{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2020:DKZKPHSTPTRYNOZUFXTHAJ6QTV","short_pith_number":"pith:DKZKPHST","canonical_record":{"source":{"id":"2003.01399","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2020-03-03T09:27:10Z","cross_cats_sorted":["cond-mat.supr-con"],"title_canon_sha256":"2a3b50c6cfa7b2a4519a726eff4ceecce7b914870a69b1c31f6f33ce5acf95fc","abstract_canon_sha256":"e53b6f5bb1120d23960e3252b95d5ab608a8e477d1cfa55da88816e1a89779f3"},"schema_version":"1.0"},"canonical_sha256":"1ab2a79e537ce386bb342de67027d09d43a39679604ebd11e2a443fa10d3ba5e","source":{"kind":"arxiv","id":"2003.01399","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2003.01399","created_at":"2026-07-05T02:02:32Z"},{"alias_kind":"arxiv_version","alias_value":"2003.01399v1","created_at":"2026-07-05T02:02:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2003.01399","created_at":"2026-07-05T02:02:32Z"},{"alias_kind":"pith_short_12","alias_value":"DKZKPHSTPTRY","created_at":"2026-07-05T02:02:32Z"},{"alias_kind":"pith_short_16","alias_value":"DKZKPHSTPTRYNOZU","created_at":"2026-07-05T02:02:32Z"},{"alias_kind":"pith_short_8","alias_value":"DKZKPHST","created_at":"2026-07-05T02:02:32Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2020:DKZKPHSTPTRYNOZUFXTHAJ6QTV","target":"record","payload":{"canonical_record":{"source":{"id":"2003.01399","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2020-03-03T09:27:10Z","cross_cats_sorted":["cond-mat.supr-con"],"title_canon_sha256":"2a3b50c6cfa7b2a4519a726eff4ceecce7b914870a69b1c31f6f33ce5acf95fc","abstract_canon_sha256":"e53b6f5bb1120d23960e3252b95d5ab608a8e477d1cfa55da88816e1a89779f3"},"schema_version":"1.0"},"canonical_sha256":"1ab2a79e537ce386bb342de67027d09d43a39679604ebd11e2a443fa10d3ba5e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:02:32.737949Z","signature_b64":"Ubwy/I9baJsw15FYOhIH2go3WDcdmZEVb1qwf/xlG/umbwSqrpRTqwbKeqn+iKXV/lW1UYwKKugMS6NpizWjBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1ab2a79e537ce386bb342de67027d09d43a39679604ebd11e2a443fa10d3ba5e","last_reissued_at":"2026-07-05T02:02:32.737497Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:02:32.737497Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2003.01399","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":"2026-07-05T02:02:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hiwuEjAU+5DiGH/jRPm0NYR6iNkTROeG+mGrwKO/n1pJn4tXoaDa9IcNmObHTCGwaE4vlvc5Dd4kY2vcJ3taAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T21:12:19.302276Z"},"content_sha256":"2f86bee77d606780d7ebd16336a692f86e7bd6e532d326ae7aa868acad448ed8","schema_version":"1.0","event_id":"sha256:2f86bee77d606780d7ebd16336a692f86e7bd6e532d326ae7aa868acad448ed8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2020:DKZKPHSTPTRYNOZUFXTHAJ6QTV","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Current density distribution in resistive fault current limiters and its effect on device stability","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con"],"primary_cat":"physics.app-ph","authors_text":"Abdollah Kavousi-Fard, Mehdi Hosseini, Mohammad Farokhiyan","submitted_at":"2020-03-03T09:27:10Z","abstract_excerpt":"The increase of current uniformity along of a resistive type superconductor fault current limiter (R-SFCL) in the design of this type of limiters is well perceived as an important issue. The non-uniform distribution of current in R-SFCL only increases the current in some superconducting regions, as a result, in the fault conditions, only certain parts of the superconductor undergo a phase change that increases the heat pressure in those areas and causes the breakdown and destruction of the device. In this paper, the current density distributions in common patterns used in R-SFCs constructions "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2003.01399","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2003.01399/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-05T02:02:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KztxKA/Yio0ccBnXM0OqmXegZxF95FnTLM/HwmR5Dtjja7Wt3bPFTj3eE7taTg9BbYxwc+MIurNNrqMvwI1yBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T21:12:19.302663Z"},"content_sha256":"d53268796a35faa954c660e24ceadb709751ad4ccbb67b2b468d3b66ed75cd3c","schema_version":"1.0","event_id":"sha256:d53268796a35faa954c660e24ceadb709751ad4ccbb67b2b468d3b66ed75cd3c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DKZKPHSTPTRYNOZUFXTHAJ6QTV/bundle.json","state_url":"https://pith.science/pith/DKZKPHSTPTRYNOZUFXTHAJ6QTV/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DKZKPHSTPTRYNOZUFXTHAJ6QTV/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":"2026-08-03T21:12:19Z","links":{"resolver":"https://pith.science/pith/DKZKPHSTPTRYNOZUFXTHAJ6QTV","bundle":"https://pith.science/pith/DKZKPHSTPTRYNOZUFXTHAJ6QTV/bundle.json","state":"https://pith.science/pith/DKZKPHSTPTRYNOZUFXTHAJ6QTV/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DKZKPHSTPTRYNOZUFXTHAJ6QTV/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2020:DKZKPHSTPTRYNOZUFXTHAJ6QTV","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":"e53b6f5bb1120d23960e3252b95d5ab608a8e477d1cfa55da88816e1a89779f3","cross_cats_sorted":["cond-mat.supr-con"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2020-03-03T09:27:10Z","title_canon_sha256":"2a3b50c6cfa7b2a4519a726eff4ceecce7b914870a69b1c31f6f33ce5acf95fc"},"schema_version":"1.0","source":{"id":"2003.01399","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2003.01399","created_at":"2026-07-05T02:02:32Z"},{"alias_kind":"arxiv_version","alias_value":"2003.01399v1","created_at":"2026-07-05T02:02:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2003.01399","created_at":"2026-07-05T02:02:32Z"},{"alias_kind":"pith_short_12","alias_value":"DKZKPHSTPTRY","created_at":"2026-07-05T02:02:32Z"},{"alias_kind":"pith_short_16","alias_value":"DKZKPHSTPTRYNOZU","created_at":"2026-07-05T02:02:32Z"},{"alias_kind":"pith_short_8","alias_value":"DKZKPHST","created_at":"2026-07-05T02:02:32Z"}],"graph_snapshots":[{"event_id":"sha256:d53268796a35faa954c660e24ceadb709751ad4ccbb67b2b468d3b66ed75cd3c","target":"graph","created_at":"2026-07-05T02:02:32Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2003.01399/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The increase of current uniformity along of a resistive type superconductor fault current limiter (R-SFCL) in the design of this type of limiters is well perceived as an important issue. The non-uniform distribution of current in R-SFCL only increases the current in some superconducting regions, as a result, in the fault conditions, only certain parts of the superconductor undergo a phase change that increases the heat pressure in those areas and causes the breakdown and destruction of the device. In this paper, the current density distributions in common patterns used in R-SFCs constructions ","authors_text":"Abdollah Kavousi-Fard, Mehdi Hosseini, Mohammad Farokhiyan","cross_cats":["cond-mat.supr-con"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2020-03-03T09:27:10Z","title":"Current density distribution in resistive fault current limiters and its effect on device stability"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2003.01399","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":"sha256:2f86bee77d606780d7ebd16336a692f86e7bd6e532d326ae7aa868acad448ed8","target":"record","created_at":"2026-07-05T02:02:32Z","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":"e53b6f5bb1120d23960e3252b95d5ab608a8e477d1cfa55da88816e1a89779f3","cross_cats_sorted":["cond-mat.supr-con"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2020-03-03T09:27:10Z","title_canon_sha256":"2a3b50c6cfa7b2a4519a726eff4ceecce7b914870a69b1c31f6f33ce5acf95fc"},"schema_version":"1.0","source":{"id":"2003.01399","kind":"arxiv","version":1}},"canonical_sha256":"1ab2a79e537ce386bb342de67027d09d43a39679604ebd11e2a443fa10d3ba5e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1ab2a79e537ce386bb342de67027d09d43a39679604ebd11e2a443fa10d3ba5e","first_computed_at":"2026-07-05T02:02:32.737497Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T02:02:32.737497Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Ubwy/I9baJsw15FYOhIH2go3WDcdmZEVb1qwf/xlG/umbwSqrpRTqwbKeqn+iKXV/lW1UYwKKugMS6NpizWjBQ==","signature_status":"signed_v1","signed_at":"2026-07-05T02:02:32.737949Z","signed_message":"canonical_sha256_bytes"},"source_id":"2003.01399","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2f86bee77d606780d7ebd16336a692f86e7bd6e532d326ae7aa868acad448ed8","sha256:d53268796a35faa954c660e24ceadb709751ad4ccbb67b2b468d3b66ed75cd3c"],"state_sha256":"57ebd4c85bfb2e067d89f96259da70715367629b379c51daa773ec893aac732c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"I1hUr5DSSbCEDQWQtnggI5Afn1l4rjQ5UgIQvNgJu+krD3aBzDkCwGu/7ALUc8CN2Oil4FQerzUeN0WrY2MYAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-03T21:12:19.305502Z","bundle_sha256":"2f0cf982e98a39b142dcadde9ee3ef45b8329cffd1be6511a0c3f38f2c2eba7f"}}