{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:6X3HJ7GNYG43NHKNRRDIAVWFMB","short_pith_number":"pith:6X3HJ7GN","schema_version":"1.0","canonical_sha256":"f5f674fccdc1b9b69d4d8c468056c56043c9b54b4c8e0c1b7e52f54706410539","source":{"kind":"arxiv","id":"1511.07516","version":1},"attestation_state":"computed","paper":{"title":"Heavy ion acceleration in the Breakout Afterburner regime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"A. G. R. Thomas, C. McGuffey, F. N. Beg, G. M. Petrov, K. Krushelnick","submitted_at":"2015-11-24T00:16:06Z","abstract_excerpt":"Theoretical study of heavy ion acceleration from an ultrathin (20 nm) gold foil irradiated by sub-picosecond lasers is presented. Using two dimensional particle-in-cell simulations we identified two highly efficient ion acceleration schemes. By varying the laser pulse duration we observed a transition from Radiation Pressure Acceleration to the Breakout Afterburner regime akin to light ions. The underlying physics and ion acceleration regimes are similar to that of light ions, however, nuances of the acceleration process make the acceleration of heavy ions more challenging. Two laser systems a"},"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":"1511.07516","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2015-11-24T00:16:06Z","cross_cats_sorted":[],"title_canon_sha256":"a0f0c6f042c156323b5dac253bd082681e22d95968f9a6e5b152830b01fee73f","abstract_canon_sha256":"5425d8bb193fa9c8092e4018724fec48f4db0ed094fa5dbdffbbaf09b48c8522"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:26:04.593628Z","signature_b64":"a0totX/VTPSm7OSSKzjFKg31E5hrpAmKR9mYqSIivrCWoSi67uwQ3Z7i4EHCbaCOjikcT+8kw2+I384PJsl3AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f5f674fccdc1b9b69d4d8c468056c56043c9b54b4c8e0c1b7e52f54706410539","last_reissued_at":"2026-05-18T01:26:04.593099Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:26:04.593099Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Heavy ion acceleration in the Breakout Afterburner regime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"A. G. R. Thomas, C. McGuffey, F. N. Beg, G. M. Petrov, K. Krushelnick","submitted_at":"2015-11-24T00:16:06Z","abstract_excerpt":"Theoretical study of heavy ion acceleration from an ultrathin (20 nm) gold foil irradiated by sub-picosecond lasers is presented. Using two dimensional particle-in-cell simulations we identified two highly efficient ion acceleration schemes. By varying the laser pulse duration we observed a transition from Radiation Pressure Acceleration to the Breakout Afterburner regime akin to light ions. The underlying physics and ion acceleration regimes are similar to that of light ions, however, nuances of the acceleration process make the acceleration of heavy ions more challenging. Two laser systems a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.07516","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":"1511.07516","created_at":"2026-05-18T01:26:04.593189+00:00"},{"alias_kind":"arxiv_version","alias_value":"1511.07516v1","created_at":"2026-05-18T01:26:04.593189+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.07516","created_at":"2026-05-18T01:26:04.593189+00:00"},{"alias_kind":"pith_short_12","alias_value":"6X3HJ7GNYG43","created_at":"2026-05-18T12:29:07.941421+00:00"},{"alias_kind":"pith_short_16","alias_value":"6X3HJ7GNYG43NHKN","created_at":"2026-05-18T12:29:07.941421+00:00"},{"alias_kind":"pith_short_8","alias_value":"6X3HJ7GN","created_at":"2026-05-18T12:29:07.941421+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/6X3HJ7GNYG43NHKNRRDIAVWFMB","json":"https://pith.science/pith/6X3HJ7GNYG43NHKNRRDIAVWFMB.json","graph_json":"https://pith.science/api/pith-number/6X3HJ7GNYG43NHKNRRDIAVWFMB/graph.json","events_json":"https://pith.science/api/pith-number/6X3HJ7GNYG43NHKNRRDIAVWFMB/events.json","paper":"https://pith.science/paper/6X3HJ7GN"},"agent_actions":{"view_html":"https://pith.science/pith/6X3HJ7GNYG43NHKNRRDIAVWFMB","download_json":"https://pith.science/pith/6X3HJ7GNYG43NHKNRRDIAVWFMB.json","view_paper":"https://pith.science/paper/6X3HJ7GN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1511.07516&json=true","fetch_graph":"https://pith.science/api/pith-number/6X3HJ7GNYG43NHKNRRDIAVWFMB/graph.json","fetch_events":"https://pith.science/api/pith-number/6X3HJ7GNYG43NHKNRRDIAVWFMB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6X3HJ7GNYG43NHKNRRDIAVWFMB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6X3HJ7GNYG43NHKNRRDIAVWFMB/action/storage_attestation","attest_author":"https://pith.science/pith/6X3HJ7GNYG43NHKNRRDIAVWFMB/action/author_attestation","sign_citation":"https://pith.science/pith/6X3HJ7GNYG43NHKNRRDIAVWFMB/action/citation_signature","submit_replication":"https://pith.science/pith/6X3HJ7GNYG43NHKNRRDIAVWFMB/action/replication_record"}},"created_at":"2026-05-18T01:26:04.593189+00:00","updated_at":"2026-05-18T01:26:04.593189+00:00"}