{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:5JHRI3ZZH72RFEPTXPATVD6W7W","short_pith_number":"pith:5JHRI3ZZ","canonical_record":{"source":{"id":"1310.8437","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2013-10-31T09:56:32Z","cross_cats_sorted":[],"title_canon_sha256":"2f44244b26138d6a40ca8781f05981118da3593cddf4085f7d039e608709ad15","abstract_canon_sha256":"daf504328e0061c7d2c7c112920c8ac0262d5e7134555c61cecc1c639c38d0df"},"schema_version":"1.0"},"canonical_sha256":"ea4f146f393ff51291f3bbc13a8fd6fdad996719c86f0403d105b78fd3905be0","source":{"kind":"arxiv","id":"1310.8437","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1310.8437","created_at":"2026-05-18T03:08:17Z"},{"alias_kind":"arxiv_version","alias_value":"1310.8437v1","created_at":"2026-05-18T03:08:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.8437","created_at":"2026-05-18T03:08:17Z"},{"alias_kind":"pith_short_12","alias_value":"5JHRI3ZZH72R","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_16","alias_value":"5JHRI3ZZH72RFEPT","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_8","alias_value":"5JHRI3ZZ","created_at":"2026-05-18T12:27:34Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:5JHRI3ZZH72RFEPTXPATVD6W7W","target":"record","payload":{"canonical_record":{"source":{"id":"1310.8437","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2013-10-31T09:56:32Z","cross_cats_sorted":[],"title_canon_sha256":"2f44244b26138d6a40ca8781f05981118da3593cddf4085f7d039e608709ad15","abstract_canon_sha256":"daf504328e0061c7d2c7c112920c8ac0262d5e7134555c61cecc1c639c38d0df"},"schema_version":"1.0"},"canonical_sha256":"ea4f146f393ff51291f3bbc13a8fd6fdad996719c86f0403d105b78fd3905be0","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:08:17.061759Z","signature_b64":"sc/17qjpZEUsrusMrWRlT30JfXoTrxVLIUUFApyx0BLViAiuDraBdozox3zimewCYaSHcn9QCnou5nLw7ctSBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ea4f146f393ff51291f3bbc13a8fd6fdad996719c86f0403d105b78fd3905be0","last_reissued_at":"2026-05-18T03:08:17.061074Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:08:17.061074Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1310.8437","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:08:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"L5um8PZ5M0jvVmuX+0wHg8majnENudIDQI0FWSxkMideYdebB+s8oAHAUzT8O/mTi4KNcl8LMRNxkLZkRJD5BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T20:50:42.146020Z"},"content_sha256":"060498d3dfa444da59370c0075f01ae19aeb17730339b65c75f2b040a30401ab","schema_version":"1.0","event_id":"sha256:060498d3dfa444da59370c0075f01ae19aeb17730339b65c75f2b040a30401ab"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:5JHRI3ZZH72RFEPTXPATVD6W7W","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Self-consistent simulation of plasma scenarios for ITER using a combination of 1.5D transport codes and free-boundary equilibrium codes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"A Loarte, C V Labate, D McDonald, E Nardon, F Imbeaux, F Koechl, G Corrigan, G Saibene, J-F Artaud, J Garcia, J Lister, J Urban, K Besseghir, L Garzotti, M Cavinato, M Mattei, P Maget, R Albanese, R Ambrosino, R Sartori, V Parail, X Litaudon, Y Gribov","submitted_at":"2013-10-31T09:56:32Z","abstract_excerpt":"Self-consistent transport simulation of ITER scenarios is a very important tool for the exploration of the operational space and for scenario optimisation. It also provides an assessment of the compatibility of developed scenarios (which include fast transient events) with machine constraints, in particular with the poloidal field (PF) coil system, heating and current drive (H&CD), fuelling and particle and energy exhaust systems. This paper discusses results of predictive modelling of all reference ITER scenarios and variants using two suite of linked transport and equilibrium codes. The firs"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.8437","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:08:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fVwvHHUnejFJvuT0BJLqNmrTzKECfqjbqEjW6IENfwj5VsksJSGYDbnIYrcsh7USHMoJ5mFJFQonPJmN5V4nAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T20:50:42.146444Z"},"content_sha256":"b6201eeeab5905854bc36dbd05c6e7a41d6d52adc89793a3e10a8fd619e91810","schema_version":"1.0","event_id":"sha256:b6201eeeab5905854bc36dbd05c6e7a41d6d52adc89793a3e10a8fd619e91810"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5JHRI3ZZH72RFEPTXPATVD6W7W/bundle.json","state_url":"https://pith.science/pith/5JHRI3ZZH72RFEPTXPATVD6W7W/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5JHRI3ZZH72RFEPTXPATVD6W7W/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":"2026-05-27T20:50:42Z","links":{"resolver":"https://pith.science/pith/5JHRI3ZZH72RFEPTXPATVD6W7W","bundle":"https://pith.science/pith/5JHRI3ZZH72RFEPTXPATVD6W7W/bundle.json","state":"https://pith.science/pith/5JHRI3ZZH72RFEPTXPATVD6W7W/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5JHRI3ZZH72RFEPTXPATVD6W7W/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:5JHRI3ZZH72RFEPTXPATVD6W7W","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":"daf504328e0061c7d2c7c112920c8ac0262d5e7134555c61cecc1c639c38d0df","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2013-10-31T09:56:32Z","title_canon_sha256":"2f44244b26138d6a40ca8781f05981118da3593cddf4085f7d039e608709ad15"},"schema_version":"1.0","source":{"id":"1310.8437","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1310.8437","created_at":"2026-05-18T03:08:17Z"},{"alias_kind":"arxiv_version","alias_value":"1310.8437v1","created_at":"2026-05-18T03:08:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.8437","created_at":"2026-05-18T03:08:17Z"},{"alias_kind":"pith_short_12","alias_value":"5JHRI3ZZH72R","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_16","alias_value":"5JHRI3ZZH72RFEPT","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_8","alias_value":"5JHRI3ZZ","created_at":"2026-05-18T12:27:34Z"}],"graph_snapshots":[{"event_id":"sha256:b6201eeeab5905854bc36dbd05c6e7a41d6d52adc89793a3e10a8fd619e91810","target":"graph","created_at":"2026-05-18T03:08:17Z","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":"Self-consistent transport simulation of ITER scenarios is a very important tool for the exploration of the operational space and for scenario optimisation. It also provides an assessment of the compatibility of developed scenarios (which include fast transient events) with machine constraints, in particular with the poloidal field (PF) coil system, heating and current drive (H&CD), fuelling and particle and energy exhaust systems. This paper discusses results of predictive modelling of all reference ITER scenarios and variants using two suite of linked transport and equilibrium codes. The firs","authors_text":"A Loarte, C V Labate, D McDonald, E Nardon, F Imbeaux, F Koechl, G Corrigan, G Saibene, J-F Artaud, J Garcia, J Lister, J Urban, K Besseghir, L Garzotti, M Cavinato, M Mattei, P Maget, R Albanese, R Ambrosino, R Sartori, V Parail, X Litaudon, Y Gribov","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2013-10-31T09:56:32Z","title":"Self-consistent simulation of plasma scenarios for ITER using a combination of 1.5D transport codes and free-boundary equilibrium codes"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.8437","kind":"arxiv","version":1},"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":"sha256:060498d3dfa444da59370c0075f01ae19aeb17730339b65c75f2b040a30401ab","target":"record","created_at":"2026-05-18T03:08:17Z","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":"daf504328e0061c7d2c7c112920c8ac0262d5e7134555c61cecc1c639c38d0df","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2013-10-31T09:56:32Z","title_canon_sha256":"2f44244b26138d6a40ca8781f05981118da3593cddf4085f7d039e608709ad15"},"schema_version":"1.0","source":{"id":"1310.8437","kind":"arxiv","version":1}},"canonical_sha256":"ea4f146f393ff51291f3bbc13a8fd6fdad996719c86f0403d105b78fd3905be0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ea4f146f393ff51291f3bbc13a8fd6fdad996719c86f0403d105b78fd3905be0","first_computed_at":"2026-05-18T03:08:17.061074Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:08:17.061074Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"sc/17qjpZEUsrusMrWRlT30JfXoTrxVLIUUFApyx0BLViAiuDraBdozox3zimewCYaSHcn9QCnou5nLw7ctSBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:08:17.061759Z","signed_message":"canonical_sha256_bytes"},"source_id":"1310.8437","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:060498d3dfa444da59370c0075f01ae19aeb17730339b65c75f2b040a30401ab","sha256:b6201eeeab5905854bc36dbd05c6e7a41d6d52adc89793a3e10a8fd619e91810"],"state_sha256":"69c3d881267bb904471f3a4811101b18d1cff63229a82b66c84f80140de27465"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ttriuKWYrwICSE2NWEc9nN4n7SPc904ixcva+PMHRR3OuoNApf1Pu5eKN8Pi20ZJKZXasypmHHprsPSOcUakAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T20:50:42.149074Z","bundle_sha256":"efd32d82c1cbf50ffd0466f169e2111387b408c87f5ccacda5c9acb881ff3c28"}}