{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2004:ATXAJLDAOPO2OVRQP2BPVGMO3J","short_pith_number":"pith:ATXAJLDA","canonical_record":{"source":{"id":"cond-mat/0410192","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2004-10-08T06:54:07Z","cross_cats_sorted":["math-ph","math.MP","nlin.SI"],"title_canon_sha256":"a4c2ac2d0fd8df001c4586f7ad1b729a5c953d65f3d36d138c79d57228deaebf","abstract_canon_sha256":"9db0ec3cc8740884870d526ee2e83464fefe552a8aef62b494e2ea8310aab67f"},"schema_version":"1.0"},"canonical_sha256":"04ee04ac6073dda756307e82fa998eda768bfcc806c249e3e5b56bf566118f13","source":{"kind":"arxiv","id":"cond-mat/0410192","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0410192","created_at":"2026-05-18T01:39:57Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0410192v2","created_at":"2026-05-18T01:39:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0410192","created_at":"2026-05-18T01:39:57Z"},{"alias_kind":"pith_short_12","alias_value":"ATXAJLDAOPO2","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"ATXAJLDAOPO2OVRQ","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"ATXAJLDA","created_at":"2026-05-18T12:25:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2004:ATXAJLDAOPO2OVRQP2BPVGMO3J","target":"record","payload":{"canonical_record":{"source":{"id":"cond-mat/0410192","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2004-10-08T06:54:07Z","cross_cats_sorted":["math-ph","math.MP","nlin.SI"],"title_canon_sha256":"a4c2ac2d0fd8df001c4586f7ad1b729a5c953d65f3d36d138c79d57228deaebf","abstract_canon_sha256":"9db0ec3cc8740884870d526ee2e83464fefe552a8aef62b494e2ea8310aab67f"},"schema_version":"1.0"},"canonical_sha256":"04ee04ac6073dda756307e82fa998eda768bfcc806c249e3e5b56bf566118f13","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:39:57.607665Z","signature_b64":"25vCCrhvWomUVur+v8UB8ubAM1DfW9RDyW+9eZE9rArWPzoHuQIkyeIm40ntsjjEYf1kpifxqZIl5l14WJB6DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"04ee04ac6073dda756307e82fa998eda768bfcc806c249e3e5b56bf566118f13","last_reissued_at":"2026-05-18T01:39:57.607270Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:39:57.607270Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"cond-mat/0410192","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:39:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6+NTlkqlF1TNL+3AjP/A4H4cIRenAg990zKfNibWdOjUjurmljYFOGIlLOcSCOxcZusvnM5J186X2ohzz+AlBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-21T23:17:58.831679Z"},"content_sha256":"27734933d9f0a0e24e7b0c570cfbc7f0644c7450731712d7298c0aeb2fbeccb0","schema_version":"1.0","event_id":"sha256:27734933d9f0a0e24e7b0c570cfbc7f0644c7450731712d7298c0aeb2fbeccb0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2004:ATXAJLDAOPO2OVRQP2BPVGMO3J","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Non-dissipative Thermal Transport and Magnetothermal Effect for the Spin-1/2 Heisenberg Chain","license":"","headline":"","cross_cats":["math-ph","math.MP","nlin.SI"],"primary_cat":"cond-mat.stat-mech","authors_text":"Andreas Klumper, Kazumitsu Sakai","submitted_at":"2004-10-08T06:54:07Z","abstract_excerpt":"Anomalous magnetothermal effects are discussed in the spin-1/2 Heisenberg chain. The energy current is related to one of the non-trivial conserved quantities underlying integrability and therefore both the diagonal and off diagonal dynamical correlations of spin and energy current diverge. The energy-energy and spin-energy current correlations at finite temperatures are exactly calculated by a lattice path integral formulation. The low-temperature behavior of the thermomagnetic (magnetic Seebeck) coefficient is also discussed. Due to effects of strong correlations, we observe the magnetic Seeb"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0410192","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:39:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NCwpFrbGTnvGjrb79K9fR2bUOnm5ISMd5Vz3TcIwTsV1U2w9fvMg90AcbvlWdW+xMX58IwlFWvEA3EXxxAcgDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-21T23:17:58.832025Z"},"content_sha256":"966c964158484b1d79b46f7fcf189daed8d4a77bdbfd9ad354b394978e3575db","schema_version":"1.0","event_id":"sha256:966c964158484b1d79b46f7fcf189daed8d4a77bdbfd9ad354b394978e3575db"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ATXAJLDAOPO2OVRQP2BPVGMO3J/bundle.json","state_url":"https://pith.science/pith/ATXAJLDAOPO2OVRQP2BPVGMO3J/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ATXAJLDAOPO2OVRQP2BPVGMO3J/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":"2026-06-21T23:17:58Z","links":{"resolver":"https://pith.science/pith/ATXAJLDAOPO2OVRQP2BPVGMO3J","bundle":"https://pith.science/pith/ATXAJLDAOPO2OVRQP2BPVGMO3J/bundle.json","state":"https://pith.science/pith/ATXAJLDAOPO2OVRQP2BPVGMO3J/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ATXAJLDAOPO2OVRQP2BPVGMO3J/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2004:ATXAJLDAOPO2OVRQP2BPVGMO3J","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":"9db0ec3cc8740884870d526ee2e83464fefe552a8aef62b494e2ea8310aab67f","cross_cats_sorted":["math-ph","math.MP","nlin.SI"],"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2004-10-08T06:54:07Z","title_canon_sha256":"a4c2ac2d0fd8df001c4586f7ad1b729a5c953d65f3d36d138c79d57228deaebf"},"schema_version":"1.0","source":{"id":"cond-mat/0410192","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0410192","created_at":"2026-05-18T01:39:57Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0410192v2","created_at":"2026-05-18T01:39:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0410192","created_at":"2026-05-18T01:39:57Z"},{"alias_kind":"pith_short_12","alias_value":"ATXAJLDAOPO2","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"ATXAJLDAOPO2OVRQ","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"ATXAJLDA","created_at":"2026-05-18T12:25:52Z"}],"graph_snapshots":[{"event_id":"sha256:966c964158484b1d79b46f7fcf189daed8d4a77bdbfd9ad354b394978e3575db","target":"graph","created_at":"2026-05-18T01:39:57Z","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":"Anomalous magnetothermal effects are discussed in the spin-1/2 Heisenberg chain. The energy current is related to one of the non-trivial conserved quantities underlying integrability and therefore both the diagonal and off diagonal dynamical correlations of spin and energy current diverge. The energy-energy and spin-energy current correlations at finite temperatures are exactly calculated by a lattice path integral formulation. The low-temperature behavior of the thermomagnetic (magnetic Seebeck) coefficient is also discussed. Due to effects of strong correlations, we observe the magnetic Seeb","authors_text":"Andreas Klumper, Kazumitsu Sakai","cross_cats":["math-ph","math.MP","nlin.SI"],"headline":"","license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2004-10-08T06:54:07Z","title":"Non-dissipative Thermal Transport and Magnetothermal Effect for the Spin-1/2 Heisenberg Chain"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0410192","kind":"arxiv","version":2},"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":"sha256:27734933d9f0a0e24e7b0c570cfbc7f0644c7450731712d7298c0aeb2fbeccb0","target":"record","created_at":"2026-05-18T01:39:57Z","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":"9db0ec3cc8740884870d526ee2e83464fefe552a8aef62b494e2ea8310aab67f","cross_cats_sorted":["math-ph","math.MP","nlin.SI"],"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2004-10-08T06:54:07Z","title_canon_sha256":"a4c2ac2d0fd8df001c4586f7ad1b729a5c953d65f3d36d138c79d57228deaebf"},"schema_version":"1.0","source":{"id":"cond-mat/0410192","kind":"arxiv","version":2}},"canonical_sha256":"04ee04ac6073dda756307e82fa998eda768bfcc806c249e3e5b56bf566118f13","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"04ee04ac6073dda756307e82fa998eda768bfcc806c249e3e5b56bf566118f13","first_computed_at":"2026-05-18T01:39:57.607270Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:39:57.607270Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"25vCCrhvWomUVur+v8UB8ubAM1DfW9RDyW+9eZE9rArWPzoHuQIkyeIm40ntsjjEYf1kpifxqZIl5l14WJB6DA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:39:57.607665Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/0410192","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:27734933d9f0a0e24e7b0c570cfbc7f0644c7450731712d7298c0aeb2fbeccb0","sha256:966c964158484b1d79b46f7fcf189daed8d4a77bdbfd9ad354b394978e3575db"],"state_sha256":"fdf69d87f3366a37d7b9c99269dae01da9102d6be999d1f8847e281e5b66aa46"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VNT/MoXl2rAiXHbk7K9diEhKYwKt6diefYBtQo1sE/nXEmSitBkXMMQI3pDpWtrkCAMV1oyljGeXmY/CdEa8Aw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-21T23:17:58.833964Z","bundle_sha256":"edb2fde209f9abfbf8d7fc666ce7382457056437f2a04e9620887b12dd9f2ea0"}}