{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:6LUQ2PQEOZD73TWN7V4OMKPRBC","short_pith_number":"pith:6LUQ2PQE","canonical_record":{"source":{"id":"1406.6790","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2014-06-26T07:15:15Z","cross_cats_sorted":[],"title_canon_sha256":"7d3b24b8ef4057fa7a6e6337154af649ffd27b23423729b3072675802d15b17c","abstract_canon_sha256":"5edd6e98e3f7ee404e423877a81a3fc1c32fd43de88f68a60910e2fa3751ea35"},"schema_version":"1.0"},"canonical_sha256":"f2e90d3e047647fdcecdfd78e629f108a10e296fa2ad6a823bd0aa39e4a1c5a3","source":{"kind":"arxiv","id":"1406.6790","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1406.6790","created_at":"2026-05-18T01:37:07Z"},{"alias_kind":"arxiv_version","alias_value":"1406.6790v2","created_at":"2026-05-18T01:37:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1406.6790","created_at":"2026-05-18T01:37:07Z"},{"alias_kind":"pith_short_12","alias_value":"6LUQ2PQEOZD7","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_16","alias_value":"6LUQ2PQEOZD73TWN","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_8","alias_value":"6LUQ2PQE","created_at":"2026-05-18T12:28:16Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:6LUQ2PQEOZD73TWN7V4OMKPRBC","target":"record","payload":{"canonical_record":{"source":{"id":"1406.6790","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2014-06-26T07:15:15Z","cross_cats_sorted":[],"title_canon_sha256":"7d3b24b8ef4057fa7a6e6337154af649ffd27b23423729b3072675802d15b17c","abstract_canon_sha256":"5edd6e98e3f7ee404e423877a81a3fc1c32fd43de88f68a60910e2fa3751ea35"},"schema_version":"1.0"},"canonical_sha256":"f2e90d3e047647fdcecdfd78e629f108a10e296fa2ad6a823bd0aa39e4a1c5a3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:37:07.881169Z","signature_b64":"l9iU3SNo/M/vyReEPE8qcn6qNjj6AMglbALlb+Ls6dRAOeZR4jao141aeiagNRPhflgxpSeVPTkqWkWftjwhDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f2e90d3e047647fdcecdfd78e629f108a10e296fa2ad6a823bd0aa39e4a1c5a3","last_reissued_at":"2026-05-18T01:37:07.880636Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:37:07.880636Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1406.6790","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":"2026-05-18T01:37:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hsT4cUM6W8xqSNsIyH1pKyTyEtMxN1iEuvzkSQHkHx3auOHtbO9uI58gmzMRrgehdcKzqvAwcb0vH78LhymQAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T23:32:05.037045Z"},"content_sha256":"05371cce43cdd3591d07af6b3ba2f54cc4e56c7fa778e57b58ca3e63da0539cb","schema_version":"1.0","event_id":"sha256:05371cce43cdd3591d07af6b3ba2f54cc4e56c7fa778e57b58ca3e63da0539cb"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:6LUQ2PQEOZD73TWN7V4OMKPRBC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Growth and angular dependent resistivity of Nb2Pd0.73S5.7 superconducting single crystals fiber","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Ajay D. Thakur, Anil K. Yadav, C. V. Tomy, Himanshu Sharma","submitted_at":"2014-06-26T07:15:15Z","abstract_excerpt":"We report the growth of Nb2Pd0.73S5.7 superconducting single crystal fibers via slow cooling solid state reaction method. Superconducting transition temperature (Tc ~ 6.5K) is confirmed from magnetization and transport measurements. A comparative study is performed for determination of superconducting anisotropy, {\\Gamma}, via conventional method (by taking ration of two superconducting parameters) and scaling approach method. Scaling approach, defined within the framework of the Ginzburg-Landau theory is applied to the angular dependent resistivity measurements to estimate the anisotropy. The"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1406.6790","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":"2026-05-18T01:37:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RJTf1UWzhi5Pkepsu4eKVmla345loRwKePB3Idfetb4nAzQpkzrTeVgGQHHlQi7hKG4YJVfwy7d/1A2YarLhCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T23:32:05.037393Z"},"content_sha256":"f7ff2097038abb5bbc583b85a5265b71dd0f9f6ba5f97da797c7827908c7ced8","schema_version":"1.0","event_id":"sha256:f7ff2097038abb5bbc583b85a5265b71dd0f9f6ba5f97da797c7827908c7ced8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6LUQ2PQEOZD73TWN7V4OMKPRBC/bundle.json","state_url":"https://pith.science/pith/6LUQ2PQEOZD73TWN7V4OMKPRBC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6LUQ2PQEOZD73TWN7V4OMKPRBC/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":"2026-06-01T23:32:05Z","links":{"resolver":"https://pith.science/pith/6LUQ2PQEOZD73TWN7V4OMKPRBC","bundle":"https://pith.science/pith/6LUQ2PQEOZD73TWN7V4OMKPRBC/bundle.json","state":"https://pith.science/pith/6LUQ2PQEOZD73TWN7V4OMKPRBC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6LUQ2PQEOZD73TWN7V4OMKPRBC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:6LUQ2PQEOZD73TWN7V4OMKPRBC","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":"5edd6e98e3f7ee404e423877a81a3fc1c32fd43de88f68a60910e2fa3751ea35","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2014-06-26T07:15:15Z","title_canon_sha256":"7d3b24b8ef4057fa7a6e6337154af649ffd27b23423729b3072675802d15b17c"},"schema_version":"1.0","source":{"id":"1406.6790","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1406.6790","created_at":"2026-05-18T01:37:07Z"},{"alias_kind":"arxiv_version","alias_value":"1406.6790v2","created_at":"2026-05-18T01:37:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1406.6790","created_at":"2026-05-18T01:37:07Z"},{"alias_kind":"pith_short_12","alias_value":"6LUQ2PQEOZD7","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_16","alias_value":"6LUQ2PQEOZD73TWN","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_8","alias_value":"6LUQ2PQE","created_at":"2026-05-18T12:28:16Z"}],"graph_snapshots":[{"event_id":"sha256:f7ff2097038abb5bbc583b85a5265b71dd0f9f6ba5f97da797c7827908c7ced8","target":"graph","created_at":"2026-05-18T01:37:07Z","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":"We report the growth of Nb2Pd0.73S5.7 superconducting single crystal fibers via slow cooling solid state reaction method. Superconducting transition temperature (Tc ~ 6.5K) is confirmed from magnetization and transport measurements. A comparative study is performed for determination of superconducting anisotropy, {\\Gamma}, via conventional method (by taking ration of two superconducting parameters) and scaling approach method. Scaling approach, defined within the framework of the Ginzburg-Landau theory is applied to the angular dependent resistivity measurements to estimate the anisotropy. The","authors_text":"Ajay D. Thakur, Anil K. Yadav, C. V. Tomy, Himanshu Sharma","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2014-06-26T07:15:15Z","title":"Growth and angular dependent resistivity of Nb2Pd0.73S5.7 superconducting single crystals fiber"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1406.6790","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":"sha256:05371cce43cdd3591d07af6b3ba2f54cc4e56c7fa778e57b58ca3e63da0539cb","target":"record","created_at":"2026-05-18T01:37:07Z","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":"5edd6e98e3f7ee404e423877a81a3fc1c32fd43de88f68a60910e2fa3751ea35","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2014-06-26T07:15:15Z","title_canon_sha256":"7d3b24b8ef4057fa7a6e6337154af649ffd27b23423729b3072675802d15b17c"},"schema_version":"1.0","source":{"id":"1406.6790","kind":"arxiv","version":2}},"canonical_sha256":"f2e90d3e047647fdcecdfd78e629f108a10e296fa2ad6a823bd0aa39e4a1c5a3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f2e90d3e047647fdcecdfd78e629f108a10e296fa2ad6a823bd0aa39e4a1c5a3","first_computed_at":"2026-05-18T01:37:07.880636Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:37:07.880636Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"l9iU3SNo/M/vyReEPE8qcn6qNjj6AMglbALlb+Ls6dRAOeZR4jao141aeiagNRPhflgxpSeVPTkqWkWftjwhDg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:37:07.881169Z","signed_message":"canonical_sha256_bytes"},"source_id":"1406.6790","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:05371cce43cdd3591d07af6b3ba2f54cc4e56c7fa778e57b58ca3e63da0539cb","sha256:f7ff2097038abb5bbc583b85a5265b71dd0f9f6ba5f97da797c7827908c7ced8"],"state_sha256":"62e3d411ae77f48d51c260378e4098c7cf0994358023803f5032496b22d6b8d9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CSwbIT6fNFgIeabeFMC/N3yqbFPSQ3jB8Um/unytd9NngI32Rvsgpsae2uIHR/9+NmKB0u4X29JDOWUYoK0GAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T23:32:05.039207Z","bundle_sha256":"1e95be9ec1e31f429952d1b70ee77d13a6f5144efb093acfd02da12ce449facb"}}