{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:7YG52EJAOSQU4RNXTYNZHW4KB2","short_pith_number":"pith:7YG52EJA","schema_version":"1.0","canonical_sha256":"fe0ddd112074a14e45b79e1b93db8a0e850abe85af9f12deeb516419881ec1c9","source":{"kind":"arxiv","id":"2411.17302","version":2},"attestation_state":"computed","paper":{"title":"All-optical compact setup for generation of collimated multi-MeV proton beams with a \"snail\" target","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.acc-ph","physics.app-ph"],"primary_cat":"physics.plasm-ph","authors_text":"N. Bukharskii, Ph. Korneev","submitted_at":"2024-11-26T10:50:31Z","abstract_excerpt":"The work considers an optical scheme for collimation of high-energy proton beams using $\\sim 10^5$~T scale magnetic fields induced in a miniature \"snail\" target by petawatt or multi-petawatt laser irradiation in ps or fs regime. Such magnetic fields are known to be frozen into hot plasma and exist on at least a hundred of picoseconds time-scale, allowing their use for control of charged particle beams. The high values of the magnetic field along with the compact size perfectly match conditions for an all-in-one optical setup, where first, the laser beam accelerates protons, by, e.g. Target Nor"},"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":"2411.17302","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2024-11-26T10:50:31Z","cross_cats_sorted":["physics.acc-ph","physics.app-ph"],"title_canon_sha256":"1e547859d7494b1b255f16529ab9de2b766344c77dfc1c90f1b5adc1cd9f0c80","abstract_canon_sha256":"f1871089ff43ca3900e54b838e0db26ea59adeac3e5d042b398a3a3ad293689a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:05:14.892457Z","signature_b64":"uXVzSFKZTBY8H8bX9eTI7OZpE5eJBcjFVfjVnU383zE2q5SNaI4uZ33xLQxjhhIEvp6lvNqstwFxcia0xSd8Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fe0ddd112074a14e45b79e1b93db8a0e850abe85af9f12deeb516419881ec1c9","last_reissued_at":"2026-07-05T10:05:14.891954Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:05:14.891954Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"All-optical compact setup for generation of collimated multi-MeV proton beams with a \"snail\" target","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.acc-ph","physics.app-ph"],"primary_cat":"physics.plasm-ph","authors_text":"N. Bukharskii, Ph. Korneev","submitted_at":"2024-11-26T10:50:31Z","abstract_excerpt":"The work considers an optical scheme for collimation of high-energy proton beams using $\\sim 10^5$~T scale magnetic fields induced in a miniature \"snail\" target by petawatt or multi-petawatt laser irradiation in ps or fs regime. Such magnetic fields are known to be frozen into hot plasma and exist on at least a hundred of picoseconds time-scale, allowing their use for control of charged particle beams. The high values of the magnetic field along with the compact size perfectly match conditions for an all-in-one optical setup, where first, the laser beam accelerates protons, by, e.g. Target Nor"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.17302","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/2411.17302/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":"2411.17302","created_at":"2026-07-05T10:05:14.892016+00:00"},{"alias_kind":"arxiv_version","alias_value":"2411.17302v2","created_at":"2026-07-05T10:05:14.892016+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.17302","created_at":"2026-07-05T10:05:14.892016+00:00"},{"alias_kind":"pith_short_12","alias_value":"7YG52EJAOSQU","created_at":"2026-07-05T10:05:14.892016+00:00"},{"alias_kind":"pith_short_16","alias_value":"7YG52EJAOSQU4RNX","created_at":"2026-07-05T10:05:14.892016+00:00"},{"alias_kind":"pith_short_8","alias_value":"7YG52EJA","created_at":"2026-07-05T10:05:14.892016+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/7YG52EJAOSQU4RNXTYNZHW4KB2","json":"https://pith.science/pith/7YG52EJAOSQU4RNXTYNZHW4KB2.json","graph_json":"https://pith.science/api/pith-number/7YG52EJAOSQU4RNXTYNZHW4KB2/graph.json","events_json":"https://pith.science/api/pith-number/7YG52EJAOSQU4RNXTYNZHW4KB2/events.json","paper":"https://pith.science/paper/7YG52EJA"},"agent_actions":{"view_html":"https://pith.science/pith/7YG52EJAOSQU4RNXTYNZHW4KB2","download_json":"https://pith.science/pith/7YG52EJAOSQU4RNXTYNZHW4KB2.json","view_paper":"https://pith.science/paper/7YG52EJA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2411.17302&json=true","fetch_graph":"https://pith.science/api/pith-number/7YG52EJAOSQU4RNXTYNZHW4KB2/graph.json","fetch_events":"https://pith.science/api/pith-number/7YG52EJAOSQU4RNXTYNZHW4KB2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7YG52EJAOSQU4RNXTYNZHW4KB2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7YG52EJAOSQU4RNXTYNZHW4KB2/action/storage_attestation","attest_author":"https://pith.science/pith/7YG52EJAOSQU4RNXTYNZHW4KB2/action/author_attestation","sign_citation":"https://pith.science/pith/7YG52EJAOSQU4RNXTYNZHW4KB2/action/citation_signature","submit_replication":"https://pith.science/pith/7YG52EJAOSQU4RNXTYNZHW4KB2/action/replication_record"}},"created_at":"2026-07-05T10:05:14.892016+00:00","updated_at":"2026-07-05T10:05:14.892016+00:00"}