{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:4ABGGPDO34Q654BLZDRMCREUDU","short_pith_number":"pith:4ABGGPDO","canonical_record":{"source":{"id":"1004.2438","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2010-04-14T16:15:47Z","cross_cats_sorted":[],"title_canon_sha256":"5af9068302b60c7d1c5c70ba2e1e98a3bc3acc4be91025b2abe5ccf13b9cfb00","abstract_canon_sha256":"504102c7ff6cd3b312e0600e09ef18b9430c528c1d21e6ff7e2412f2debfce3a"},"schema_version":"1.0"},"canonical_sha256":"e002633c6edf21eef02bc8e2c144941d3af3b50d503f958f9fb18ebb926e5467","source":{"kind":"arxiv","id":"1004.2438","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1004.2438","created_at":"2026-05-18T01:04:46Z"},{"alias_kind":"arxiv_version","alias_value":"1004.2438v2","created_at":"2026-05-18T01:04:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1004.2438","created_at":"2026-05-18T01:04:46Z"},{"alias_kind":"pith_short_12","alias_value":"4ABGGPDO34Q6","created_at":"2026-05-18T12:26:03Z"},{"alias_kind":"pith_short_16","alias_value":"4ABGGPDO34Q654BL","created_at":"2026-05-18T12:26:03Z"},{"alias_kind":"pith_short_8","alias_value":"4ABGGPDO","created_at":"2026-05-18T12:26:03Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:4ABGGPDO34Q654BLZDRMCREUDU","target":"record","payload":{"canonical_record":{"source":{"id":"1004.2438","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2010-04-14T16:15:47Z","cross_cats_sorted":[],"title_canon_sha256":"5af9068302b60c7d1c5c70ba2e1e98a3bc3acc4be91025b2abe5ccf13b9cfb00","abstract_canon_sha256":"504102c7ff6cd3b312e0600e09ef18b9430c528c1d21e6ff7e2412f2debfce3a"},"schema_version":"1.0"},"canonical_sha256":"e002633c6edf21eef02bc8e2c144941d3af3b50d503f958f9fb18ebb926e5467","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:04:46.226489Z","signature_b64":"ZoaAfAtKfuKqe6tphf82gzkHrwv5iwLe1J2i80L1uj+khSHqyE27eoKVJoyq6Oj1Sz9d3+ffG4vw8wVOiPI6AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e002633c6edf21eef02bc8e2c144941d3af3b50d503f958f9fb18ebb926e5467","last_reissued_at":"2026-05-18T01:04:46.225837Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:04:46.225837Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1004.2438","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":"2026-05-18T01:04:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GriwU/KH9hxsNYJEw8IUxh6gFb0nZWaWnPV8TdGdCLy8BeoUH9uOgVduohH1DexY+Q7fJoZRFwk9mCQJ1ug7CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T08:44:04.841678Z"},"content_sha256":"71ab1b35f4bbce7cfbcfdec2277adb3b3283d73a684a3ac43a8ec04bfce5766e","schema_version":"1.0","event_id":"sha256:71ab1b35f4bbce7cfbcfdec2277adb3b3283d73a684a3ac43a8ec04bfce5766e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:4ABGGPDO34Q654BLZDRMCREUDU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Random-matrix theory of thermal conduction in superconducting quantum dots","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"B. B\\'eri, C. W. J. Beenakker, J. P. Dahlhaus","submitted_at":"2010-04-14T16:15:47Z","abstract_excerpt":"We calculate the probability distribution of the transmission eigenvalues T_n of Bogoliubov quasiparticles at the Fermi level in an ensemble of chaotic Andreev quantum dots. The four Altland-Zirnbauer symmetry classes (determined by the presence or absence of time-reversal and spin-rotation symmetry) give rise to four circular ensembles of scattering matrices. We determine P({T_n}) for each ensemble, characterized by two symmetry indices \\beta and \\gamma . For a single d-fold degenerate transmission channel we thus obtain the distribution P(g) ~ g^{-1+\\beta /2}(1-g)^{\\gamma /2} of the thermal "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1004.2438","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":"2026-05-18T01:04:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BMgxKodltOXBSOkSRZFxQ6cUZJbpdBcACrfPG/UHnHpMv/HWzfpCKNLODxhYS6x9jYF2e/fifpL1IXOCqptpCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T08:44:04.842031Z"},"content_sha256":"03145478675a39b3db19ecccb36d7707759f4e57351303efdbf3d80f534e8e55","schema_version":"1.0","event_id":"sha256:03145478675a39b3db19ecccb36d7707759f4e57351303efdbf3d80f534e8e55"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4ABGGPDO34Q654BLZDRMCREUDU/bundle.json","state_url":"https://pith.science/pith/4ABGGPDO34Q654BLZDRMCREUDU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4ABGGPDO34Q654BLZDRMCREUDU/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":"2026-05-30T08:44:04Z","links":{"resolver":"https://pith.science/pith/4ABGGPDO34Q654BLZDRMCREUDU","bundle":"https://pith.science/pith/4ABGGPDO34Q654BLZDRMCREUDU/bundle.json","state":"https://pith.science/pith/4ABGGPDO34Q654BLZDRMCREUDU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4ABGGPDO34Q654BLZDRMCREUDU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:4ABGGPDO34Q654BLZDRMCREUDU","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":"504102c7ff6cd3b312e0600e09ef18b9430c528c1d21e6ff7e2412f2debfce3a","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2010-04-14T16:15:47Z","title_canon_sha256":"5af9068302b60c7d1c5c70ba2e1e98a3bc3acc4be91025b2abe5ccf13b9cfb00"},"schema_version":"1.0","source":{"id":"1004.2438","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1004.2438","created_at":"2026-05-18T01:04:46Z"},{"alias_kind":"arxiv_version","alias_value":"1004.2438v2","created_at":"2026-05-18T01:04:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1004.2438","created_at":"2026-05-18T01:04:46Z"},{"alias_kind":"pith_short_12","alias_value":"4ABGGPDO34Q6","created_at":"2026-05-18T12:26:03Z"},{"alias_kind":"pith_short_16","alias_value":"4ABGGPDO34Q654BL","created_at":"2026-05-18T12:26:03Z"},{"alias_kind":"pith_short_8","alias_value":"4ABGGPDO","created_at":"2026-05-18T12:26:03Z"}],"graph_snapshots":[{"event_id":"sha256:03145478675a39b3db19ecccb36d7707759f4e57351303efdbf3d80f534e8e55","target":"graph","created_at":"2026-05-18T01:04:46Z","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 calculate the probability distribution of the transmission eigenvalues T_n of Bogoliubov quasiparticles at the Fermi level in an ensemble of chaotic Andreev quantum dots. The four Altland-Zirnbauer symmetry classes (determined by the presence or absence of time-reversal and spin-rotation symmetry) give rise to four circular ensembles of scattering matrices. We determine P({T_n}) for each ensemble, characterized by two symmetry indices \\beta and \\gamma . For a single d-fold degenerate transmission channel we thus obtain the distribution P(g) ~ g^{-1+\\beta /2}(1-g)^{\\gamma /2} of the thermal ","authors_text":"B. B\\'eri, C. W. J. Beenakker, J. P. Dahlhaus","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2010-04-14T16:15:47Z","title":"Random-matrix theory of thermal conduction in superconducting quantum dots"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1004.2438","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":"sha256:71ab1b35f4bbce7cfbcfdec2277adb3b3283d73a684a3ac43a8ec04bfce5766e","target":"record","created_at":"2026-05-18T01:04:46Z","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":"504102c7ff6cd3b312e0600e09ef18b9430c528c1d21e6ff7e2412f2debfce3a","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2010-04-14T16:15:47Z","title_canon_sha256":"5af9068302b60c7d1c5c70ba2e1e98a3bc3acc4be91025b2abe5ccf13b9cfb00"},"schema_version":"1.0","source":{"id":"1004.2438","kind":"arxiv","version":2}},"canonical_sha256":"e002633c6edf21eef02bc8e2c144941d3af3b50d503f958f9fb18ebb926e5467","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e002633c6edf21eef02bc8e2c144941d3af3b50d503f958f9fb18ebb926e5467","first_computed_at":"2026-05-18T01:04:46.225837Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:04:46.225837Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ZoaAfAtKfuKqe6tphf82gzkHrwv5iwLe1J2i80L1uj+khSHqyE27eoKVJoyq6Oj1Sz9d3+ffG4vw8wVOiPI6AQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:04:46.226489Z","signed_message":"canonical_sha256_bytes"},"source_id":"1004.2438","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:71ab1b35f4bbce7cfbcfdec2277adb3b3283d73a684a3ac43a8ec04bfce5766e","sha256:03145478675a39b3db19ecccb36d7707759f4e57351303efdbf3d80f534e8e55"],"state_sha256":"8133941b39a8b2058767aa679ce2b6a7055df19c6566a9911eb6bebab59fa919"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XLEqlgr4AmK7Y3wx4iLGKvMyJGjpTZ24o9oQDtkh7FbrxPncPlPpAjr3B/5015O9Ua5zncL+3N8urYozRmLiAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T08:44:04.844236Z","bundle_sha256":"06fbda2288ee456fd1adec5dc1984fc33b5d53f8d3c6175fc1f2f4bd40f909c7"}}