{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:2NBC22VJ7F4R7PKJFFM2GOAQEE","short_pith_number":"pith:2NBC22VJ","schema_version":"1.0","canonical_sha256":"d3422d6aa9f9791fbd492959a33810212f9bb2ce2fa10fd168c9bc13900fa28b","source":{"kind":"arxiv","id":"1205.3154","version":1},"attestation_state":"computed","paper":{"title":"Influence of Laser Pulse Parameters on the Properties of e-e+ Plasmas Created from Vacuum","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","physics.optics"],"primary_cat":"physics.plasm-ph","authors_text":"A. D. Panferov, A. V. Prozorkevich, B. Kaempfer, D. B. Blaschke, S. A. Smolyansky","submitted_at":"2012-05-14T19:57:47Z","abstract_excerpt":"We use the low density approximation within the kinetic theory approach to vacuum creation of an e-e+ pair plasma (EPPP) in a strong laser field in order to investigate the dependence of the observed EPPP on the form and parameters of a single laser pulse. The EPPP distribution function is calculated for an arbitrary time dependence of the electric field in the multiphoton domain (adiabaticity parameter gamma >> 1). The dependence on the field strength, the form and spectrum of the field pulse is investigated on the basis both analytical and numerical methods. The obtained results can be usefu"},"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":"1205.3154","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2012-05-14T19:57:47Z","cross_cats_sorted":["hep-ph","physics.optics"],"title_canon_sha256":"33284a2886e7b9bf25f34129b3da130dd2aa46cad0e35982e80341222842b44c","abstract_canon_sha256":"0aaaac03219d27bccedd51d9a78118236cd310d7559b0dd4315bd64a38816214"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:34:38.246183Z","signature_b64":"e66ZlF+Qi6uqpkYZDCJmaFAu7vdwBWBWDFGT8T04u7pGl+ZYEr9yqOF0WqjJKIsFwlYA19HAFx68T97igFUDDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d3422d6aa9f9791fbd492959a33810212f9bb2ce2fa10fd168c9bc13900fa28b","last_reissued_at":"2026-05-18T03:34:38.245655Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:34:38.245655Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Influence of Laser Pulse Parameters on the Properties of e-e+ Plasmas Created from Vacuum","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","physics.optics"],"primary_cat":"physics.plasm-ph","authors_text":"A. D. Panferov, A. V. Prozorkevich, B. Kaempfer, D. B. Blaschke, S. A. Smolyansky","submitted_at":"2012-05-14T19:57:47Z","abstract_excerpt":"We use the low density approximation within the kinetic theory approach to vacuum creation of an e-e+ pair plasma (EPPP) in a strong laser field in order to investigate the dependence of the observed EPPP on the form and parameters of a single laser pulse. The EPPP distribution function is calculated for an arbitrary time dependence of the electric field in the multiphoton domain (adiabaticity parameter gamma >> 1). The dependence on the field strength, the form and spectrum of the field pulse is investigated on the basis both analytical and numerical methods. The obtained results can be usefu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1205.3154","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":"1205.3154","created_at":"2026-05-18T03:34:38.245730+00:00"},{"alias_kind":"arxiv_version","alias_value":"1205.3154v1","created_at":"2026-05-18T03:34:38.245730+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1205.3154","created_at":"2026-05-18T03:34:38.245730+00:00"},{"alias_kind":"pith_short_12","alias_value":"2NBC22VJ7F4R","created_at":"2026-05-18T12:26:50.516681+00:00"},{"alias_kind":"pith_short_16","alias_value":"2NBC22VJ7F4R7PKJ","created_at":"2026-05-18T12:26:50.516681+00:00"},{"alias_kind":"pith_short_8","alias_value":"2NBC22VJ","created_at":"2026-05-18T12:26:50.516681+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/2NBC22VJ7F4R7PKJFFM2GOAQEE","json":"https://pith.science/pith/2NBC22VJ7F4R7PKJFFM2GOAQEE.json","graph_json":"https://pith.science/api/pith-number/2NBC22VJ7F4R7PKJFFM2GOAQEE/graph.json","events_json":"https://pith.science/api/pith-number/2NBC22VJ7F4R7PKJFFM2GOAQEE/events.json","paper":"https://pith.science/paper/2NBC22VJ"},"agent_actions":{"view_html":"https://pith.science/pith/2NBC22VJ7F4R7PKJFFM2GOAQEE","download_json":"https://pith.science/pith/2NBC22VJ7F4R7PKJFFM2GOAQEE.json","view_paper":"https://pith.science/paper/2NBC22VJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1205.3154&json=true","fetch_graph":"https://pith.science/api/pith-number/2NBC22VJ7F4R7PKJFFM2GOAQEE/graph.json","fetch_events":"https://pith.science/api/pith-number/2NBC22VJ7F4R7PKJFFM2GOAQEE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2NBC22VJ7F4R7PKJFFM2GOAQEE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2NBC22VJ7F4R7PKJFFM2GOAQEE/action/storage_attestation","attest_author":"https://pith.science/pith/2NBC22VJ7F4R7PKJFFM2GOAQEE/action/author_attestation","sign_citation":"https://pith.science/pith/2NBC22VJ7F4R7PKJFFM2GOAQEE/action/citation_signature","submit_replication":"https://pith.science/pith/2NBC22VJ7F4R7PKJFFM2GOAQEE/action/replication_record"}},"created_at":"2026-05-18T03:34:38.245730+00:00","updated_at":"2026-05-18T03:34:38.245730+00:00"}