{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:USKAIMISVT4F4EPVN2YXXA4R24","short_pith_number":"pith:USKAIMIS","schema_version":"1.0","canonical_sha256":"a494043112acf85e11f56eb17b8391d7020fa034f7300ad10ac0ae8a42c2ed19","source":{"kind":"arxiv","id":"1106.2405","version":3},"attestation_state":"computed","paper":{"title":"Superconducting transitions of intrinsic arrays of weakly coupled 1D superconducting chains: The case of the extreme quasi-1D superconductor Tl2Mo6Se6","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"A. P. Petrovi\\'c, B. Bergk, D. Salloum, M. Potel, P. Gougeon, R. Lortz, Y. Wang, Z. Wang","submitted_at":"2011-06-13T09:43:54Z","abstract_excerpt":"Tl2Mo6Se6 represents a model system for quasi-one-dimensional superconductors. We investigate its superconducting transition in detail by means of electrical transport experiments on high-quality single crystalline samples with onset Tc = 6.8 K. Our measurements indicate a highly complex superconducting transition which occurs in different stages, with a characteristic bump in the resistivity and distinct plateau structures in the supercurrent gap imaged by V-I curves. We interpret these features as fingerprints of the gradual establishment of global phase coherence in an array of weakly coupl"},"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":"1106.2405","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2011-06-13T09:43:54Z","cross_cats_sorted":[],"title_canon_sha256":"899115b07b154bf8f0c613473f7dbc293bfc83f2a59bab27d64eba10902ef414","abstract_canon_sha256":"950b2dee44575032971b0e9406e4ece6c51f2e35e06a8c4d168a38b1cde62e93"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:01:39.450385Z","signature_b64":"urA3JCIE0KEXSwZZ5SRrKa0Y3pnu8T1mx5pEsDhtBw+Q/2ZQhv1xUZJJwQN4K95LAZqYZuCzu/0pFWcD1OugDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a494043112acf85e11f56eb17b8391d7020fa034f7300ad10ac0ae8a42c2ed19","last_reissued_at":"2026-05-18T02:01:39.449874Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:01:39.449874Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Superconducting transitions of intrinsic arrays of weakly coupled 1D superconducting chains: The case of the extreme quasi-1D superconductor Tl2Mo6Se6","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"A. P. Petrovi\\'c, B. Bergk, D. Salloum, M. Potel, P. Gougeon, R. Lortz, Y. Wang, Z. Wang","submitted_at":"2011-06-13T09:43:54Z","abstract_excerpt":"Tl2Mo6Se6 represents a model system for quasi-one-dimensional superconductors. We investigate its superconducting transition in detail by means of electrical transport experiments on high-quality single crystalline samples with onset Tc = 6.8 K. Our measurements indicate a highly complex superconducting transition which occurs in different stages, with a characteristic bump in the resistivity and distinct plateau structures in the supercurrent gap imaged by V-I curves. We interpret these features as fingerprints of the gradual establishment of global phase coherence in an array of weakly coupl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.2405","kind":"arxiv","version":3},"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":"1106.2405","created_at":"2026-05-18T02:01:39.449938+00:00"},{"alias_kind":"arxiv_version","alias_value":"1106.2405v3","created_at":"2026-05-18T02:01:39.449938+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.2405","created_at":"2026-05-18T02:01:39.449938+00:00"},{"alias_kind":"pith_short_12","alias_value":"USKAIMISVT4F","created_at":"2026-05-18T12:26:42.757692+00:00"},{"alias_kind":"pith_short_16","alias_value":"USKAIMISVT4F4EPV","created_at":"2026-05-18T12:26:42.757692+00:00"},{"alias_kind":"pith_short_8","alias_value":"USKAIMIS","created_at":"2026-05-18T12:26:42.757692+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/USKAIMISVT4F4EPVN2YXXA4R24","json":"https://pith.science/pith/USKAIMISVT4F4EPVN2YXXA4R24.json","graph_json":"https://pith.science/api/pith-number/USKAIMISVT4F4EPVN2YXXA4R24/graph.json","events_json":"https://pith.science/api/pith-number/USKAIMISVT4F4EPVN2YXXA4R24/events.json","paper":"https://pith.science/paper/USKAIMIS"},"agent_actions":{"view_html":"https://pith.science/pith/USKAIMISVT4F4EPVN2YXXA4R24","download_json":"https://pith.science/pith/USKAIMISVT4F4EPVN2YXXA4R24.json","view_paper":"https://pith.science/paper/USKAIMIS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1106.2405&json=true","fetch_graph":"https://pith.science/api/pith-number/USKAIMISVT4F4EPVN2YXXA4R24/graph.json","fetch_events":"https://pith.science/api/pith-number/USKAIMISVT4F4EPVN2YXXA4R24/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/USKAIMISVT4F4EPVN2YXXA4R24/action/timestamp_anchor","attest_storage":"https://pith.science/pith/USKAIMISVT4F4EPVN2YXXA4R24/action/storage_attestation","attest_author":"https://pith.science/pith/USKAIMISVT4F4EPVN2YXXA4R24/action/author_attestation","sign_citation":"https://pith.science/pith/USKAIMISVT4F4EPVN2YXXA4R24/action/citation_signature","submit_replication":"https://pith.science/pith/USKAIMISVT4F4EPVN2YXXA4R24/action/replication_record"}},"created_at":"2026-05-18T02:01:39.449938+00:00","updated_at":"2026-05-18T02:01:39.449938+00:00"}