shows that axion","authors_text":"Nemanja Kaloper","cross_cats":["astro-ph.CO","cond-mat.mes-hall","hep-ph","physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-06-10T18:00:00Z","title":"Localization of Chiral Electromagnetic Waves on Thick Axion Domain Walls"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.12513","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":"sha256:6e088366c6be00cfd3debe25065606d790f5af5e92b6f461aa7b3b545a720e5a","target":"record","created_at":"2026-06-12T00:07:52Z","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":"665b3d1fee050781e95a0f6a9e5700a3cfc7b38daa4adeb5f960fc5ae43f448a","cross_cats_sorted":["astro-ph.CO","cond-mat.mes-hall","hep-ph","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-06-10T18:00:00Z","title_canon_sha256":"f19afba515b63b3873b4593e1ab545899f8ecc5473d2bdd78e71015ed5ad85bb"},"schema_version":"1.0","source":{"id":"2606.12513","kind":"arxiv","version":1}},"canonical_sha256":"4c6896290871fc89fd668df107083599f9117ddae2c8b64bf483b12b028c1a45","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4c6896290871fc89fd668df107083599f9117ddae2c8b64bf483b12b028c1a45","first_computed_at":"2026-06-12T00:07:52.958826Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-12T00:07:52.958826Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"+0Q8NWCEM35uwFGYnI26DQiZonyYH9vjRqoyaaxIVGsyYh0cjq6gB0nYtk+rhOnFUVYCVedCyJWbXfqXvkopCQ==","signature_status":"signed_v1","signed_at":"2026-06-12T00:07:52.959247Z","signed_message":"canonical_sha256_bytes"},"source_id":"2606.12513","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6e088366c6be00cfd3debe25065606d790f5af5e92b6f461aa7b3b545a720e5a","sha256:6b9eddc5e34e7ed7cbda723ad051d7df57a0cd03e8b9792a86b3a70c7e182f1b"],"state_sha256":"d610875965aceca2aadfc35e596d6b8e8871d0e4b597db1b81e96187b469476b"}