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Our work was motivated by Klein \\emph{et. al}, \"Thermodynamic phase diagram of Fe(Se$_{0.5}$Te$_{0.5}$) single crystals in fields up to 28 Tesla\", Phys. Rev. B 82, 184506 (2010). In their paper, Klein et al. have attributed a factor of five difference in the value of the London penetration depth obtained from their tunnel diode resonator (TDR) measurements and calculated from"},"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":"1207.3542","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2012-07-15T21:11:02Z","cross_cats_sorted":[],"title_canon_sha256":"06fb5b56f4687ddff1f052f5a583b244d5eaeb52149102767f25cb8840051ea3","abstract_canon_sha256":"7668a5bc15b9f1d06041a9112c6e81fb177baaaa42f7deb7f6fced21e65161b3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:56:18.319944Z","signature_b64":"t1+NU/TvDrD/YwKJixos9baCcTwGsCKHQtggZ9rL/iJyPgSmKfmaezd8Y+cV/Z4xi2gyANoedLACEiPMSn8sAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6a214c3b4f5c6bcf30e7f07b5e237e3453f83d8b18595c3d3242eab64b14e767","last_reissued_at":"2026-05-18T01:56:18.319435Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:56:18.319435Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Reply to \"Comment on \\emph{\"Precision global measurements of London penetration depth in Fe(Te$_{0.58}$Se$_{0.42}$)\"}\"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"H. Kim, K. Cho, M. A. Tanatar, R. Prozorov","submitted_at":"2012-07-15T21:11:02Z","abstract_excerpt":"We reply to the Comment by T. Klein, P. Rodi\\`{e}re and C. Marcenat (arXiv:1205.2566), on our paper, \"Precision global measurements of London penetration depth in FeTe$_{0.58}$Se$_{0.42}$\", Phys. Rev. B 84, 174502 (2011). Our work was motivated by Klein \\emph{et. al}, \"Thermodynamic phase diagram of Fe(Se$_{0.5}$Te$_{0.5}$) single crystals in fields up to 28 Tesla\", Phys. Rev. B 82, 184506 (2010). In their paper, Klein et al. have attributed a factor of five difference in the value of the London penetration depth obtained from their tunnel diode resonator (TDR) measurements and calculated from"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.3542","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1207.3542","created_at":"2026-05-18T01:56:18.319523+00:00"},{"alias_kind":"arxiv_version","alias_value":"1207.3542v1","created_at":"2026-05-18T01:56:18.319523+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.3542","created_at":"2026-05-18T01:56:18.319523+00:00"},{"alias_kind":"pith_short_12","alias_value":"NIQUYO2PLRV4","created_at":"2026-05-18T12:27:16.716162+00:00"},{"alias_kind":"pith_short_16","alias_value":"NIQUYO2PLRV46MHH","created_at":"2026-05-18T12:27:16.716162+00:00"},{"alias_kind":"pith_short_8","alias_value":"NIQUYO2P","created_at":"2026-05-18T12:27:16.716162+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NIQUYO2PLRV46MHH6B5V4I36GR","json":"https://pith.science/pith/NIQUYO2PLRV46MHH6B5V4I36GR.json","graph_json":"https://pith.science/api/pith-number/NIQUYO2PLRV46MHH6B5V4I36GR/graph.json","events_json":"https://pith.science/api/pith-number/NIQUYO2PLRV46MHH6B5V4I36GR/events.json","paper":"https://pith.science/paper/NIQUYO2P"},"agent_actions":{"view_html":"https://pith.science/pith/NIQUYO2PLRV46MHH6B5V4I36GR","download_json":"https://pith.science/pith/NIQUYO2PLRV46MHH6B5V4I36GR.json","view_paper":"https://pith.science/paper/NIQUYO2P","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1207.3542&json=true","fetch_graph":"https://pith.science/api/pith-number/NIQUYO2PLRV46MHH6B5V4I36GR/graph.json","fetch_events":"https://pith.science/api/pith-number/NIQUYO2PLRV46MHH6B5V4I36GR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NIQUYO2PLRV46MHH6B5V4I36GR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NIQUYO2PLRV46MHH6B5V4I36GR/action/storage_attestation","attest_author":"https://pith.science/pith/NIQUYO2PLRV46MHH6B5V4I36GR/action/author_attestation","sign_citation":"https://pith.science/pith/NIQUYO2PLRV46MHH6B5V4I36GR/action/citation_signature","submit_replication":"https://pith.science/pith/NIQUYO2PLRV46MHH6B5V4I36GR/action/replication_record"}},"created_at":"2026-05-18T01:56:18.319523+00:00","updated_at":"2026-05-18T01:56:18.319523+00:00"}