{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:ZKZWS3X6IPTABWHMTIGOERHNHU","short_pith_number":"pith:ZKZWS3X6","schema_version":"1.0","canonical_sha256":"cab3696efe43e600d8ec9a0ce244ed3d3569e3f00665caef70eee5f4d1ac4f24","source":{"kind":"arxiv","id":"1611.06616","version":1},"attestation_state":"computed","paper":{"title":"Collisionless electrostatic shock formation and ion acceleration in intense laser interactions with near critical density plasmas","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.HE","physics.acc-ph"],"primary_cat":"physics.plasm-ph","authors_text":"D. W. Yuan, J. Zhang, L. L. Yu, M. Chen, M. Liu, M. Murakami, P. Mulser, S. M. Weng, X. L. Zheng, Y. T. Li, Z. M. Sheng","submitted_at":"2016-11-21T00:22:45Z","abstract_excerpt":"Laser-driven collisonless electrostatic shock formation and the subsequent ion acceleration have been studied in near critical density plasmas. Particle-in-cell simulations show that both the speed of laser-driven collisionless electrostatic shock and the energies of shock-accelerated ions can be greatly enhanced due to fast laser propagation in near critical density plasmas. However, a response time longer than tens of laser wave cycles is required before the shock formation in a near critical density plasma, in contrast to the quick shock formation in a highly overdense target. More importan"},"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":"1611.06616","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2016-11-21T00:22:45Z","cross_cats_sorted":["astro-ph.HE","physics.acc-ph"],"title_canon_sha256":"92727fdcecb525c74312b8aead0bdca8b85feea69712ca0fd94d3d27214c3d88","abstract_canon_sha256":"4d635150a41e87e5b0b1481cde820104a82b8cc79faa022c295946cf4b063e02"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:57:36.289008Z","signature_b64":"jqUIcAsT2DkJbHhddCgiLkCu6GYaxkjksDGiOs/6cA2qPNjFN5Blm6QNF/fOJAUqAEoDL7HHdUX4WR7S2H3lDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cab3696efe43e600d8ec9a0ce244ed3d3569e3f00665caef70eee5f4d1ac4f24","last_reissued_at":"2026-05-18T00:57:36.288187Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:57:36.288187Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Collisionless electrostatic shock formation and ion acceleration in intense laser interactions with near critical density plasmas","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.HE","physics.acc-ph"],"primary_cat":"physics.plasm-ph","authors_text":"D. W. Yuan, J. Zhang, L. L. Yu, M. Chen, M. Liu, M. Murakami, P. Mulser, S. M. Weng, X. L. Zheng, Y. T. Li, Z. M. Sheng","submitted_at":"2016-11-21T00:22:45Z","abstract_excerpt":"Laser-driven collisonless electrostatic shock formation and the subsequent ion acceleration have been studied in near critical density plasmas. Particle-in-cell simulations show that both the speed of laser-driven collisionless electrostatic shock and the energies of shock-accelerated ions can be greatly enhanced due to fast laser propagation in near critical density plasmas. However, a response time longer than tens of laser wave cycles is required before the shock formation in a near critical density plasma, in contrast to the quick shock formation in a highly overdense target. More importan"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.06616","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":"1611.06616","created_at":"2026-05-18T00:57:36.288377+00:00"},{"alias_kind":"arxiv_version","alias_value":"1611.06616v1","created_at":"2026-05-18T00:57:36.288377+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.06616","created_at":"2026-05-18T00:57:36.288377+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZKZWS3X6IPTA","created_at":"2026-05-18T12:30:53.716459+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZKZWS3X6IPTABWHM","created_at":"2026-05-18T12:30:53.716459+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZKZWS3X6","created_at":"2026-05-18T12:30:53.716459+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/ZKZWS3X6IPTABWHMTIGOERHNHU","json":"https://pith.science/pith/ZKZWS3X6IPTABWHMTIGOERHNHU.json","graph_json":"https://pith.science/api/pith-number/ZKZWS3X6IPTABWHMTIGOERHNHU/graph.json","events_json":"https://pith.science/api/pith-number/ZKZWS3X6IPTABWHMTIGOERHNHU/events.json","paper":"https://pith.science/paper/ZKZWS3X6"},"agent_actions":{"view_html":"https://pith.science/pith/ZKZWS3X6IPTABWHMTIGOERHNHU","download_json":"https://pith.science/pith/ZKZWS3X6IPTABWHMTIGOERHNHU.json","view_paper":"https://pith.science/paper/ZKZWS3X6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1611.06616&json=true","fetch_graph":"https://pith.science/api/pith-number/ZKZWS3X6IPTABWHMTIGOERHNHU/graph.json","fetch_events":"https://pith.science/api/pith-number/ZKZWS3X6IPTABWHMTIGOERHNHU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZKZWS3X6IPTABWHMTIGOERHNHU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZKZWS3X6IPTABWHMTIGOERHNHU/action/storage_attestation","attest_author":"https://pith.science/pith/ZKZWS3X6IPTABWHMTIGOERHNHU/action/author_attestation","sign_citation":"https://pith.science/pith/ZKZWS3X6IPTABWHMTIGOERHNHU/action/citation_signature","submit_replication":"https://pith.science/pith/ZKZWS3X6IPTABWHMTIGOERHNHU/action/replication_record"}},"created_at":"2026-05-18T00:57:36.288377+00:00","updated_at":"2026-05-18T00:57:36.288377+00:00"}