{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2008:7BAOKSUJR4I2RP6VH2JECN2OPO","short_pith_number":"pith:7BAOKSUJ","canonical_record":{"source":{"id":"0811.1344","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2008-11-09T15:57:58Z","cross_cats_sorted":["cond-mat.stat-mech","cond-mat.str-el","physics.chem-ph"],"title_canon_sha256":"1604812f7c42984e6b1857146942742d08187d2a9cbacbf6368c34e2566a9cf1","abstract_canon_sha256":"d9eaf5d03ddab1ec8d932f2444cce802f8850c8361724db4cc5bef7660316063"},"schema_version":"1.0"},"canonical_sha256":"f840e54a898f11a8bfd53e9241374e7b917604ace59338ded054996c95b6ce15","source":{"kind":"arxiv","id":"0811.1344","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0811.1344","created_at":"2026-05-18T01:05:13Z"},{"alias_kind":"arxiv_version","alias_value":"0811.1344v3","created_at":"2026-05-18T01:05:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0811.1344","created_at":"2026-05-18T01:05:13Z"},{"alias_kind":"pith_short_12","alias_value":"7BAOKSUJR4I2","created_at":"2026-05-18T12:25:56Z"},{"alias_kind":"pith_short_16","alias_value":"7BAOKSUJR4I2RP6V","created_at":"2026-05-18T12:25:56Z"},{"alias_kind":"pith_short_8","alias_value":"7BAOKSUJ","created_at":"2026-05-18T12:25:56Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2008:7BAOKSUJR4I2RP6VH2JECN2OPO","target":"record","payload":{"canonical_record":{"source":{"id":"0811.1344","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2008-11-09T15:57:58Z","cross_cats_sorted":["cond-mat.stat-mech","cond-mat.str-el","physics.chem-ph"],"title_canon_sha256":"1604812f7c42984e6b1857146942742d08187d2a9cbacbf6368c34e2566a9cf1","abstract_canon_sha256":"d9eaf5d03ddab1ec8d932f2444cce802f8850c8361724db4cc5bef7660316063"},"schema_version":"1.0"},"canonical_sha256":"f840e54a898f11a8bfd53e9241374e7b917604ace59338ded054996c95b6ce15","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:05:13.390729Z","signature_b64":"IH16rF918kAJGGo/D2nRpf+pAEvPvpzcAsI399lUtUnkKiOBYk00Y22BAAZcfSygpoL2CDyZPT/6iQ3rpC4oAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f840e54a898f11a8bfd53e9241374e7b917604ace59338ded054996c95b6ce15","last_reissued_at":"2026-05-18T01:05:13.390047Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:05:13.390047Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0811.1344","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:05:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"POESPRysjSBQDBo3l4B7Bmn36lYhCJNrmZhxxeoMv/WQVDsW55LNVExveF/UTcaORD1o+Gw/914yVc8kNLnLAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T02:05:19.167911Z"},"content_sha256":"55d2a7a39574ffa78ea1f2e1f81b1e1d0997c68f09b2e8a68d66b93e4d687fd2","schema_version":"1.0","event_id":"sha256:55d2a7a39574ffa78ea1f2e1f81b1e1d0997c68f09b2e8a68d66b93e4d687fd2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2008:7BAOKSUJR4I2RP6VH2JECN2OPO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Thermodynamics of ferromagnetic superconductors with spin-triplet electron pairing","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","cond-mat.str-el","physics.chem-ph"],"primary_cat":"cond-mat.supr-con","authors_text":"Diana V. Shopova, Dimo I. Uzunov","submitted_at":"2008-11-09T15:57:58Z","abstract_excerpt":"We present a general thermodynamic theory that describes phases and phase transitions of ferromagnetic superconductors with spin-triplet electron Cooper pairing. The theory is based on extended Ginzburg-Landau expansion in powers of superconducting and ferromagnetic order parameters. We propose a simple form for the dependence of theory parameters on the pressure that allows correct theoretical outline of the temperature-pressure phase diagram for which at low temperatures a stable phase of coexistence of p-wave superconductivity and itinerant ferromagnetism appears. We demonstrate that the th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0811.1344","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:05:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FLz3PW3SJECJoEBGIMu0v99dSAWl7zghaAEFRsqs18Cru91BJkBGrmKn9+7tIlSK5J5iu8scCgVYUtDzbCGVBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T02:05:19.168254Z"},"content_sha256":"e9e162929efc97c73713d6a1284b37d2261c0a2bd445bca78c00f780082b52fb","schema_version":"1.0","event_id":"sha256:e9e162929efc97c73713d6a1284b37d2261c0a2bd445bca78c00f780082b52fb"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/7BAOKSUJR4I2RP6VH2JECN2OPO/bundle.json","state_url":"https://pith.science/pith/7BAOKSUJR4I2RP6VH2JECN2OPO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/7BAOKSUJR4I2RP6VH2JECN2OPO/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-07T02:05:19Z","links":{"resolver":"https://pith.science/pith/7BAOKSUJR4I2RP6VH2JECN2OPO","bundle":"https://pith.science/pith/7BAOKSUJR4I2RP6VH2JECN2OPO/bundle.json","state":"https://pith.science/pith/7BAOKSUJR4I2RP6VH2JECN2OPO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/7BAOKSUJR4I2RP6VH2JECN2OPO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2008:7BAOKSUJR4I2RP6VH2JECN2OPO","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"d9eaf5d03ddab1ec8d932f2444cce802f8850c8361724db4cc5bef7660316063","cross_cats_sorted":["cond-mat.stat-mech","cond-mat.str-el","physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2008-11-09T15:57:58Z","title_canon_sha256":"1604812f7c42984e6b1857146942742d08187d2a9cbacbf6368c34e2566a9cf1"},"schema_version":"1.0","source":{"id":"0811.1344","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0811.1344","created_at":"2026-05-18T01:05:13Z"},{"alias_kind":"arxiv_version","alias_value":"0811.1344v3","created_at":"2026-05-18T01:05:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0811.1344","created_at":"2026-05-18T01:05:13Z"},{"alias_kind":"pith_short_12","alias_value":"7BAOKSUJR4I2","created_at":"2026-05-18T12:25:56Z"},{"alias_kind":"pith_short_16","alias_value":"7BAOKSUJR4I2RP6V","created_at":"2026-05-18T12:25:56Z"},{"alias_kind":"pith_short_8","alias_value":"7BAOKSUJ","created_at":"2026-05-18T12:25:56Z"}],"graph_snapshots":[{"event_id":"sha256:e9e162929efc97c73713d6a1284b37d2261c0a2bd445bca78c00f780082b52fb","target":"graph","created_at":"2026-05-18T01:05:13Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We present a general thermodynamic theory that describes phases and phase transitions of ferromagnetic superconductors with spin-triplet electron Cooper pairing. The theory is based on extended Ginzburg-Landau expansion in powers of superconducting and ferromagnetic order parameters. We propose a simple form for the dependence of theory parameters on the pressure that allows correct theoretical outline of the temperature-pressure phase diagram for which at low temperatures a stable phase of coexistence of p-wave superconductivity and itinerant ferromagnetism appears. We demonstrate that the th","authors_text":"Diana V. Shopova, Dimo I. Uzunov","cross_cats":["cond-mat.stat-mech","cond-mat.str-el","physics.chem-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2008-11-09T15:57:58Z","title":"Thermodynamics of ferromagnetic superconductors with spin-triplet electron pairing"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0811.1344","kind":"arxiv","version":3},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:55d2a7a39574ffa78ea1f2e1f81b1e1d0997c68f09b2e8a68d66b93e4d687fd2","target":"record","created_at":"2026-05-18T01:05:13Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"d9eaf5d03ddab1ec8d932f2444cce802f8850c8361724db4cc5bef7660316063","cross_cats_sorted":["cond-mat.stat-mech","cond-mat.str-el","physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2008-11-09T15:57:58Z","title_canon_sha256":"1604812f7c42984e6b1857146942742d08187d2a9cbacbf6368c34e2566a9cf1"},"schema_version":"1.0","source":{"id":"0811.1344","kind":"arxiv","version":3}},"canonical_sha256":"f840e54a898f11a8bfd53e9241374e7b917604ace59338ded054996c95b6ce15","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f840e54a898f11a8bfd53e9241374e7b917604ace59338ded054996c95b6ce15","first_computed_at":"2026-05-18T01:05:13.390047Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:05:13.390047Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"IH16rF918kAJGGo/D2nRpf+pAEvPvpzcAsI399lUtUnkKiOBYk00Y22BAAZcfSygpoL2CDyZPT/6iQ3rpC4oAA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:05:13.390729Z","signed_message":"canonical_sha256_bytes"},"source_id":"0811.1344","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:55d2a7a39574ffa78ea1f2e1f81b1e1d0997c68f09b2e8a68d66b93e4d687fd2","sha256:e9e162929efc97c73713d6a1284b37d2261c0a2bd445bca78c00f780082b52fb"],"state_sha256":"af2ab1d318c560d046dd44a2ae18ed1e6e28001d23bd008941f19dc39f23092a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FsCUKvAwUHYWOxKMWFzqNBCWnk3O/nyZVLaWvQJG1xbF1U9GUNKmsoXWydxY/Px9FqIbz5gx0zdMNXG0mfmlAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-07T02:05:19.170295Z","bundle_sha256":"16c3f2b5349802962603fa42cb810e0017fcbb97914a7b6c89978513ff010d3c"}}