{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:KRMARLUTCOWPKHA26TZG4JJM3R","short_pith_number":"pith:KRMARLUT","schema_version":"1.0","canonical_sha256":"545808ae9313acf51c1af4f26e252cdc4d76edda497cfa32c2219538f0fe41c4","source":{"kind":"arxiv","id":"cond-mat/0606403","version":1},"attestation_state":"computed","paper":{"title":"Interplay between phase defects and spin polarization in the specific heat of the spin density wave compound (TMTTF)_2Br in a magnetic field","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.dis-nn","authors_text":"G. Remenyi, J.C. Lasjaunias, K. Biljakovic, R. M\\'elin, S. Sahling","submitted_at":"2006-06-15T08:20:38Z","abstract_excerpt":"Equilibrium heat relaxation experiments provide evidence that the ground state of the commensurate spin density wave (SDW) compound (TMTTF)$_2$Br after the application of a sufficient magnetic field is different from the conventional ground state. The experiments are interpreted on the basis of the local model of strong pinning as the deconfinement of soliton-antisoliton pairs triggered by the Zeeman coupling to spin degrees of freedom, resulting in a magnetic field induced density wave glass for the spin carrying phase configuration."},"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":"cond-mat/0606403","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.dis-nn","submitted_at":"2006-06-15T08:20:38Z","cross_cats_sorted":[],"title_canon_sha256":"bede848eec1669ae908053e992475e89f81aa2fca21c8afe803eae44426cd65c","abstract_canon_sha256":"5dfa40fa49fb2a214c918393590dd7ac828f0b86af7bd7e963053a4267f12cfb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:54:53.239830Z","signature_b64":"n/eZ4zQadqxoONqepqeNiMyVteCs9K8Y4qHltFMGJiE71ySaipq6esyTzyrRaMqxSIeL8UP2Z3+poIdzwVFPDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"545808ae9313acf51c1af4f26e252cdc4d76edda497cfa32c2219538f0fe41c4","last_reissued_at":"2026-07-04T14:54:53.239479Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:54:53.239479Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Interplay between phase defects and spin polarization in the specific heat of the spin density wave compound (TMTTF)_2Br in a magnetic field","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.dis-nn","authors_text":"G. Remenyi, J.C. Lasjaunias, K. Biljakovic, R. M\\'elin, S. Sahling","submitted_at":"2006-06-15T08:20:38Z","abstract_excerpt":"Equilibrium heat relaxation experiments provide evidence that the ground state of the commensurate spin density wave (SDW) compound (TMTTF)$_2$Br after the application of a sufficient magnetic field is different from the conventional ground state. The experiments are interpreted on the basis of the local model of strong pinning as the deconfinement of soliton-antisoliton pairs triggered by the Zeeman coupling to spin degrees of freedom, resulting in a magnetic field induced density wave glass for the spin carrying phase configuration."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0606403","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/cond-mat/0606403/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"cond-mat/0606403","created_at":"2026-07-04T14:54:53.239543+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0606403v1","created_at":"2026-07-04T14:54:53.239543+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0606403","created_at":"2026-07-04T14:54:53.239543+00:00"},{"alias_kind":"pith_short_12","alias_value":"KRMARLUTCOWP","created_at":"2026-07-04T14:54:53.239543+00:00"},{"alias_kind":"pith_short_16","alias_value":"KRMARLUTCOWPKHA2","created_at":"2026-07-04T14:54:53.239543+00:00"},{"alias_kind":"pith_short_8","alias_value":"KRMARLUT","created_at":"2026-07-04T14:54:53.239543+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/KRMARLUTCOWPKHA26TZG4JJM3R","json":"https://pith.science/pith/KRMARLUTCOWPKHA26TZG4JJM3R.json","graph_json":"https://pith.science/api/pith-number/KRMARLUTCOWPKHA26TZG4JJM3R/graph.json","events_json":"https://pith.science/api/pith-number/KRMARLUTCOWPKHA26TZG4JJM3R/events.json","paper":"https://pith.science/paper/KRMARLUT"},"agent_actions":{"view_html":"https://pith.science/pith/KRMARLUTCOWPKHA26TZG4JJM3R","download_json":"https://pith.science/pith/KRMARLUTCOWPKHA26TZG4JJM3R.json","view_paper":"https://pith.science/paper/KRMARLUT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/0606403&json=true","fetch_graph":"https://pith.science/api/pith-number/KRMARLUTCOWPKHA26TZG4JJM3R/graph.json","fetch_events":"https://pith.science/api/pith-number/KRMARLUTCOWPKHA26TZG4JJM3R/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KRMARLUTCOWPKHA26TZG4JJM3R/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KRMARLUTCOWPKHA26TZG4JJM3R/action/storage_attestation","attest_author":"https://pith.science/pith/KRMARLUTCOWPKHA26TZG4JJM3R/action/author_attestation","sign_citation":"https://pith.science/pith/KRMARLUTCOWPKHA26TZG4JJM3R/action/citation_signature","submit_replication":"https://pith.science/pith/KRMARLUTCOWPKHA26TZG4JJM3R/action/replication_record"}},"created_at":"2026-07-04T14:54:53.239543+00:00","updated_at":"2026-07-04T14:54:53.239543+00:00"}