{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:DX43KXSX27GTIFJVEORWS7EH7F","short_pith_number":"pith:DX43KXSX","schema_version":"1.0","canonical_sha256":"1df9b55e57d7cd34153523a3697c87f946a9ff57182eb179ecd57d932856855f","source":{"kind":"arxiv","id":"1509.08629","version":1},"attestation_state":"computed","paper":{"title":"Stable and polarized Betatron x-ray radiation from a laser plasma accelerator in ionization injection regime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"Agustin Lifschitz, Amar Tafzi, Andreas Doepp, Antoine Doche, Antoine Rousse, Benoit Mahieu, Cedric Thaury, Emilien Guillaume, Gabriele Grittani, Jean Philippe Goddet, Julien Gautier, Kim Ta Phuoc, Martin Hansson, Michaela Kozlova, Olle Lund, Pascal Rousseau, Sebastien Corde, Victor Malka","submitted_at":"2015-09-29T08:18:05Z","abstract_excerpt":"Betatron x-ray source from laser plasma interaction combines high brightness, few femtosecond duration and broad band energy spectrum. However, despite these unique features the Betatron source has a crippling drawback preventing its use for applications. Its properties significantly vary shot-to-shot and none of the developments performed so far resolved this problem. In this letter we present a simple method that allows to produce stable and bright Betatron x-ray beams. In addition, we demonstrate that this scheme provides polarized and easily tunable radiation. Experimental results show tha"},"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":"1509.08629","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2015-09-29T08:18:05Z","cross_cats_sorted":[],"title_canon_sha256":"05bc45db251c353e4f46d9cb07300aaa0e58e41d4cddb4878511a349907f2167","abstract_canon_sha256":"3a7ecd1b09e157a9d642b4f6e810dcd171133e0b16bd8c050d10664511782f53"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:31:47.461539Z","signature_b64":"BOiYur5cT1csccafxPwJenbG5YPS2RqAdtjTbHu7Cd81xwx2rwgiDfVmDKVqo4UDq0XGEf5yIi1NNucSQKmTAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1df9b55e57d7cd34153523a3697c87f946a9ff57182eb179ecd57d932856855f","last_reissued_at":"2026-05-18T01:31:47.461092Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:31:47.461092Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Stable and polarized Betatron x-ray radiation from a laser plasma accelerator in ionization injection regime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"Agustin Lifschitz, Amar Tafzi, Andreas Doepp, Antoine Doche, Antoine Rousse, Benoit Mahieu, Cedric Thaury, Emilien Guillaume, Gabriele Grittani, Jean Philippe Goddet, Julien Gautier, Kim Ta Phuoc, Martin Hansson, Michaela Kozlova, Olle Lund, Pascal Rousseau, Sebastien Corde, Victor Malka","submitted_at":"2015-09-29T08:18:05Z","abstract_excerpt":"Betatron x-ray source from laser plasma interaction combines high brightness, few femtosecond duration and broad band energy spectrum. However, despite these unique features the Betatron source has a crippling drawback preventing its use for applications. Its properties significantly vary shot-to-shot and none of the developments performed so far resolved this problem. In this letter we present a simple method that allows to produce stable and bright Betatron x-ray beams. In addition, we demonstrate that this scheme provides polarized and easily tunable radiation. Experimental results show tha"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.08629","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":"1509.08629","created_at":"2026-05-18T01:31:47.461149+00:00"},{"alias_kind":"arxiv_version","alias_value":"1509.08629v1","created_at":"2026-05-18T01:31:47.461149+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.08629","created_at":"2026-05-18T01:31:47.461149+00:00"},{"alias_kind":"pith_short_12","alias_value":"DX43KXSX27GT","created_at":"2026-05-18T12:29:17.054201+00:00"},{"alias_kind":"pith_short_16","alias_value":"DX43KXSX27GTIFJV","created_at":"2026-05-18T12:29:17.054201+00:00"},{"alias_kind":"pith_short_8","alias_value":"DX43KXSX","created_at":"2026-05-18T12:29:17.054201+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/DX43KXSX27GTIFJVEORWS7EH7F","json":"https://pith.science/pith/DX43KXSX27GTIFJVEORWS7EH7F.json","graph_json":"https://pith.science/api/pith-number/DX43KXSX27GTIFJVEORWS7EH7F/graph.json","events_json":"https://pith.science/api/pith-number/DX43KXSX27GTIFJVEORWS7EH7F/events.json","paper":"https://pith.science/paper/DX43KXSX"},"agent_actions":{"view_html":"https://pith.science/pith/DX43KXSX27GTIFJVEORWS7EH7F","download_json":"https://pith.science/pith/DX43KXSX27GTIFJVEORWS7EH7F.json","view_paper":"https://pith.science/paper/DX43KXSX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1509.08629&json=true","fetch_graph":"https://pith.science/api/pith-number/DX43KXSX27GTIFJVEORWS7EH7F/graph.json","fetch_events":"https://pith.science/api/pith-number/DX43KXSX27GTIFJVEORWS7EH7F/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DX43KXSX27GTIFJVEORWS7EH7F/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DX43KXSX27GTIFJVEORWS7EH7F/action/storage_attestation","attest_author":"https://pith.science/pith/DX43KXSX27GTIFJVEORWS7EH7F/action/author_attestation","sign_citation":"https://pith.science/pith/DX43KXSX27GTIFJVEORWS7EH7F/action/citation_signature","submit_replication":"https://pith.science/pith/DX43KXSX27GTIFJVEORWS7EH7F/action/replication_record"}},"created_at":"2026-05-18T01:31:47.461149+00:00","updated_at":"2026-05-18T01:31:47.461149+00:00"}