{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:T2IAA5ELEHAJST5D6QVIPK5CQ7","short_pith_number":"pith:T2IAA5EL","canonical_record":{"source":{"id":"1701.07375","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-01-25T16:56:42Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"604179e44cdc409d0d142594fc3e5aa0e5c3e5d537fae3e781c796421855bbf0","abstract_canon_sha256":"7f42b8884eec2e968159c5b07ee35456efcbc458b54755b63dbc53beb46a46ff"},"schema_version":"1.0"},"canonical_sha256":"9e9000748b21c0994fa3f42a87aba287fb08771a9595a3418d2261c77eeca309","source":{"kind":"arxiv","id":"1701.07375","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1701.07375","created_at":"2026-05-18T00:45:58Z"},{"alias_kind":"arxiv_version","alias_value":"1701.07375v3","created_at":"2026-05-18T00:45:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1701.07375","created_at":"2026-05-18T00:45:58Z"},{"alias_kind":"pith_short_12","alias_value":"T2IAA5ELEHAJ","created_at":"2026-05-18T12:31:43Z"},{"alias_kind":"pith_short_16","alias_value":"T2IAA5ELEHAJST5D","created_at":"2026-05-18T12:31:43Z"},{"alias_kind":"pith_short_8","alias_value":"T2IAA5EL","created_at":"2026-05-18T12:31:43Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:T2IAA5ELEHAJST5D6QVIPK5CQ7","target":"record","payload":{"canonical_record":{"source":{"id":"1701.07375","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-01-25T16:56:42Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"604179e44cdc409d0d142594fc3e5aa0e5c3e5d537fae3e781c796421855bbf0","abstract_canon_sha256":"7f42b8884eec2e968159c5b07ee35456efcbc458b54755b63dbc53beb46a46ff"},"schema_version":"1.0"},"canonical_sha256":"9e9000748b21c0994fa3f42a87aba287fb08771a9595a3418d2261c77eeca309","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:45:58.304959Z","signature_b64":"Mezym9KxiR//k/NFj/DTbX8vWO3Vl8xU/LE9eMRUey4E6q4PK42WXwtZYWPW27eWckxLYs1oKR+/II2nvA2XDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9e9000748b21c0994fa3f42a87aba287fb08771a9595a3418d2261c77eeca309","last_reissued_at":"2026-05-18T00:45:58.304488Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:45:58.304488Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1701.07375","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:45:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ef150LJCCbciCiQGhR5YK4aryyQyX/NkqnvahcMi0H8IMpdeq79/3/IuqViUNZrIB3e4ybYUOpED8CN3XQwwBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T06:13:46.664240Z"},"content_sha256":"439ea7dbc001df34d92cddd93947aa39ddb87a87f17c824772d0fef43051d8f5","schema_version":"1.0","event_id":"sha256:439ea7dbc001df34d92cddd93947aa39ddb87a87f17c824772d0fef43051d8f5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:T2IAA5ELEHAJST5D6QVIPK5CQ7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Polarization effects in light-by-light scattering: Euler-Heisenberg versus Born-Infeld","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"hep-ph","authors_text":"A. Rebhan, G. Turk","submitted_at":"2017-01-25T16:56:42Z","abstract_excerpt":"The angular dependence of the differential cross section of unpolarized light-by-light scattering summed over final polarizations is the same in any low-energy effective theory of quantum electrodynamics and also in Born-Infeld electrodynamics. In this paper we derive general expressions for polarization-dependent low-energy scattering amplitudes, including a hypothetical parity-violating situation. These are evaluated for quantum electrodynamics with charged scalar or spinor particles, which give strikingly different polarization effects. Ordinary quantum electrodynamics is found to exhibit r"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1701.07375","kind":"arxiv","version":3},"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":"2026-05-18T00:45:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fOfiUcqGPC76uANeV+W44enhGg+ywjNOURAHPIqGvFfmnb+dp2wx9eyt/jGighaKbg0LtJ+Ki1YpE6gYYkC2BQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T06:13:46.664629Z"},"content_sha256":"934310953e1729e36b829f8a734d76f926e4a3e77345406cd332aa41ad5e2c07","schema_version":"1.0","event_id":"sha256:934310953e1729e36b829f8a734d76f926e4a3e77345406cd332aa41ad5e2c07"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/T2IAA5ELEHAJST5D6QVIPK5CQ7/bundle.json","state_url":"https://pith.science/pith/T2IAA5ELEHAJST5D6QVIPK5CQ7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/T2IAA5ELEHAJST5D6QVIPK5CQ7/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":"2026-05-28T06:13:46Z","links":{"resolver":"https://pith.science/pith/T2IAA5ELEHAJST5D6QVIPK5CQ7","bundle":"https://pith.science/pith/T2IAA5ELEHAJST5D6QVIPK5CQ7/bundle.json","state":"https://pith.science/pith/T2IAA5ELEHAJST5D6QVIPK5CQ7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/T2IAA5ELEHAJST5D6QVIPK5CQ7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:T2IAA5ELEHAJST5D6QVIPK5CQ7","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":"7f42b8884eec2e968159c5b07ee35456efcbc458b54755b63dbc53beb46a46ff","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-01-25T16:56:42Z","title_canon_sha256":"604179e44cdc409d0d142594fc3e5aa0e5c3e5d537fae3e781c796421855bbf0"},"schema_version":"1.0","source":{"id":"1701.07375","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1701.07375","created_at":"2026-05-18T00:45:58Z"},{"alias_kind":"arxiv_version","alias_value":"1701.07375v3","created_at":"2026-05-18T00:45:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1701.07375","created_at":"2026-05-18T00:45:58Z"},{"alias_kind":"pith_short_12","alias_value":"T2IAA5ELEHAJ","created_at":"2026-05-18T12:31:43Z"},{"alias_kind":"pith_short_16","alias_value":"T2IAA5ELEHAJST5D","created_at":"2026-05-18T12:31:43Z"},{"alias_kind":"pith_short_8","alias_value":"T2IAA5EL","created_at":"2026-05-18T12:31:43Z"}],"graph_snapshots":[{"event_id":"sha256:934310953e1729e36b829f8a734d76f926e4a3e77345406cd332aa41ad5e2c07","target":"graph","created_at":"2026-05-18T00:45:58Z","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":"The angular dependence of the differential cross section of unpolarized light-by-light scattering summed over final polarizations is the same in any low-energy effective theory of quantum electrodynamics and also in Born-Infeld electrodynamics. In this paper we derive general expressions for polarization-dependent low-energy scattering amplitudes, including a hypothetical parity-violating situation. These are evaluated for quantum electrodynamics with charged scalar or spinor particles, which give strikingly different polarization effects. Ordinary quantum electrodynamics is found to exhibit r","authors_text":"A. Rebhan, G. Turk","cross_cats":["physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-01-25T16:56:42Z","title":"Polarization effects in light-by-light scattering: Euler-Heisenberg versus Born-Infeld"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1701.07375","kind":"arxiv","version":3},"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":"sha256:439ea7dbc001df34d92cddd93947aa39ddb87a87f17c824772d0fef43051d8f5","target":"record","created_at":"2026-05-18T00:45:58Z","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":"7f42b8884eec2e968159c5b07ee35456efcbc458b54755b63dbc53beb46a46ff","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-01-25T16:56:42Z","title_canon_sha256":"604179e44cdc409d0d142594fc3e5aa0e5c3e5d537fae3e781c796421855bbf0"},"schema_version":"1.0","source":{"id":"1701.07375","kind":"arxiv","version":3}},"canonical_sha256":"9e9000748b21c0994fa3f42a87aba287fb08771a9595a3418d2261c77eeca309","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9e9000748b21c0994fa3f42a87aba287fb08771a9595a3418d2261c77eeca309","first_computed_at":"2026-05-18T00:45:58.304488Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:45:58.304488Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Mezym9KxiR//k/NFj/DTbX8vWO3Vl8xU/LE9eMRUey4E6q4PK42WXwtZYWPW27eWckxLYs1oKR+/II2nvA2XDw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:45:58.304959Z","signed_message":"canonical_sha256_bytes"},"source_id":"1701.07375","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:439ea7dbc001df34d92cddd93947aa39ddb87a87f17c824772d0fef43051d8f5","sha256:934310953e1729e36b829f8a734d76f926e4a3e77345406cd332aa41ad5e2c07"],"state_sha256":"3129c88195a420ab25ed14bd121fd3144282d3d4c9160034d71dd9bbe1258d43"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KZb/FWtBg5R7FHxfPdZ+vPiBRzHCmpPUOZnpxImk/r9yqj3rko2hL1wbgPh51UGTuzSBOXYbw4fBCRdH0GS2BA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T06:13:46.666656Z","bundle_sha256":"d16ddb32a563b8c04ffb26224ac0fc088298fb61b48529e8e400ce31183f17da"}}