{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:II4AIUJAPWGSKVQNUV75HFA7DE","short_pith_number":"pith:II4AIUJA","schema_version":"1.0","canonical_sha256":"42380451207d8d25560da57fd3941f193fbc08065f12ec43d61b97c2a0663ea2","source":{"kind":"arxiv","id":"1912.09035","version":2},"attestation_state":"computed","paper":{"title":"Modeling and simulation of transverse wakefields in PWFA","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.acc-ph","authors_text":"Daniel Schulte, Erik Adli, Jian Bin Ben Chen","submitted_at":"2019-12-19T06:51:12Z","abstract_excerpt":"A simplified model describing the PWFA (plasma wakefield acceleration) transverse instability in the form of a wake function parameterized only with an effective cavity aperture radius $a$ is benchmarked against PIC-simulations. This wake function implies a $1/a^4$ scaling of the transverse wakefields, which indicates transverse intra-beam wakefields typically several orders of magnitude higher than in conventional acceleration structures. Furthermore, the wakefield formalism is utilized to perform a parameter study for a \\SI{1.5}{\\tera\\electronvolt} plasma wakefield accelerator, where the con"},"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":"1912.09035","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.acc-ph","submitted_at":"2019-12-19T06:51:12Z","cross_cats_sorted":[],"title_canon_sha256":"43c9c7d0f3c4e7ee25efc3a81596d24197a284f1f11c78ac7efa03ca5b3f3f94","abstract_canon_sha256":"5d5ee0a22df37c211a04171d29aa21894138fadb6ec4368ab69f036f13b5ad61"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:37:33.805500Z","signature_b64":"Hm/z+t3KfL7e7RUi0gtOn/mdVMYaPSvYo0zsg2fsix9GAjseblcwD6Ji5DjSa3X0nOzzaQVKvfx5vaueh7e5AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"42380451207d8d25560da57fd3941f193fbc08065f12ec43d61b97c2a0663ea2","last_reissued_at":"2026-07-05T01:37:33.805046Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:37:33.805046Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Modeling and simulation of transverse wakefields in PWFA","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.acc-ph","authors_text":"Daniel Schulte, Erik Adli, Jian Bin Ben Chen","submitted_at":"2019-12-19T06:51:12Z","abstract_excerpt":"A simplified model describing the PWFA (plasma wakefield acceleration) transverse instability in the form of a wake function parameterized only with an effective cavity aperture radius $a$ is benchmarked against PIC-simulations. This wake function implies a $1/a^4$ scaling of the transverse wakefields, which indicates transverse intra-beam wakefields typically several orders of magnitude higher than in conventional acceleration structures. Furthermore, the wakefield formalism is utilized to perform a parameter study for a \\SI{1.5}{\\tera\\electronvolt} plasma wakefield accelerator, where the con"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1912.09035","kind":"arxiv","version":2},"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/1912.09035/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":"1912.09035","created_at":"2026-07-05T01:37:33.805094+00:00"},{"alias_kind":"arxiv_version","alias_value":"1912.09035v2","created_at":"2026-07-05T01:37:33.805094+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1912.09035","created_at":"2026-07-05T01:37:33.805094+00:00"},{"alias_kind":"pith_short_12","alias_value":"II4AIUJAPWGS","created_at":"2026-07-05T01:37:33.805094+00:00"},{"alias_kind":"pith_short_16","alias_value":"II4AIUJAPWGSKVQN","created_at":"2026-07-05T01:37:33.805094+00:00"},{"alias_kind":"pith_short_8","alias_value":"II4AIUJA","created_at":"2026-07-05T01:37:33.805094+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/II4AIUJAPWGSKVQNUV75HFA7DE","json":"https://pith.science/pith/II4AIUJAPWGSKVQNUV75HFA7DE.json","graph_json":"https://pith.science/api/pith-number/II4AIUJAPWGSKVQNUV75HFA7DE/graph.json","events_json":"https://pith.science/api/pith-number/II4AIUJAPWGSKVQNUV75HFA7DE/events.json","paper":"https://pith.science/paper/II4AIUJA"},"agent_actions":{"view_html":"https://pith.science/pith/II4AIUJAPWGSKVQNUV75HFA7DE","download_json":"https://pith.science/pith/II4AIUJAPWGSKVQNUV75HFA7DE.json","view_paper":"https://pith.science/paper/II4AIUJA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1912.09035&json=true","fetch_graph":"https://pith.science/api/pith-number/II4AIUJAPWGSKVQNUV75HFA7DE/graph.json","fetch_events":"https://pith.science/api/pith-number/II4AIUJAPWGSKVQNUV75HFA7DE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/II4AIUJAPWGSKVQNUV75HFA7DE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/II4AIUJAPWGSKVQNUV75HFA7DE/action/storage_attestation","attest_author":"https://pith.science/pith/II4AIUJAPWGSKVQNUV75HFA7DE/action/author_attestation","sign_citation":"https://pith.science/pith/II4AIUJAPWGSKVQNUV75HFA7DE/action/citation_signature","submit_replication":"https://pith.science/pith/II4AIUJAPWGSKVQNUV75HFA7DE/action/replication_record"}},"created_at":"2026-07-05T01:37:33.805094+00:00","updated_at":"2026-07-05T01:37:33.805094+00:00"}