{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:KXEFLZDGSSW2ONIBU7V7X3UTPY","short_pith_number":"pith:KXEFLZDG","schema_version":"1.0","canonical_sha256":"55c855e46694ada73501a7ebfbee937e0f3e586df8f527a6474c07a24425ca6d","source":{"kind":"arxiv","id":"2201.01570","version":1},"attestation_state":"computed","paper":{"title":"The Flexible Plasma Trap (FPT) for the production of overdense plasmas","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.acc-ph","authors_text":"D. Mascali, F. Chines, G. Calabrese, G. Castro, G. Gallo, G. Sorbello, G. Torrisi, L. Allegra, L. Celona, L. Neri, M. Mazzaglia, O. Leonardi, S. Gammino, S. Passerello","submitted_at":"2022-01-05T12:21:35Z","abstract_excerpt":"Electron Cyclotron Resonance Ion Sources are currently the most efficient ion sources among those used in facilities dedicated to nuclear physics. The need for a more flexible magnetic field and RF injection system suggested to design and develop a different type of plasma trap, named Flexible Plasma Trap (FPT). The magnetic field of FPT is generated by means of three coils while microwaves in the range 4-7 GHz can be injected by three different inputs, one placed along the axis and two placed radially. FPT can work in different plasma heating schemes so it will be an ideal tool for studies of"},"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":"2201.01570","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.acc-ph","submitted_at":"2022-01-05T12:21:35Z","cross_cats_sorted":[],"title_canon_sha256":"831503bd56452973a31e365d8e9fc8cd3de7e4c7ad5b1409704a3a30cd126f8e","abstract_canon_sha256":"939099fc20d7b7abadcd4f30918c697a58beeb360a3e084e9a86e206e0bd3500"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:46:06.962442Z","signature_b64":"JEyrPoRgubI5tf3eZfqe2ShdAEQ5/26EZvzsN6KIhC4l7S6AI78vutBRcAjKkjcQxHIyKqz9FQ21Qg7arhE6Dw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"55c855e46694ada73501a7ebfbee937e0f3e586df8f527a6474c07a24425ca6d","last_reissued_at":"2026-07-05T03:46:06.961985Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:46:06.961985Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Flexible Plasma Trap (FPT) for the production of overdense plasmas","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.acc-ph","authors_text":"D. Mascali, F. Chines, G. Calabrese, G. Castro, G. Gallo, G. Sorbello, G. Torrisi, L. Allegra, L. Celona, L. Neri, M. Mazzaglia, O. Leonardi, S. Gammino, S. Passerello","submitted_at":"2022-01-05T12:21:35Z","abstract_excerpt":"Electron Cyclotron Resonance Ion Sources are currently the most efficient ion sources among those used in facilities dedicated to nuclear physics. The need for a more flexible magnetic field and RF injection system suggested to design and develop a different type of plasma trap, named Flexible Plasma Trap (FPT). The magnetic field of FPT is generated by means of three coils while microwaves in the range 4-7 GHz can be injected by three different inputs, one placed along the axis and two placed radially. FPT can work in different plasma heating schemes so it will be an ideal tool for studies of"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2201.01570","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2201.01570/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":"2201.01570","created_at":"2026-07-05T03:46:06.962041+00:00"},{"alias_kind":"arxiv_version","alias_value":"2201.01570v1","created_at":"2026-07-05T03:46:06.962041+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2201.01570","created_at":"2026-07-05T03:46:06.962041+00:00"},{"alias_kind":"pith_short_12","alias_value":"KXEFLZDGSSW2","created_at":"2026-07-05T03:46:06.962041+00:00"},{"alias_kind":"pith_short_16","alias_value":"KXEFLZDGSSW2ONIB","created_at":"2026-07-05T03:46:06.962041+00:00"},{"alias_kind":"pith_short_8","alias_value":"KXEFLZDG","created_at":"2026-07-05T03:46:06.962041+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/KXEFLZDGSSW2ONIBU7V7X3UTPY","json":"https://pith.science/pith/KXEFLZDGSSW2ONIBU7V7X3UTPY.json","graph_json":"https://pith.science/api/pith-number/KXEFLZDGSSW2ONIBU7V7X3UTPY/graph.json","events_json":"https://pith.science/api/pith-number/KXEFLZDGSSW2ONIBU7V7X3UTPY/events.json","paper":"https://pith.science/paper/KXEFLZDG"},"agent_actions":{"view_html":"https://pith.science/pith/KXEFLZDGSSW2ONIBU7V7X3UTPY","download_json":"https://pith.science/pith/KXEFLZDGSSW2ONIBU7V7X3UTPY.json","view_paper":"https://pith.science/paper/KXEFLZDG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2201.01570&json=true","fetch_graph":"https://pith.science/api/pith-number/KXEFLZDGSSW2ONIBU7V7X3UTPY/graph.json","fetch_events":"https://pith.science/api/pith-number/KXEFLZDGSSW2ONIBU7V7X3UTPY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KXEFLZDGSSW2ONIBU7V7X3UTPY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KXEFLZDGSSW2ONIBU7V7X3UTPY/action/storage_attestation","attest_author":"https://pith.science/pith/KXEFLZDGSSW2ONIBU7V7X3UTPY/action/author_attestation","sign_citation":"https://pith.science/pith/KXEFLZDGSSW2ONIBU7V7X3UTPY/action/citation_signature","submit_replication":"https://pith.science/pith/KXEFLZDGSSW2ONIBU7V7X3UTPY/action/replication_record"}},"created_at":"2026-07-05T03:46:06.962041+00:00","updated_at":"2026-07-05T03:46:06.962041+00:00"}