{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:GBQDVBSH5DRR5ZBVUR2B6KJUSV","short_pith_number":"pith:GBQDVBSH","schema_version":"1.0","canonical_sha256":"30603a8647e8e31ee435a4741f2934954cffee495e7b09b360359d385ca900f3","source":{"kind":"arxiv","id":"1105.5524","version":1},"attestation_state":"computed","paper":{"title":"The Properties of the Superconducting State in YNi2B2C: The One-Band Eliashberg Approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"M.W. Jarosik, R. Szczesniak","submitted_at":"2011-05-27T10:58:48Z","abstract_excerpt":"The basic thermodynamic parameters of the superconducting state in $\\rm{YNi_{2}B_{2}C}$ were calculated in the framework of the one-band Eliashberg model. The effective Eliashberg function, determined on the basis of the transport function (R.S. Gonnelli, {\\it et al.}, Physica C \\textbf{341}, 1957 (2000)), was used during calculations. It was shown that the dimensionless ratios are equal to: $R_{1}\\equiv 2\\Delta(0)/k_{B}T_{C}=3.87$, $R_{2}\\equiv\\Delta C(T_{C})/C^{N}(T_{C})=1.79$ and $R_{3}\\equiv T_{C}C^{N}(T_{C})/H_{C}^{2}(0)=0.159$. The value $R_{1}$ fairly agrees with the experimental data w"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1105.5524","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2011-05-27T10:58:48Z","cross_cats_sorted":[],"title_canon_sha256":"fbcdcd3b8c2c56bad37751f3e7cce563c8476ff71fcbb80e7c05f0b006f3e53f","abstract_canon_sha256":"33bf28070ce28e5062147548f48b9a0cb436e003ba66d310df5515da195060b9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:36:16.723705Z","signature_b64":"4dkK1HvTxuHPb3xXxu6mQSIeFbXTg5z9fJKVyE+ny3YeGjhZTm4BMu9hTZ3R349gpHtF3nnDTlpQW6FW8IRsCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"30603a8647e8e31ee435a4741f2934954cffee495e7b09b360359d385ca900f3","last_reissued_at":"2026-05-18T03:36:16.722926Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:36:16.722926Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Properties of the Superconducting State in YNi2B2C: The One-Band Eliashberg Approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"M.W. Jarosik, R. Szczesniak","submitted_at":"2011-05-27T10:58:48Z","abstract_excerpt":"The basic thermodynamic parameters of the superconducting state in $\\rm{YNi_{2}B_{2}C}$ were calculated in the framework of the one-band Eliashberg model. The effective Eliashberg function, determined on the basis of the transport function (R.S. Gonnelli, {\\it et al.}, Physica C \\textbf{341}, 1957 (2000)), was used during calculations. It was shown that the dimensionless ratios are equal to: $R_{1}\\equiv 2\\Delta(0)/k_{B}T_{C}=3.87$, $R_{2}\\equiv\\Delta C(T_{C})/C^{N}(T_{C})=1.79$ and $R_{3}\\equiv T_{C}C^{N}(T_{C})/H_{C}^{2}(0)=0.159$. 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