{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:LO6AQ6CR4RG7PRWAJMH3K5PDJK","short_pith_number":"pith:LO6AQ6CR","schema_version":"1.0","canonical_sha256":"5bbc087851e44df7c6c04b0fb575e34a85df40cc40960f97a4d697d18eaa397d","source":{"kind":"arxiv","id":"1411.1508","version":2},"attestation_state":"computed","paper":{"title":"Constraints for the aperiodic O-mode streaming instability","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.SR"],"primary_cat":"physics.plasm-ph","authors_text":"A. Stockem, M. Lazar, R. Schlickeiser, S. Poedts, S. Vafin","submitted_at":"2014-11-06T07:02:28Z","abstract_excerpt":"In plasmas where the thermal energy density exceeds the magnetic energy density ($\\beta_\\parallel > 1$), the aperiodic ordinary mode (O-mode) instability is driven by an excess of parallel temperature $A = T_\\perp /T_\\parallel < 1$ (where $\\parallel$ and $\\perp$ denote directions relative to the uniform magnetic field). When stimulated by parallel plasma streams the instability conditions extend to low beta states, i.e., $\\beta_\\parallel <1$, and recent studies have proven the existence of a new regime, where the anisotropy threshold decreases steeply with lowering $\\beta_\\parallel \\to 0$ if t"},"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":"1411.1508","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2014-11-06T07:02:28Z","cross_cats_sorted":["astro-ph.SR"],"title_canon_sha256":"e62a33ec96af41c6b5783e83f75f02998f141da4606789690ba5aa7c937bd2d6","abstract_canon_sha256":"0f89240e3956f72394511e2c64bf069a0ea9df4ed479a9f212d38034a16c1bd1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:41:34.494548Z","signature_b64":"Ul5nreNasmdNwV7gzLRag9WIpGzUU5k01BHAiuVLtSME5GjhGEAzhTD9RCzXZicGMb6DLE3l61PnbWSwT070Dw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5bbc087851e44df7c6c04b0fb575e34a85df40cc40960f97a4d697d18eaa397d","last_reissued_at":"2026-05-18T01:41:34.493863Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:41:34.493863Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Constraints for the aperiodic O-mode streaming instability","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.SR"],"primary_cat":"physics.plasm-ph","authors_text":"A. Stockem, M. Lazar, R. Schlickeiser, S. Poedts, S. Vafin","submitted_at":"2014-11-06T07:02:28Z","abstract_excerpt":"In plasmas where the thermal energy density exceeds the magnetic energy density ($\\beta_\\parallel > 1$), the aperiodic ordinary mode (O-mode) instability is driven by an excess of parallel temperature $A = T_\\perp /T_\\parallel < 1$ (where $\\parallel$ and $\\perp$ denote directions relative to the uniform magnetic field). When stimulated by parallel plasma streams the instability conditions extend to low beta states, i.e., $\\beta_\\parallel <1$, and recent studies have proven the existence of a new regime, where the anisotropy threshold decreases steeply with lowering $\\beta_\\parallel \\to 0$ if t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.1508","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":""},"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":"1411.1508","created_at":"2026-05-18T01:41:34.493976+00:00"},{"alias_kind":"arxiv_version","alias_value":"1411.1508v2","created_at":"2026-05-18T01:41:34.493976+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.1508","created_at":"2026-05-18T01:41:34.493976+00:00"},{"alias_kind":"pith_short_12","alias_value":"LO6AQ6CR4RG7","created_at":"2026-05-18T12:28:38.356838+00:00"},{"alias_kind":"pith_short_16","alias_value":"LO6AQ6CR4RG7PRWA","created_at":"2026-05-18T12:28:38.356838+00:00"},{"alias_kind":"pith_short_8","alias_value":"LO6AQ6CR","created_at":"2026-05-18T12:28:38.356838+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/LO6AQ6CR4RG7PRWAJMH3K5PDJK","json":"https://pith.science/pith/LO6AQ6CR4RG7PRWAJMH3K5PDJK.json","graph_json":"https://pith.science/api/pith-number/LO6AQ6CR4RG7PRWAJMH3K5PDJK/graph.json","events_json":"https://pith.science/api/pith-number/LO6AQ6CR4RG7PRWAJMH3K5PDJK/events.json","paper":"https://pith.science/paper/LO6AQ6CR"},"agent_actions":{"view_html":"https://pith.science/pith/LO6AQ6CR4RG7PRWAJMH3K5PDJK","download_json":"https://pith.science/pith/LO6AQ6CR4RG7PRWAJMH3K5PDJK.json","view_paper":"https://pith.science/paper/LO6AQ6CR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1411.1508&json=true","fetch_graph":"https://pith.science/api/pith-number/LO6AQ6CR4RG7PRWAJMH3K5PDJK/graph.json","fetch_events":"https://pith.science/api/pith-number/LO6AQ6CR4RG7PRWAJMH3K5PDJK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LO6AQ6CR4RG7PRWAJMH3K5PDJK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LO6AQ6CR4RG7PRWAJMH3K5PDJK/action/storage_attestation","attest_author":"https://pith.science/pith/LO6AQ6CR4RG7PRWAJMH3K5PDJK/action/author_attestation","sign_citation":"https://pith.science/pith/LO6AQ6CR4RG7PRWAJMH3K5PDJK/action/citation_signature","submit_replication":"https://pith.science/pith/LO6AQ6CR4RG7PRWAJMH3K5PDJK/action/replication_record"}},"created_at":"2026-05-18T01:41:34.493976+00:00","updated_at":"2026-05-18T01:41:34.493976+00:00"}