{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:CJBIZQEYETEIA7JSSZZ4RQM54R","short_pith_number":"pith:CJBIZQEY","canonical_record":{"source":{"id":"1409.8340","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2014-09-29T22:17:21Z","cross_cats_sorted":["cond-mat.mes-hall","physics.comp-ph"],"title_canon_sha256":"61e0aad2bc2d553feb05c066ec49cb69f33796d14cf7003cdc153e1f8f058897","abstract_canon_sha256":"e8c38edce15de44284d5822b77b08e1185cf4396b072b03f211576a236f7e190"},"schema_version":"1.0"},"canonical_sha256":"12428cc09824c8807d329673c8c19de459e192322c1c77ef6595aee5b7133c32","source":{"kind":"arxiv","id":"1409.8340","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.8340","created_at":"2026-05-18T02:16:39Z"},{"alias_kind":"arxiv_version","alias_value":"1409.8340v2","created_at":"2026-05-18T02:16:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.8340","created_at":"2026-05-18T02:16:39Z"},{"alias_kind":"pith_short_12","alias_value":"CJBIZQEYETEI","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_16","alias_value":"CJBIZQEYETEIA7JS","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_8","alias_value":"CJBIZQEY","created_at":"2026-05-18T12:28:22Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:CJBIZQEYETEIA7JSSZZ4RQM54R","target":"record","payload":{"canonical_record":{"source":{"id":"1409.8340","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2014-09-29T22:17:21Z","cross_cats_sorted":["cond-mat.mes-hall","physics.comp-ph"],"title_canon_sha256":"61e0aad2bc2d553feb05c066ec49cb69f33796d14cf7003cdc153e1f8f058897","abstract_canon_sha256":"e8c38edce15de44284d5822b77b08e1185cf4396b072b03f211576a236f7e190"},"schema_version":"1.0"},"canonical_sha256":"12428cc09824c8807d329673c8c19de459e192322c1c77ef6595aee5b7133c32","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:16:39.230419Z","signature_b64":"xJdeSf9HFqbXHeI2Sf3odzlHH59LArJOO1vZ2Jw66rItiL+BmdUMdhrfir1qmpQNFAEDC85LaOrueewewlCuAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"12428cc09824c8807d329673c8c19de459e192322c1c77ef6595aee5b7133c32","last_reissued_at":"2026-05-18T02:16:39.229879Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:16:39.229879Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1409.8340","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:16:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bZYx9je2qRM1eBxnKYNeOd8UCdaY2DATFEywxNs7iakMDlB5Zvn9zpk/NgvwCjAslbTpY5xSaWVLEGlwboZRDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T07:15:05.579216Z"},"content_sha256":"c0057bf148b2148c0658178a48bae58a940168a011519882f523b9ce87a1fede","schema_version":"1.0","event_id":"sha256:c0057bf148b2148c0658178a48bae58a940168a011519882f523b9ce87a1fede"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:CJBIZQEYETEIA7JSSZZ4RQM54R","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Stable large-scale solver for Ginzburg-Landau equations for superconductors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","physics.comp-ph"],"primary_cat":"cond-mat.supr-con","authors_text":"A. E. Koshelev, A. Glatz, C. L. Phillips, D. A. Karpeyev, I. A. Sadovskyy","submitted_at":"2014-09-29T22:17:21Z","abstract_excerpt":"Understanding the interaction of vortices with inclusions in type-II superconductors is a major outstanding challenge both for fundamental science and energy applications. At application-relevant scales, the long-range interactions between a dense configuration of vortices and the dependence of their behavior on external parameters, such as temperature and an applied magnetic field, are all important to the net response of the superconductor. Capturing these features, in general, precludes analytical description of vortex dynamics and has also made numerical simulation prohibitively expensive."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.8340","kind":"arxiv","version":2},"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":"2026-05-18T02:16:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"l2FwJowPEBeyBYm5LIYGqSz7LykFNammiWZ+GiD2LeeoKXAK5M+8Dh/WXqNP0v9H72v2im9RLEH3feUg9ChVCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T07:15:05.579581Z"},"content_sha256":"f043e957db85bda0eb8cc23396428e2459d6c67950282416afbf70d77ee64b45","schema_version":"1.0","event_id":"sha256:f043e957db85bda0eb8cc23396428e2459d6c67950282416afbf70d77ee64b45"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/CJBIZQEYETEIA7JSSZZ4RQM54R/bundle.json","state_url":"https://pith.science/pith/CJBIZQEYETEIA7JSSZZ4RQM54R/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/CJBIZQEYETEIA7JSSZZ4RQM54R/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":"2026-06-02T07:15:05Z","links":{"resolver":"https://pith.science/pith/CJBIZQEYETEIA7JSSZZ4RQM54R","bundle":"https://pith.science/pith/CJBIZQEYETEIA7JSSZZ4RQM54R/bundle.json","state":"https://pith.science/pith/CJBIZQEYETEIA7JSSZZ4RQM54R/state.json","well_known_bundle":"https://pith.science/.well-known/pith/CJBIZQEYETEIA7JSSZZ4RQM54R/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:CJBIZQEYETEIA7JSSZZ4RQM54R","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":"e8c38edce15de44284d5822b77b08e1185cf4396b072b03f211576a236f7e190","cross_cats_sorted":["cond-mat.mes-hall","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2014-09-29T22:17:21Z","title_canon_sha256":"61e0aad2bc2d553feb05c066ec49cb69f33796d14cf7003cdc153e1f8f058897"},"schema_version":"1.0","source":{"id":"1409.8340","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.8340","created_at":"2026-05-18T02:16:39Z"},{"alias_kind":"arxiv_version","alias_value":"1409.8340v2","created_at":"2026-05-18T02:16:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.8340","created_at":"2026-05-18T02:16:39Z"},{"alias_kind":"pith_short_12","alias_value":"CJBIZQEYETEI","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_16","alias_value":"CJBIZQEYETEIA7JS","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_8","alias_value":"CJBIZQEY","created_at":"2026-05-18T12:28:22Z"}],"graph_snapshots":[{"event_id":"sha256:f043e957db85bda0eb8cc23396428e2459d6c67950282416afbf70d77ee64b45","target":"graph","created_at":"2026-05-18T02:16:39Z","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":"Understanding the interaction of vortices with inclusions in type-II superconductors is a major outstanding challenge both for fundamental science and energy applications. At application-relevant scales, the long-range interactions between a dense configuration of vortices and the dependence of their behavior on external parameters, such as temperature and an applied magnetic field, are all important to the net response of the superconductor. Capturing these features, in general, precludes analytical description of vortex dynamics and has also made numerical simulation prohibitively expensive.","authors_text":"A. E. Koshelev, A. Glatz, C. L. Phillips, D. A. Karpeyev, I. A. Sadovskyy","cross_cats":["cond-mat.mes-hall","physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2014-09-29T22:17:21Z","title":"Stable large-scale solver for Ginzburg-Landau equations for superconductors"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.8340","kind":"arxiv","version":2},"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:c0057bf148b2148c0658178a48bae58a940168a011519882f523b9ce87a1fede","target":"record","created_at":"2026-05-18T02:16:39Z","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":"e8c38edce15de44284d5822b77b08e1185cf4396b072b03f211576a236f7e190","cross_cats_sorted":["cond-mat.mes-hall","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2014-09-29T22:17:21Z","title_canon_sha256":"61e0aad2bc2d553feb05c066ec49cb69f33796d14cf7003cdc153e1f8f058897"},"schema_version":"1.0","source":{"id":"1409.8340","kind":"arxiv","version":2}},"canonical_sha256":"12428cc09824c8807d329673c8c19de459e192322c1c77ef6595aee5b7133c32","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"12428cc09824c8807d329673c8c19de459e192322c1c77ef6595aee5b7133c32","first_computed_at":"2026-05-18T02:16:39.229879Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:16:39.229879Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"xJdeSf9HFqbXHeI2Sf3odzlHH59LArJOO1vZ2Jw66rItiL+BmdUMdhrfir1qmpQNFAEDC85LaOrueewewlCuAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:16:39.230419Z","signed_message":"canonical_sha256_bytes"},"source_id":"1409.8340","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c0057bf148b2148c0658178a48bae58a940168a011519882f523b9ce87a1fede","sha256:f043e957db85bda0eb8cc23396428e2459d6c67950282416afbf70d77ee64b45"],"state_sha256":"c09e5d5e18b3e9f125460e35c73d869bb82f74f2a3c8e020f202afb8a08085e7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pVtSBeM9yiv8pXJ1S07xwptfxEKFzKW7amnDnZGXubggd9RF3G8GnsoFFf+0bGuBSt9TDz4uXIB97yG2Rw32Dg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T07:15:05.581570Z","bundle_sha256":"75706230a91ce4b1d09660ebe552da31a06a61d0096c807da377d85abb72d16f"}}