{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:3KWIKI6GFV4GXDRRP7VPFAB5AQ","short_pith_number":"pith:3KWIKI6G","canonical_record":{"source":{"id":"1412.7898","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2014-12-26T06:44:33Z","cross_cats_sorted":[],"title_canon_sha256":"3b8e0a383dc95565604a1d0b1dd6f2d09c1e87aa189f14cee3b7acfdc88437da","abstract_canon_sha256":"4e3edb4a248263c58de594d61095b577524063a49219be4fa5ee34948142eafb"},"schema_version":"1.0"},"canonical_sha256":"daac8523c62d786b8e317feaf2803d043b891f9479d3e1fde1511667ec034300","source":{"kind":"arxiv","id":"1412.7898","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.7898","created_at":"2026-05-18T01:34:25Z"},{"alias_kind":"arxiv_version","alias_value":"1412.7898v3","created_at":"2026-05-18T01:34:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.7898","created_at":"2026-05-18T01:34:25Z"},{"alias_kind":"pith_short_12","alias_value":"3KWIKI6GFV4G","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_16","alias_value":"3KWIKI6GFV4GXDRR","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_8","alias_value":"3KWIKI6G","created_at":"2026-05-18T12:28:11Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:3KWIKI6GFV4GXDRRP7VPFAB5AQ","target":"record","payload":{"canonical_record":{"source":{"id":"1412.7898","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2014-12-26T06:44:33Z","cross_cats_sorted":[],"title_canon_sha256":"3b8e0a383dc95565604a1d0b1dd6f2d09c1e87aa189f14cee3b7acfdc88437da","abstract_canon_sha256":"4e3edb4a248263c58de594d61095b577524063a49219be4fa5ee34948142eafb"},"schema_version":"1.0"},"canonical_sha256":"daac8523c62d786b8e317feaf2803d043b891f9479d3e1fde1511667ec034300","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:34:25.028641Z","signature_b64":"dr2hJUXAYRwAtTzDN0mD/SOvnrped8+8pwt6vLTE7k4kpcmUagvfmob4xC4VycG9vZ0gPr9t0u3hj19VppTZDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"daac8523c62d786b8e317feaf2803d043b891f9479d3e1fde1511667ec034300","last_reissued_at":"2026-05-18T01:34:25.028170Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:34:25.028170Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1412.7898","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:34:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"muBisPP8Vtt4Dk/hVFDVArhhGyCZyyroPl7fTtBW8IrMcwPgnCn665wWYDkzonqrY+5rl9aHCUV4DG8gZ/1BBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T17:18:03.363897Z"},"content_sha256":"f692101a9c10898b16cd0582700233c0f0cdd9fe10c227218f8c488b650b7a73","schema_version":"1.0","event_id":"sha256:f692101a9c10898b16cd0582700233c0f0cdd9fe10c227218f8c488b650b7a73"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:3KWIKI6GFV4GXDRRP7VPFAB5AQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Analysis of the Thermonuclear Instability including Low-Power ICRH Minority Heating in IGNITOR","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"Alessandro Cardinali, Giorgio Sonnino","submitted_at":"2014-12-26T06:44:33Z","abstract_excerpt":"The nonlinear thermal balance equation for classical plasma in a toroidal geometry is analytically and numerically investigated including ICRH power. The determination of the equilibrium temperature and the analysis of the stability of the solution are performed by solving the energy balance equation that includes the transport relations obtained by the classical kinetic theory. An estimation of the confinement time is also provided. We show that the ICRH heating in the IGNITOR experiment, among other applications, is expected to be used to trigger the thermonuclear instability. Here a scenari"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.7898","kind":"arxiv","version":3},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:34:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JxidK3ZjDvVKcZ4b/VQvALSAHZkkJm9v/4EAfKp5qmNanbOnhMe1yLoQyp4l6UDrkjowwgjTSVu/Th3umj12DA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T17:18:03.364238Z"},"content_sha256":"9b7a81f168917eaefec45ab6db989e91828321ce9c7270aed568bf144fc084af","schema_version":"1.0","event_id":"sha256:9b7a81f168917eaefec45ab6db989e91828321ce9c7270aed568bf144fc084af"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3KWIKI6GFV4GXDRRP7VPFAB5AQ/bundle.json","state_url":"https://pith.science/pith/3KWIKI6GFV4GXDRRP7VPFAB5AQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3KWIKI6GFV4GXDRRP7VPFAB5AQ/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-03T17:18:03Z","links":{"resolver":"https://pith.science/pith/3KWIKI6GFV4GXDRRP7VPFAB5AQ","bundle":"https://pith.science/pith/3KWIKI6GFV4GXDRRP7VPFAB5AQ/bundle.json","state":"https://pith.science/pith/3KWIKI6GFV4GXDRRP7VPFAB5AQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3KWIKI6GFV4GXDRRP7VPFAB5AQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:3KWIKI6GFV4GXDRRP7VPFAB5AQ","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"4e3edb4a248263c58de594d61095b577524063a49219be4fa5ee34948142eafb","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2014-12-26T06:44:33Z","title_canon_sha256":"3b8e0a383dc95565604a1d0b1dd6f2d09c1e87aa189f14cee3b7acfdc88437da"},"schema_version":"1.0","source":{"id":"1412.7898","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.7898","created_at":"2026-05-18T01:34:25Z"},{"alias_kind":"arxiv_version","alias_value":"1412.7898v3","created_at":"2026-05-18T01:34:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.7898","created_at":"2026-05-18T01:34:25Z"},{"alias_kind":"pith_short_12","alias_value":"3KWIKI6GFV4G","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_16","alias_value":"3KWIKI6GFV4GXDRR","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_8","alias_value":"3KWIKI6G","created_at":"2026-05-18T12:28:11Z"}],"graph_snapshots":[{"event_id":"sha256:9b7a81f168917eaefec45ab6db989e91828321ce9c7270aed568bf144fc084af","target":"graph","created_at":"2026-05-18T01:34:25Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"The nonlinear thermal balance equation for classical plasma in a toroidal geometry is analytically and numerically investigated including ICRH power. The determination of the equilibrium temperature and the analysis of the stability of the solution are performed by solving the energy balance equation that includes the transport relations obtained by the classical kinetic theory. An estimation of the confinement time is also provided. We show that the ICRH heating in the IGNITOR experiment, among other applications, is expected to be used to trigger the thermonuclear instability. Here a scenari","authors_text":"Alessandro Cardinali, Giorgio Sonnino","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2014-12-26T06:44:33Z","title":"Analysis of the Thermonuclear Instability including Low-Power ICRH Minority Heating in IGNITOR"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.7898","kind":"arxiv","version":3},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:f692101a9c10898b16cd0582700233c0f0cdd9fe10c227218f8c488b650b7a73","target":"record","created_at":"2026-05-18T01:34:25Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"4e3edb4a248263c58de594d61095b577524063a49219be4fa5ee34948142eafb","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2014-12-26T06:44:33Z","title_canon_sha256":"3b8e0a383dc95565604a1d0b1dd6f2d09c1e87aa189f14cee3b7acfdc88437da"},"schema_version":"1.0","source":{"id":"1412.7898","kind":"arxiv","version":3}},"canonical_sha256":"daac8523c62d786b8e317feaf2803d043b891f9479d3e1fde1511667ec034300","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"daac8523c62d786b8e317feaf2803d043b891f9479d3e1fde1511667ec034300","first_computed_at":"2026-05-18T01:34:25.028170Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:34:25.028170Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"dr2hJUXAYRwAtTzDN0mD/SOvnrped8+8pwt6vLTE7k4kpcmUagvfmob4xC4VycG9vZ0gPr9t0u3hj19VppTZDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:34:25.028641Z","signed_message":"canonical_sha256_bytes"},"source_id":"1412.7898","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f692101a9c10898b16cd0582700233c0f0cdd9fe10c227218f8c488b650b7a73","sha256:9b7a81f168917eaefec45ab6db989e91828321ce9c7270aed568bf144fc084af"],"state_sha256":"c717f6cc50b64e119d6bc2b973cfa1e21e9681cac82078317b4aedd221a0d971"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7zgCE34zgt5p4YiLJNXq71JgSSwIsqotLRlu9IKA2OfZ4FbzMabPpZOAsuCvNO/mkcSnECT0aMoXEpxOSb37Bg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T17:18:03.366167Z","bundle_sha256":"9ac520c7707455694935f085d1a3bffe00f6d20db8b38dcadf33e555d1f1b3be"}}