{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:TL57XVURNLJDLWCUNAK3S3JSOW","short_pith_number":"pith:TL57XVUR","schema_version":"1.0","canonical_sha256":"9afbfbd6916ad235d8546815b96d32758e37719394decf916f0a07b7348762a3","source":{"kind":"arxiv","id":"2007.07556","version":3},"attestation_state":"computed","paper":{"title":"Accurately simulating nine-dimensional phase space of relativistic particles in strong fields","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.plasm-ph"],"primary_cat":"physics.comp-ph","authors_text":"Adam Tableman, Fei Li, Frank S. Tsung, Kyle G. Miller, Marija Vranic, Ricardo A. Fonseca, Viktor K. Decyk, Warren B. Mori","submitted_at":"2020-07-15T09:12:31Z","abstract_excerpt":"Next-generation high-power lasers that can be focused to intensities exceeding 10^23 W/cm^2 are enabling new physics and applications. The physics of how these lasers interact with matter is highly nonlinear, relativistic, and can involve lowest-order quantum effects. The current tool of choice for modeling these interactions is the particle-in-cell (PIC) method. In strong fields, the motion of charged particles and their spin is affected by radiation reaction. Standard PIC codes usually use Boris or its variants to advance the particles, which requires very small time steps in the strong-fiel"},"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":"2007.07556","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2020-07-15T09:12:31Z","cross_cats_sorted":["physics.plasm-ph"],"title_canon_sha256":"5c3bda78c23b3b5fc5ad120eb4f3b123345d54f5eb46862dc325198ce2aed169","abstract_canon_sha256":"aafe42ea3cab15f34e37be1eee2b83d261d85ed3bd57357aaff7ed2dd855a6e5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:45:15.235829Z","signature_b64":"SYKuxnpqdoKRRlHdXZdes1bOnFwr/VpR9iH7uA6Rq8cjUGwqOXMz5mzucbLZ7b3+hL2i8mXNlS/HJoUJtVcBBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9afbfbd6916ad235d8546815b96d32758e37719394decf916f0a07b7348762a3","last_reissued_at":"2026-07-05T02:45:15.235345Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:45:15.235345Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Accurately simulating nine-dimensional phase space of relativistic particles in strong fields","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.plasm-ph"],"primary_cat":"physics.comp-ph","authors_text":"Adam Tableman, Fei Li, Frank S. Tsung, Kyle G. Miller, Marija Vranic, Ricardo A. Fonseca, Viktor K. Decyk, Warren B. Mori","submitted_at":"2020-07-15T09:12:31Z","abstract_excerpt":"Next-generation high-power lasers that can be focused to intensities exceeding 10^23 W/cm^2 are enabling new physics and applications. The physics of how these lasers interact with matter is highly nonlinear, relativistic, and can involve lowest-order quantum effects. The current tool of choice for modeling these interactions is the particle-in-cell (PIC) method. In strong fields, the motion of charged particles and their spin is affected by radiation reaction. Standard PIC codes usually use Boris or its variants to advance the particles, which requires very small time steps in the strong-fiel"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2007.07556","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2007.07556/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2007.07556","created_at":"2026-07-05T02:45:15.235398+00:00"},{"alias_kind":"arxiv_version","alias_value":"2007.07556v3","created_at":"2026-07-05T02:45:15.235398+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2007.07556","created_at":"2026-07-05T02:45:15.235398+00:00"},{"alias_kind":"pith_short_12","alias_value":"TL57XVURNLJD","created_at":"2026-07-05T02:45:15.235398+00:00"},{"alias_kind":"pith_short_16","alias_value":"TL57XVURNLJDLWCU","created_at":"2026-07-05T02:45:15.235398+00:00"},{"alias_kind":"pith_short_8","alias_value":"TL57XVUR","created_at":"2026-07-05T02:45:15.235398+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.11698","citing_title":"Interaction of Strong Electromagnetic Waves with Unmagnetized Pair Plasmas","ref_index":42,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TL57XVURNLJDLWCUNAK3S3JSOW","json":"https://pith.science/pith/TL57XVURNLJDLWCUNAK3S3JSOW.json","graph_json":"https://pith.science/api/pith-number/TL57XVURNLJDLWCUNAK3S3JSOW/graph.json","events_json":"https://pith.science/api/pith-number/TL57XVURNLJDLWCUNAK3S3JSOW/events.json","paper":"https://pith.science/paper/TL57XVUR"},"agent_actions":{"view_html":"https://pith.science/pith/TL57XVURNLJDLWCUNAK3S3JSOW","download_json":"https://pith.science/pith/TL57XVURNLJDLWCUNAK3S3JSOW.json","view_paper":"https://pith.science/paper/TL57XVUR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2007.07556&json=true","fetch_graph":"https://pith.science/api/pith-number/TL57XVURNLJDLWCUNAK3S3JSOW/graph.json","fetch_events":"https://pith.science/api/pith-number/TL57XVURNLJDLWCUNAK3S3JSOW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TL57XVURNLJDLWCUNAK3S3JSOW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TL57XVURNLJDLWCUNAK3S3JSOW/action/storage_attestation","attest_author":"https://pith.science/pith/TL57XVURNLJDLWCUNAK3S3JSOW/action/author_attestation","sign_citation":"https://pith.science/pith/TL57XVURNLJDLWCUNAK3S3JSOW/action/citation_signature","submit_replication":"https://pith.science/pith/TL57XVURNLJDLWCUNAK3S3JSOW/action/replication_record"}},"created_at":"2026-07-05T02:45:15.235398+00:00","updated_at":"2026-07-05T02:45:15.235398+00:00"}