{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:T5VHIGU2HPN2T5DXICQXZRGV7N","short_pith_number":"pith:T5VHIGU2","schema_version":"1.0","canonical_sha256":"9f6a741a9a3bdba9f47740a17cc4d5fb6260d9d44a565c9f2ffc0802d0dcc18c","source":{"kind":"arxiv","id":"1505.05685","version":3},"attestation_state":"computed","paper":{"title":"Pulse shape dependence in the dynamically assisted Sauter-Schwinger effect","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Christian Schneider, Joachim Sicking, Malte F. Linder, Nikodem Szpak, Ralf Sch\\\"utzhold","submitted_at":"2015-05-21T11:57:29Z","abstract_excerpt":"While the Sauter-Schwinger effect describes nonperturbative electron-positron pair creation from vacuum by a strong and slowly varying electric field $E_{\\mathrm{strong}}$ via tunneling, the dynamically assisted Sauter-Schwinger effect corresponds to a strong (exponential) enhancement of the pair-creation probability by an additional weak and fast electric or electromagnetic pulse $E_{\\mathrm{weak}}$. Using the WKB and worldline instanton method, we find that this enhancement mechanism strongly depends on the shape of the fast pulse. For the Sauter profile $1/\\cosh^2(\\omega t)$ considered prev"},"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":"1505.05685","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-05-21T11:57:29Z","cross_cats_sorted":[],"title_canon_sha256":"79471c95dd43380c0269d0ca6cb642a5a4136f3002e95491c69ea4399023032e","abstract_canon_sha256":"ec178c7b36ad02a369aa3f747f2bd5c85c7ee8d846ba194241d5de40b944dc75"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:30:34.577144Z","signature_b64":"3sSCROdklHkOf2sXA6zhfr3/t9+gjzN+6gaCcNk/V+skHro1T3BQ1aR6ieINNMijCf1LkNdx5xJkgWAYCdelDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9f6a741a9a3bdba9f47740a17cc4d5fb6260d9d44a565c9f2ffc0802d0dcc18c","last_reissued_at":"2026-05-18T01:30:34.576469Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:30:34.576469Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Pulse shape dependence in the dynamically assisted Sauter-Schwinger effect","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Christian Schneider, Joachim Sicking, Malte F. Linder, Nikodem Szpak, Ralf Sch\\\"utzhold","submitted_at":"2015-05-21T11:57:29Z","abstract_excerpt":"While the Sauter-Schwinger effect describes nonperturbative electron-positron pair creation from vacuum by a strong and slowly varying electric field $E_{\\mathrm{strong}}$ via tunneling, the dynamically assisted Sauter-Schwinger effect corresponds to a strong (exponential) enhancement of the pair-creation probability by an additional weak and fast electric or electromagnetic pulse $E_{\\mathrm{weak}}$. Using the WKB and worldline instanton method, we find that this enhancement mechanism strongly depends on the shape of the fast pulse. For the Sauter profile $1/\\cosh^2(\\omega t)$ considered prev"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1505.05685","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1505.05685","created_at":"2026-05-18T01:30:34.576573+00:00"},{"alias_kind":"arxiv_version","alias_value":"1505.05685v3","created_at":"2026-05-18T01:30:34.576573+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1505.05685","created_at":"2026-05-18T01:30:34.576573+00:00"},{"alias_kind":"pith_short_12","alias_value":"T5VHIGU2HPN2","created_at":"2026-05-18T12:29:42.218222+00:00"},{"alias_kind":"pith_short_16","alias_value":"T5VHIGU2HPN2T5DX","created_at":"2026-05-18T12:29:42.218222+00:00"},{"alias_kind":"pith_short_8","alias_value":"T5VHIGU2","created_at":"2026-05-18T12:29:42.218222+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/T5VHIGU2HPN2T5DXICQXZRGV7N","json":"https://pith.science/pith/T5VHIGU2HPN2T5DXICQXZRGV7N.json","graph_json":"https://pith.science/api/pith-number/T5VHIGU2HPN2T5DXICQXZRGV7N/graph.json","events_json":"https://pith.science/api/pith-number/T5VHIGU2HPN2T5DXICQXZRGV7N/events.json","paper":"https://pith.science/paper/T5VHIGU2"},"agent_actions":{"view_html":"https://pith.science/pith/T5VHIGU2HPN2T5DXICQXZRGV7N","download_json":"https://pith.science/pith/T5VHIGU2HPN2T5DXICQXZRGV7N.json","view_paper":"https://pith.science/paper/T5VHIGU2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1505.05685&json=true","fetch_graph":"https://pith.science/api/pith-number/T5VHIGU2HPN2T5DXICQXZRGV7N/graph.json","fetch_events":"https://pith.science/api/pith-number/T5VHIGU2HPN2T5DXICQXZRGV7N/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/T5VHIGU2HPN2T5DXICQXZRGV7N/action/timestamp_anchor","attest_storage":"https://pith.science/pith/T5VHIGU2HPN2T5DXICQXZRGV7N/action/storage_attestation","attest_author":"https://pith.science/pith/T5VHIGU2HPN2T5DXICQXZRGV7N/action/author_attestation","sign_citation":"https://pith.science/pith/T5VHIGU2HPN2T5DXICQXZRGV7N/action/citation_signature","submit_replication":"https://pith.science/pith/T5VHIGU2HPN2T5DXICQXZRGV7N/action/replication_record"}},"created_at":"2026-05-18T01:30:34.576573+00:00","updated_at":"2026-05-18T01:30:34.576573+00:00"}