{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:UDIPFD43YRWQQVXX4H4P2DJNR6","short_pith_number":"pith:UDIPFD43","canonical_record":{"source":{"id":"1411.7526","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.SR","submitted_at":"2014-11-27T10:14:33Z","cross_cats_sorted":["physics.space-ph"],"title_canon_sha256":"9acd9bab1aac14bacfcb46c1c369e89b587ed3b528ca52a9b43cb73c780f4bcc","abstract_canon_sha256":"81d591540c857505492d775e82206e6f93263f3aaf6c6951fbfabb1f4b702ee1"},"schema_version":"1.0"},"canonical_sha256":"a0d0f28f9bc46d0856f7e1f8fd0d2d8faaf71445b42eff97fa35f3e996988634","source":{"kind":"arxiv","id":"1411.7526","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1411.7526","created_at":"2026-05-18T02:32:37Z"},{"alias_kind":"arxiv_version","alias_value":"1411.7526v1","created_at":"2026-05-18T02:32:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.7526","created_at":"2026-05-18T02:32:37Z"},{"alias_kind":"pith_short_12","alias_value":"UDIPFD43YRWQ","created_at":"2026-05-18T12:28:52Z"},{"alias_kind":"pith_short_16","alias_value":"UDIPFD43YRWQQVXX","created_at":"2026-05-18T12:28:52Z"},{"alias_kind":"pith_short_8","alias_value":"UDIPFD43","created_at":"2026-05-18T12:28:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:UDIPFD43YRWQQVXX4H4P2DJNR6","target":"record","payload":{"canonical_record":{"source":{"id":"1411.7526","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.SR","submitted_at":"2014-11-27T10:14:33Z","cross_cats_sorted":["physics.space-ph"],"title_canon_sha256":"9acd9bab1aac14bacfcb46c1c369e89b587ed3b528ca52a9b43cb73c780f4bcc","abstract_canon_sha256":"81d591540c857505492d775e82206e6f93263f3aaf6c6951fbfabb1f4b702ee1"},"schema_version":"1.0"},"canonical_sha256":"a0d0f28f9bc46d0856f7e1f8fd0d2d8faaf71445b42eff97fa35f3e996988634","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:32:37.795121Z","signature_b64":"2UVfg+0NSE7ymYa2NJ01Lkq4/aweKDW+PnCDbO6hSeR1LAIkib0Uf84mFqBOZzmKO6JRhFSaCGFoAdalDL25AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a0d0f28f9bc46d0856f7e1f8fd0d2d8faaf71445b42eff97fa35f3e996988634","last_reissued_at":"2026-05-18T02:32:37.794674Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:32:37.794674Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1411.7526","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":"2026-05-18T02:32:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kbDkyJ+kQaMvzuHTLkOtpPQkEn2+rRhfCaPHwzHGSteAQ1KpYTubxlWiB/3CaDIgnvVtUdlmwR9FIa71GgcFAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T20:43:05.556255Z"},"content_sha256":"cdd3b8120537ff197530c270fafe74d63a96ed017fbdd69882958b1c6b1dd437","schema_version":"1.0","event_id":"sha256:cdd3b8120537ff197530c270fafe74d63a96ed017fbdd69882958b1c6b1dd437"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:UDIPFD43YRWQQVXX4H4P2DJNR6","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Modeling the time and energy behavior of the GCR intensity in the periods of low activity around the last three solar minima","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.space-ph"],"primary_cat":"astro-ph.SR","authors_text":"A. K. Svirzhevskaya, G. A. Bazilevskaya, M. B. Krainev, M. S. Kalinin, N. S. Svirzhevsky","submitted_at":"2014-11-27T10:14:33Z","abstract_excerpt":"Using the simple model for the description of the GCR modulation in the heliosphere and the sets of parameters discussed in the accompanying paper we model some features of the time and energy behavior of the GCR intensity near the Earth observed during periods of low solar activity around three last solar minima. In order to understand the mechanisms underlying these features in the GCR behavior, we use the suggested earlier decomposition of the calculated intensity into the partial intensities corresponding to the main processes (diffusion, adiabatic losses, convection and drifts)."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.7526","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":"2026-05-18T02:32:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YnP24/QEKyXNlxJqIiMwpdgHZCgjE1DMa/1iIuREMCCxpyOtlSoML9ENJkdmf9weUkw4TgpdEQvloCzBHvGzAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T20:43:05.557125Z"},"content_sha256":"2a0a67d5544c1179660318e7051b2ccfdfcaa8f7b2835f5941e2b2974d730c16","schema_version":"1.0","event_id":"sha256:2a0a67d5544c1179660318e7051b2ccfdfcaa8f7b2835f5941e2b2974d730c16"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UDIPFD43YRWQQVXX4H4P2DJNR6/bundle.json","state_url":"https://pith.science/pith/UDIPFD43YRWQQVXX4H4P2DJNR6/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UDIPFD43YRWQQVXX4H4P2DJNR6/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":"2026-06-04T20:43:05Z","links":{"resolver":"https://pith.science/pith/UDIPFD43YRWQQVXX4H4P2DJNR6","bundle":"https://pith.science/pith/UDIPFD43YRWQQVXX4H4P2DJNR6/bundle.json","state":"https://pith.science/pith/UDIPFD43YRWQQVXX4H4P2DJNR6/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UDIPFD43YRWQQVXX4H4P2DJNR6/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:UDIPFD43YRWQQVXX4H4P2DJNR6","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":"81d591540c857505492d775e82206e6f93263f3aaf6c6951fbfabb1f4b702ee1","cross_cats_sorted":["physics.space-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.SR","submitted_at":"2014-11-27T10:14:33Z","title_canon_sha256":"9acd9bab1aac14bacfcb46c1c369e89b587ed3b528ca52a9b43cb73c780f4bcc"},"schema_version":"1.0","source":{"id":"1411.7526","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1411.7526","created_at":"2026-05-18T02:32:37Z"},{"alias_kind":"arxiv_version","alias_value":"1411.7526v1","created_at":"2026-05-18T02:32:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.7526","created_at":"2026-05-18T02:32:37Z"},{"alias_kind":"pith_short_12","alias_value":"UDIPFD43YRWQ","created_at":"2026-05-18T12:28:52Z"},{"alias_kind":"pith_short_16","alias_value":"UDIPFD43YRWQQVXX","created_at":"2026-05-18T12:28:52Z"},{"alias_kind":"pith_short_8","alias_value":"UDIPFD43","created_at":"2026-05-18T12:28:52Z"}],"graph_snapshots":[{"event_id":"sha256:2a0a67d5544c1179660318e7051b2ccfdfcaa8f7b2835f5941e2b2974d730c16","target":"graph","created_at":"2026-05-18T02:32:37Z","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":"Using the simple model for the description of the GCR modulation in the heliosphere and the sets of parameters discussed in the accompanying paper we model some features of the time and energy behavior of the GCR intensity near the Earth observed during periods of low solar activity around three last solar minima. In order to understand the mechanisms underlying these features in the GCR behavior, we use the suggested earlier decomposition of the calculated intensity into the partial intensities corresponding to the main processes (diffusion, adiabatic losses, convection and drifts).","authors_text":"A. K. Svirzhevskaya, G. A. Bazilevskaya, M. B. Krainev, M. S. Kalinin, N. S. Svirzhevsky","cross_cats":["physics.space-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.SR","submitted_at":"2014-11-27T10:14:33Z","title":"Modeling the time and energy behavior of the GCR intensity in the periods of low activity around the last three solar minima"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.7526","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:cdd3b8120537ff197530c270fafe74d63a96ed017fbdd69882958b1c6b1dd437","target":"record","created_at":"2026-05-18T02:32:37Z","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":"81d591540c857505492d775e82206e6f93263f3aaf6c6951fbfabb1f4b702ee1","cross_cats_sorted":["physics.space-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.SR","submitted_at":"2014-11-27T10:14:33Z","title_canon_sha256":"9acd9bab1aac14bacfcb46c1c369e89b587ed3b528ca52a9b43cb73c780f4bcc"},"schema_version":"1.0","source":{"id":"1411.7526","kind":"arxiv","version":1}},"canonical_sha256":"a0d0f28f9bc46d0856f7e1f8fd0d2d8faaf71445b42eff97fa35f3e996988634","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a0d0f28f9bc46d0856f7e1f8fd0d2d8faaf71445b42eff97fa35f3e996988634","first_computed_at":"2026-05-18T02:32:37.794674Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:32:37.794674Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"2UVfg+0NSE7ymYa2NJ01Lkq4/aweKDW+PnCDbO6hSeR1LAIkib0Uf84mFqBOZzmKO6JRhFSaCGFoAdalDL25AQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:32:37.795121Z","signed_message":"canonical_sha256_bytes"},"source_id":"1411.7526","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cdd3b8120537ff197530c270fafe74d63a96ed017fbdd69882958b1c6b1dd437","sha256:2a0a67d5544c1179660318e7051b2ccfdfcaa8f7b2835f5941e2b2974d730c16"],"state_sha256":"62b8ebe7b1056738884b0848186e55939222e69f2e6c6e44f3a2b128d8a1d8fe"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"L8iSCokQddkbiC6g5GDdx8I+yTWSgQYEnK/2vrfy78g8lOCNsFV21PJeyRjJOuQkVVTlL6zzukbwNLCSnvSPCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-04T20:43:05.561141Z","bundle_sha256":"f37d4c74d0dbcb318b48ddf60d9006509e1f0601c4efa2518dccd8dd6718b5b6"}}