{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:EXDFCRCUZWBBL7YPQXTEFCTZN4","short_pith_number":"pith:EXDFCRCU","schema_version":"1.0","canonical_sha256":"25c6514454cd8215ff0f85e6428a796f29d0475919a88463e6b3db4922db6337","source":{"kind":"arxiv","id":"1803.10398","version":1},"attestation_state":"computed","paper":{"title":"Scalings and Plasma Profile Parameterisation of ASDEX High Density Ohmic Discharges","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"H. Murmann, K. Lackner, K.S. Riedel, O.J.W.F. Kardaun, P.J. Mc Carthy","submitted_at":"2018-03-28T03:20:37Z","abstract_excerpt":"High density ($.3 < \\bar{n}/10^{20}{\\rm m^{-3}} < .8$), low $q_a$ ($1.9<q_a<3.4$), Ohmic discharges from the ASDEX experiment is analysed statistically.\n  Bulk parameter scalings and parameterised temperature and density profile shapes are presented. The total plasma kinetic energy, assuming $T_i=T_e$, scales as $\\bar{n}^{\\ .54\\pm .01} {I_p}^{.90\\pm .04 } $ and is almost independent of $B_t$. The electron temperature profile peaking factor scales as ${T_0^{3/2}/<T^{3/2}>} = .94(\\pm.04){q_a}^{1.07\\pm.04}$ in close agreement with the assumption of classical resistive equilibrium. In the inner ha"},"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":"1803.10398","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2018-03-28T03:20:37Z","cross_cats_sorted":[],"title_canon_sha256":"7e07bdc6634bdd0f16719f44d1a89c96107b4f2be91d2d4640a31e1d515db8a5","abstract_canon_sha256":"76ef76e888d2ee23afb4668f0efe0ad7c0007621d80307ec644a4e8a2db513be"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:19:55.535001Z","signature_b64":"+BBhKM3drebh5+xS+RszlQo2nWAUaRpnLr9I8LQLzqYSNcMvrdXtWOuaqRyLDI+nT4uUTbBNDQ8vOgKYwCDvAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"25c6514454cd8215ff0f85e6428a796f29d0475919a88463e6b3db4922db6337","last_reissued_at":"2026-05-18T00:19:55.534399Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:19:55.534399Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Scalings and Plasma Profile Parameterisation of ASDEX High Density Ohmic Discharges","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"H. Murmann, K. Lackner, K.S. Riedel, O.J.W.F. Kardaun, P.J. Mc Carthy","submitted_at":"2018-03-28T03:20:37Z","abstract_excerpt":"High density ($.3 < \\bar{n}/10^{20}{\\rm m^{-3}} < .8$), low $q_a$ ($1.9<q_a<3.4$), Ohmic discharges from the ASDEX experiment is analysed statistically.\n  Bulk parameter scalings and parameterised temperature and density profile shapes are presented. The total plasma kinetic energy, assuming $T_i=T_e$, scales as $\\bar{n}^{\\ .54\\pm .01} {I_p}^{.90\\pm .04 } $ and is almost independent of $B_t$. The electron temperature profile peaking factor scales as ${T_0^{3/2}/<T^{3/2}>} = .94(\\pm.04){q_a}^{1.07\\pm.04}$ in close agreement with the assumption of classical resistive equilibrium. In the inner ha"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1803.10398","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":"1803.10398","created_at":"2026-05-18T00:19:55.534501+00:00"},{"alias_kind":"arxiv_version","alias_value":"1803.10398v1","created_at":"2026-05-18T00:19:55.534501+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1803.10398","created_at":"2026-05-18T00:19:55.534501+00:00"},{"alias_kind":"pith_short_12","alias_value":"EXDFCRCUZWBB","created_at":"2026-05-18T12:32:22.470017+00:00"},{"alias_kind":"pith_short_16","alias_value":"EXDFCRCUZWBBL7YP","created_at":"2026-05-18T12:32:22.470017+00:00"},{"alias_kind":"pith_short_8","alias_value":"EXDFCRCU","created_at":"2026-05-18T12:32:22.470017+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/EXDFCRCUZWBBL7YPQXTEFCTZN4","json":"https://pith.science/pith/EXDFCRCUZWBBL7YPQXTEFCTZN4.json","graph_json":"https://pith.science/api/pith-number/EXDFCRCUZWBBL7YPQXTEFCTZN4/graph.json","events_json":"https://pith.science/api/pith-number/EXDFCRCUZWBBL7YPQXTEFCTZN4/events.json","paper":"https://pith.science/paper/EXDFCRCU"},"agent_actions":{"view_html":"https://pith.science/pith/EXDFCRCUZWBBL7YPQXTEFCTZN4","download_json":"https://pith.science/pith/EXDFCRCUZWBBL7YPQXTEFCTZN4.json","view_paper":"https://pith.science/paper/EXDFCRCU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1803.10398&json=true","fetch_graph":"https://pith.science/api/pith-number/EXDFCRCUZWBBL7YPQXTEFCTZN4/graph.json","fetch_events":"https://pith.science/api/pith-number/EXDFCRCUZWBBL7YPQXTEFCTZN4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EXDFCRCUZWBBL7YPQXTEFCTZN4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EXDFCRCUZWBBL7YPQXTEFCTZN4/action/storage_attestation","attest_author":"https://pith.science/pith/EXDFCRCUZWBBL7YPQXTEFCTZN4/action/author_attestation","sign_citation":"https://pith.science/pith/EXDFCRCUZWBBL7YPQXTEFCTZN4/action/citation_signature","submit_replication":"https://pith.science/pith/EXDFCRCUZWBBL7YPQXTEFCTZN4/action/replication_record"}},"created_at":"2026-05-18T00:19:55.534501+00:00","updated_at":"2026-05-18T00:19:55.534501+00:00"}