{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:YOU2DDXHGBKOBKBDZWVWDBEOCT","short_pith_number":"pith:YOU2DDXH","schema_version":"1.0","canonical_sha256":"c3a9a18ee73054e0a823cdab61848e14e459c854873e0da5ad7463f41a25ff5c","source":{"kind":"arxiv","id":"1105.0924","version":2},"attestation_state":"computed","paper":{"title":"Critical temperature and Ginzburg region near a quantum critical point in two-dimensional metals","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.str-el","authors_text":"J. Bauer, P. Jakubczyk, W. Metzner","submitted_at":"2011-05-04T20:05:16Z","abstract_excerpt":"We compute the transition temperature $T_c$ and the Ginzburg temperature $T_{\\rm G}$ above $T_c$ near a quantum critical point at the boundary of an ordered phase with a broken discrete symmetry in a two-dimensional metallic electron system. Our calculation is based on a renormalization group analysis of the Hertz action with a scalar order parameter. We provide analytic expressions for $T_c$ and $T_{\\rm G}$ as a function of the non-thermal control parameter for the quantum phase transition, including logarithmic corrections. The Ginzburg regime between $T_c$ and $T_{\\rm G}$ occupies a sizable"},"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":"1105.0924","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-05-04T20:05:16Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"c9c1ae0b0ac4e1d34c6e22b63b10276358dd627830777adce525d5748fadcdbd","abstract_canon_sha256":"38b6a333cf5d9bed15bad44c60321bd7acfd369aba318c8b9857d9c3727b769f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:15:18.562206Z","signature_b64":"rWiA2exaQWxDkuMCYeLtsNjWvVpbq2q2A7yPTS4K2ifVqJlvl9jzZ1NdPBjTHg+r4vkNfVFYSHDdU5+xw4mmAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c3a9a18ee73054e0a823cdab61848e14e459c854873e0da5ad7463f41a25ff5c","last_reissued_at":"2026-05-18T04:15:18.561560Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:15:18.561560Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Critical temperature and Ginzburg region near a quantum critical point in two-dimensional metals","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.str-el","authors_text":"J. Bauer, P. Jakubczyk, W. Metzner","submitted_at":"2011-05-04T20:05:16Z","abstract_excerpt":"We compute the transition temperature $T_c$ and the Ginzburg temperature $T_{\\rm G}$ above $T_c$ near a quantum critical point at the boundary of an ordered phase with a broken discrete symmetry in a two-dimensional metallic electron system. Our calculation is based on a renormalization group analysis of the Hertz action with a scalar order parameter. We provide analytic expressions for $T_c$ and $T_{\\rm G}$ as a function of the non-thermal control parameter for the quantum phase transition, including logarithmic corrections. The Ginzburg regime between $T_c$ and $T_{\\rm G}$ occupies a sizable"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.0924","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1105.0924","created_at":"2026-05-18T04:15:18.561664+00:00"},{"alias_kind":"arxiv_version","alias_value":"1105.0924v2","created_at":"2026-05-18T04:15:18.561664+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.0924","created_at":"2026-05-18T04:15:18.561664+00:00"},{"alias_kind":"pith_short_12","alias_value":"YOU2DDXHGBKO","created_at":"2026-05-18T12:26:47.523578+00:00"},{"alias_kind":"pith_short_16","alias_value":"YOU2DDXHGBKOBKBD","created_at":"2026-05-18T12:26:47.523578+00:00"},{"alias_kind":"pith_short_8","alias_value":"YOU2DDXH","created_at":"2026-05-18T12:26:47.523578+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/YOU2DDXHGBKOBKBDZWVWDBEOCT","json":"https://pith.science/pith/YOU2DDXHGBKOBKBDZWVWDBEOCT.json","graph_json":"https://pith.science/api/pith-number/YOU2DDXHGBKOBKBDZWVWDBEOCT/graph.json","events_json":"https://pith.science/api/pith-number/YOU2DDXHGBKOBKBDZWVWDBEOCT/events.json","paper":"https://pith.science/paper/YOU2DDXH"},"agent_actions":{"view_html":"https://pith.science/pith/YOU2DDXHGBKOBKBDZWVWDBEOCT","download_json":"https://pith.science/pith/YOU2DDXHGBKOBKBDZWVWDBEOCT.json","view_paper":"https://pith.science/paper/YOU2DDXH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1105.0924&json=true","fetch_graph":"https://pith.science/api/pith-number/YOU2DDXHGBKOBKBDZWVWDBEOCT/graph.json","fetch_events":"https://pith.science/api/pith-number/YOU2DDXHGBKOBKBDZWVWDBEOCT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YOU2DDXHGBKOBKBDZWVWDBEOCT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YOU2DDXHGBKOBKBDZWVWDBEOCT/action/storage_attestation","attest_author":"https://pith.science/pith/YOU2DDXHGBKOBKBDZWVWDBEOCT/action/author_attestation","sign_citation":"https://pith.science/pith/YOU2DDXHGBKOBKBDZWVWDBEOCT/action/citation_signature","submit_replication":"https://pith.science/pith/YOU2DDXHGBKOBKBDZWVWDBEOCT/action/replication_record"}},"created_at":"2026-05-18T04:15:18.561664+00:00","updated_at":"2026-05-18T04:15:18.561664+00:00"}