{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:RZHCDZY5DF2EB5GYBQQCKAWV5C","short_pith_number":"pith:RZHCDZY5","canonical_record":{"source":{"id":"1505.00726","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2015-05-04T17:42:08Z","cross_cats_sorted":["astro-ph.HE","astro-ph.SR","physics.space-ph"],"title_canon_sha256":"b56f504731cad1fcee06f5823582450438b5bd5d2fcc2832b2e818237794b42f","abstract_canon_sha256":"a790a6fe9068fc4e4bb011dc6933d8710ece1d3b6bedd6de75d6452d991c004c"},"schema_version":"1.0"},"canonical_sha256":"8e4e21e71d197440f4d80c202502d5e898c679fa68b51c86101df87df79778e2","source":{"kind":"arxiv","id":"1505.00726","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1505.00726","created_at":"2026-05-18T01:36:33Z"},{"alias_kind":"arxiv_version","alias_value":"1505.00726v1","created_at":"2026-05-18T01:36:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1505.00726","created_at":"2026-05-18T01:36:33Z"},{"alias_kind":"pith_short_12","alias_value":"RZHCDZY5DF2E","created_at":"2026-05-18T12:29:39Z"},{"alias_kind":"pith_short_16","alias_value":"RZHCDZY5DF2EB5GY","created_at":"2026-05-18T12:29:39Z"},{"alias_kind":"pith_short_8","alias_value":"RZHCDZY5","created_at":"2026-05-18T12:29:39Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:RZHCDZY5DF2EB5GYBQQCKAWV5C","target":"record","payload":{"canonical_record":{"source":{"id":"1505.00726","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2015-05-04T17:42:08Z","cross_cats_sorted":["astro-ph.HE","astro-ph.SR","physics.space-ph"],"title_canon_sha256":"b56f504731cad1fcee06f5823582450438b5bd5d2fcc2832b2e818237794b42f","abstract_canon_sha256":"a790a6fe9068fc4e4bb011dc6933d8710ece1d3b6bedd6de75d6452d991c004c"},"schema_version":"1.0"},"canonical_sha256":"8e4e21e71d197440f4d80c202502d5e898c679fa68b51c86101df87df79778e2","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:36:33.448282Z","signature_b64":"CrNX5itK9Ufbmjc1846tALw3u0WTPjvJ9mpUcyfeWbFY3SHZh/w1uiw3AFc8DHhxgMRq10nMso+xwzpkzJ1pAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8e4e21e71d197440f4d80c202502d5e898c679fa68b51c86101df87df79778e2","last_reissued_at":"2026-05-18T01:36:33.447805Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:36:33.447805Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1505.00726","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":"2026-05-18T01:36:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lc0n3FeIaORi+24ccUo2+jDylSUuubNmCh1zqmlLBjjuUmBqCkYk4WffgIu7Ck7RNf4x9OFFsGwCOC2N4oPcCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T07:51:14.603438Z"},"content_sha256":"924219fc318db068e3d49c48376a3f087032f397ff66065b0024a20758cd4dae","schema_version":"1.0","event_id":"sha256:924219fc318db068e3d49c48376a3f087032f397ff66065b0024a20758cd4dae"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:RZHCDZY5DF2EB5GYBQQCKAWV5C","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Phase Diagrams of Forced Magnetic Reconnection in Taylor's Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.HE","astro-ph.SR","physics.space-ph"],"primary_cat":"physics.plasm-ph","authors_text":"D. Grasso, F.L. Waelbroeck, L. Comisso","submitted_at":"2015-05-04T17:42:08Z","abstract_excerpt":"Recent progress in the understanding of how externally driven magnetic reconnection evolves is organized in terms of parameter space diagrams. These diagrams are constructed using four pivotal dimensionless parameters: the Lundquist number $S$, the magnetic Prandtl number $P_m$, the amplitude of the boundary perturbation $\\hat \\Psi_0$, and the perturbation wave number $\\hat k$. This new representation highlights the parameters regions of a given system in which the magnetic reconnection process is expected to be distinguished by a specific evolution. Contrary to previously proposed phase diagr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1505.00726","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":"2026-05-18T01:36:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2vCtQh0epqOrHoL2Qtq5QDTBwFIBMznLcq6xSUJU6tVM+jWLYQDt3zqEn62dLNHi6vSWN5YF4I/cjsEbjqUtDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T07:51:14.603795Z"},"content_sha256":"825d23219ad76966200531b8956de47e3694e1370055aa513e268101201cea75","schema_version":"1.0","event_id":"sha256:825d23219ad76966200531b8956de47e3694e1370055aa513e268101201cea75"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RZHCDZY5DF2EB5GYBQQCKAWV5C/bundle.json","state_url":"https://pith.science/pith/RZHCDZY5DF2EB5GYBQQCKAWV5C/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RZHCDZY5DF2EB5GYBQQCKAWV5C/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":"2026-06-02T07:51:14Z","links":{"resolver":"https://pith.science/pith/RZHCDZY5DF2EB5GYBQQCKAWV5C","bundle":"https://pith.science/pith/RZHCDZY5DF2EB5GYBQQCKAWV5C/bundle.json","state":"https://pith.science/pith/RZHCDZY5DF2EB5GYBQQCKAWV5C/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RZHCDZY5DF2EB5GYBQQCKAWV5C/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:RZHCDZY5DF2EB5GYBQQCKAWV5C","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":"a790a6fe9068fc4e4bb011dc6933d8710ece1d3b6bedd6de75d6452d991c004c","cross_cats_sorted":["astro-ph.HE","astro-ph.SR","physics.space-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2015-05-04T17:42:08Z","title_canon_sha256":"b56f504731cad1fcee06f5823582450438b5bd5d2fcc2832b2e818237794b42f"},"schema_version":"1.0","source":{"id":"1505.00726","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1505.00726","created_at":"2026-05-18T01:36:33Z"},{"alias_kind":"arxiv_version","alias_value":"1505.00726v1","created_at":"2026-05-18T01:36:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1505.00726","created_at":"2026-05-18T01:36:33Z"},{"alias_kind":"pith_short_12","alias_value":"RZHCDZY5DF2E","created_at":"2026-05-18T12:29:39Z"},{"alias_kind":"pith_short_16","alias_value":"RZHCDZY5DF2EB5GY","created_at":"2026-05-18T12:29:39Z"},{"alias_kind":"pith_short_8","alias_value":"RZHCDZY5","created_at":"2026-05-18T12:29:39Z"}],"graph_snapshots":[{"event_id":"sha256:825d23219ad76966200531b8956de47e3694e1370055aa513e268101201cea75","target":"graph","created_at":"2026-05-18T01:36:33Z","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":"Recent progress in the understanding of how externally driven magnetic reconnection evolves is organized in terms of parameter space diagrams. These diagrams are constructed using four pivotal dimensionless parameters: the Lundquist number $S$, the magnetic Prandtl number $P_m$, the amplitude of the boundary perturbation $\\hat \\Psi_0$, and the perturbation wave number $\\hat k$. This new representation highlights the parameters regions of a given system in which the magnetic reconnection process is expected to be distinguished by a specific evolution. Contrary to previously proposed phase diagr","authors_text":"D. Grasso, F.L. Waelbroeck, L. Comisso","cross_cats":["astro-ph.HE","astro-ph.SR","physics.space-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2015-05-04T17:42:08Z","title":"Phase Diagrams of Forced Magnetic Reconnection in Taylor's Model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1505.00726","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":"sha256:924219fc318db068e3d49c48376a3f087032f397ff66065b0024a20758cd4dae","target":"record","created_at":"2026-05-18T01:36:33Z","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":"a790a6fe9068fc4e4bb011dc6933d8710ece1d3b6bedd6de75d6452d991c004c","cross_cats_sorted":["astro-ph.HE","astro-ph.SR","physics.space-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2015-05-04T17:42:08Z","title_canon_sha256":"b56f504731cad1fcee06f5823582450438b5bd5d2fcc2832b2e818237794b42f"},"schema_version":"1.0","source":{"id":"1505.00726","kind":"arxiv","version":1}},"canonical_sha256":"8e4e21e71d197440f4d80c202502d5e898c679fa68b51c86101df87df79778e2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8e4e21e71d197440f4d80c202502d5e898c679fa68b51c86101df87df79778e2","first_computed_at":"2026-05-18T01:36:33.447805Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:36:33.447805Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"CrNX5itK9Ufbmjc1846tALw3u0WTPjvJ9mpUcyfeWbFY3SHZh/w1uiw3AFc8DHhxgMRq10nMso+xwzpkzJ1pAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:36:33.448282Z","signed_message":"canonical_sha256_bytes"},"source_id":"1505.00726","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:924219fc318db068e3d49c48376a3f087032f397ff66065b0024a20758cd4dae","sha256:825d23219ad76966200531b8956de47e3694e1370055aa513e268101201cea75"],"state_sha256":"42d7ea7ace47b6895bc285ab152a296cfc163c0697a776b5f99ea1fd7bb83d2c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"63QXysHXOZluKtHs5WMM87XE+ag2aWWJQsJN/6eDr+uXcR1Ewpa0hlAQC4MdB7c1mYtB3ITgLzbpG4rW9ywMBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T07:51:14.605823Z","bundle_sha256":"988c7be03765101fd06d5cbbeb57f4a6edf79b51d2796c4ba9230470ea1f6c45"}}