{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:5F7LK2B5MP4OZXXW6T2L7QIXNL","short_pith_number":"pith:5F7LK2B5","schema_version":"1.0","canonical_sha256":"e97eb5683d63f8ecdef6f4f4bfc1176ae09640269f5b40d9674a8ea73290927c","source":{"kind":"arxiv","id":"1412.3390","version":1},"attestation_state":"computed","paper":{"title":"Self-induced mode mixing of ultraintense lasers in vacuum","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"physics.optics","authors_text":"Angel Paredes, Daniele Tommasini, David Novoa","submitted_at":"2014-12-10T17:55:25Z","abstract_excerpt":"We study the effects of the quantum vacuum on the propagation of a Gaussian laser beam in vacuum. By means of a double perturbative expansion in paraxiality and quantum vacuum terms, we provide analytical expressions for the self-induced transverse mode mixing, rotation of polarization, and third harmonic generarion. We discuss the possibility of searching for the self-induced, spatially dependent phase shift of a multipetawatt laser pulse, which may allow the testing of quantum electrodynamics and new physics models, such as Born-Infeld theory and models involving new minicharged or axion-lik"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1412.3390","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-12-10T17:55:25Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"6db65fce5a9dd70f43b3560d5ee8fe94d0f01baf1cede5209f34a43602d4ab9d","abstract_canon_sha256":"faf3af22d880c613687f0082fd08a00ede44d9eed3605283ed840da644dc7561"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:41:20.052959Z","signature_b64":"OlefCQF31T31KAbiOiBgrkhvWxlKPPnXAqrVB3DgO1e/XdznXYwT04ixEtNA2yjZeSjm3OIVaE/BSQIvyUdXAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e97eb5683d63f8ecdef6f4f4bfc1176ae09640269f5b40d9674a8ea73290927c","last_reissued_at":"2026-05-18T01:41:20.052373Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:41:20.052373Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Self-induced mode mixing of ultraintense lasers in vacuum","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"physics.optics","authors_text":"Angel Paredes, Daniele Tommasini, David Novoa","submitted_at":"2014-12-10T17:55:25Z","abstract_excerpt":"We study the effects of the quantum vacuum on the propagation of a Gaussian laser beam in vacuum. By means of a double perturbative expansion in paraxiality and quantum vacuum terms, we provide analytical expressions for the self-induced transverse mode mixing, rotation of polarization, and third harmonic generarion. We discuss the possibility of searching for the self-induced, spatially dependent phase shift of a multipetawatt laser pulse, which may allow the testing of quantum electrodynamics and new physics models, such as Born-Infeld theory and models involving new minicharged or axion-lik"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.3390","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":""},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1412.3390","created_at":"2026-05-18T01:41:20.052452+00:00"},{"alias_kind":"arxiv_version","alias_value":"1412.3390v1","created_at":"2026-05-18T01:41:20.052452+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.3390","created_at":"2026-05-18T01:41:20.052452+00:00"},{"alias_kind":"pith_short_12","alias_value":"5F7LK2B5MP4O","created_at":"2026-05-18T12:28:14.216126+00:00"},{"alias_kind":"pith_short_16","alias_value":"5F7LK2B5MP4OZXXW","created_at":"2026-05-18T12:28:14.216126+00:00"},{"alias_kind":"pith_short_8","alias_value":"5F7LK2B5","created_at":"2026-05-18T12:28:14.216126+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5F7LK2B5MP4OZXXW6T2L7QIXNL","json":"https://pith.science/pith/5F7LK2B5MP4OZXXW6T2L7QIXNL.json","graph_json":"https://pith.science/api/pith-number/5F7LK2B5MP4OZXXW6T2L7QIXNL/graph.json","events_json":"https://pith.science/api/pith-number/5F7LK2B5MP4OZXXW6T2L7QIXNL/events.json","paper":"https://pith.science/paper/5F7LK2B5"},"agent_actions":{"view_html":"https://pith.science/pith/5F7LK2B5MP4OZXXW6T2L7QIXNL","download_json":"https://pith.science/pith/5F7LK2B5MP4OZXXW6T2L7QIXNL.json","view_paper":"https://pith.science/paper/5F7LK2B5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1412.3390&json=true","fetch_graph":"https://pith.science/api/pith-number/5F7LK2B5MP4OZXXW6T2L7QIXNL/graph.json","fetch_events":"https://pith.science/api/pith-number/5F7LK2B5MP4OZXXW6T2L7QIXNL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5F7LK2B5MP4OZXXW6T2L7QIXNL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5F7LK2B5MP4OZXXW6T2L7QIXNL/action/storage_attestation","attest_author":"https://pith.science/pith/5F7LK2B5MP4OZXXW6T2L7QIXNL/action/author_attestation","sign_citation":"https://pith.science/pith/5F7LK2B5MP4OZXXW6T2L7QIXNL/action/citation_signature","submit_replication":"https://pith.science/pith/5F7LK2B5MP4OZXXW6T2L7QIXNL/action/replication_record"}},"created_at":"2026-05-18T01:41:20.052452+00:00","updated_at":"2026-05-18T01:41:20.052452+00:00"}