{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1994:TVVOY3UCY3EHNOBCRI7PX4MDJT","short_pith_number":"pith:TVVOY3UC","canonical_record":{"source":{"id":"cond-mat/9405084","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat","submitted_at":"1994-05-27T15:23:03Z","cross_cats_sorted":[],"title_canon_sha256":"ac40491c26a391e38025e114e7d910ee020c285464d6562bb416d61221818ae9","abstract_canon_sha256":"861e8e473f2183230ded26a4f2ccb63d3a68714e7cbce7634ea5fd65c4f0acc8"},"schema_version":"1.0"},"canonical_sha256":"9d6aec6e82c6c876b8228a3efbf1834cff5021a05555fbfbe259537487afed87","source":{"kind":"arxiv","id":"cond-mat/9405084","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/9405084","created_at":"2026-07-04T14:22:38Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9405084v1","created_at":"2026-07-04T14:22:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9405084","created_at":"2026-07-04T14:22:38Z"},{"alias_kind":"pith_short_12","alias_value":"TVVOY3UCY3EH","created_at":"2026-07-04T14:22:38Z"},{"alias_kind":"pith_short_16","alias_value":"TVVOY3UCY3EHNOBC","created_at":"2026-07-04T14:22:38Z"},{"alias_kind":"pith_short_8","alias_value":"TVVOY3UC","created_at":"2026-07-04T14:22:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1994:TVVOY3UCY3EHNOBCRI7PX4MDJT","target":"record","payload":{"canonical_record":{"source":{"id":"cond-mat/9405084","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat","submitted_at":"1994-05-27T15:23:03Z","cross_cats_sorted":[],"title_canon_sha256":"ac40491c26a391e38025e114e7d910ee020c285464d6562bb416d61221818ae9","abstract_canon_sha256":"861e8e473f2183230ded26a4f2ccb63d3a68714e7cbce7634ea5fd65c4f0acc8"},"schema_version":"1.0"},"canonical_sha256":"9d6aec6e82c6c876b8228a3efbf1834cff5021a05555fbfbe259537487afed87","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:22:38.761081Z","signature_b64":"dKXaYqXhvOdtZsNn8dYRuDgPMOcwJRkm98AbVgWBcOmuuSBiP5MRShaX10O0R1lvAZZmBV5GmcQGFjks9PGEBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9d6aec6e82c6c876b8228a3efbf1834cff5021a05555fbfbe259537487afed87","last_reissued_at":"2026-07-04T14:22:38.760674Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:22:38.760674Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"cond-mat/9405084","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T14:22:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fSGIuY+ZgSz4UFcPgUa8rnA5M4W3D41gewmTovAyDwc7DIIjzD7Ale+bu/+jCEpCY2iNRaU6+Y4r6Rs8roC+BQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T17:29:07.480922Z"},"content_sha256":"3e5669f36f44f2b53791464dfa6f7587164da80f6f9c68cf3f1553a0b23b098a","schema_version":"1.0","event_id":"sha256:3e5669f36f44f2b53791464dfa6f7587164da80f6f9c68cf3f1553a0b23b098a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1994:TVVOY3UCY3EHNOBCRI7PX4MDJT","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Exactly solvable random matrix models with additional two-body interactions","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat","authors_text":"K.A.Muttalib","submitted_at":"1994-05-27T15:23:03Z","abstract_excerpt":"It has been argued that despite remarkable success, existing random matrix theories are not adequate to describe disordered conductors in the metallic regime, due to the presence of certain two-body interactions in the effective Hamiltonian for the eigenvalues, in addition to the standard logarithmic interaction that arises entirely from symmetry considerations. We present a new method that allows exact solution of random matrix models with such additional two-body interactions. This should broaden the scope of random matrix models in general."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9405084","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/9405084/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T14:22:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+qIbdrF8S/lk68KPtYxyAAe2tUBZ37xI4cOQ3IEPSiHXrpvWnp5yn7Ewkapq2jpuHJG6n3Wa4wEy5NhiJx7ZCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T17:29:07.481415Z"},"content_sha256":"08509f5bee4682df07d9f9a2306ab7b657eaf232a6898272acf04d37091878e1","schema_version":"1.0","event_id":"sha256:08509f5bee4682df07d9f9a2306ab7b657eaf232a6898272acf04d37091878e1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/TVVOY3UCY3EHNOBCRI7PX4MDJT/bundle.json","state_url":"https://pith.science/pith/TVVOY3UCY3EHNOBCRI7PX4MDJT/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/TVVOY3UCY3EHNOBCRI7PX4MDJT/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":"2026-08-11T17:29:07Z","links":{"resolver":"https://pith.science/pith/TVVOY3UCY3EHNOBCRI7PX4MDJT","bundle":"https://pith.science/pith/TVVOY3UCY3EHNOBCRI7PX4MDJT/bundle.json","state":"https://pith.science/pith/TVVOY3UCY3EHNOBCRI7PX4MDJT/state.json","well_known_bundle":"https://pith.science/.well-known/pith/TVVOY3UCY3EHNOBCRI7PX4MDJT/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1994:TVVOY3UCY3EHNOBCRI7PX4MDJT","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":"861e8e473f2183230ded26a4f2ccb63d3a68714e7cbce7634ea5fd65c4f0acc8","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat","submitted_at":"1994-05-27T15:23:03Z","title_canon_sha256":"ac40491c26a391e38025e114e7d910ee020c285464d6562bb416d61221818ae9"},"schema_version":"1.0","source":{"id":"cond-mat/9405084","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/9405084","created_at":"2026-07-04T14:22:38Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9405084v1","created_at":"2026-07-04T14:22:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9405084","created_at":"2026-07-04T14:22:38Z"},{"alias_kind":"pith_short_12","alias_value":"TVVOY3UCY3EH","created_at":"2026-07-04T14:22:38Z"},{"alias_kind":"pith_short_16","alias_value":"TVVOY3UCY3EHNOBC","created_at":"2026-07-04T14:22:38Z"},{"alias_kind":"pith_short_8","alias_value":"TVVOY3UC","created_at":"2026-07-04T14:22:38Z"}],"graph_snapshots":[{"event_id":"sha256:08509f5bee4682df07d9f9a2306ab7b657eaf232a6898272acf04d37091878e1","target":"graph","created_at":"2026-07-04T14:22:38Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/cond-mat/9405084/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"It has been argued that despite remarkable success, existing random matrix theories are not adequate to describe disordered conductors in the metallic regime, due to the presence of certain two-body interactions in the effective Hamiltonian for the eigenvalues, in addition to the standard logarithmic interaction that arises entirely from symmetry considerations. We present a new method that allows exact solution of random matrix models with such additional two-body interactions. This should broaden the scope of random matrix models in general.","authors_text":"K.A.Muttalib","cross_cats":[],"headline":"","license":"","primary_cat":"cond-mat","submitted_at":"1994-05-27T15:23:03Z","title":"Exactly solvable random matrix models with additional two-body interactions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9405084","kind":"arxiv","version":1},"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":"sha256:3e5669f36f44f2b53791464dfa6f7587164da80f6f9c68cf3f1553a0b23b098a","target":"record","created_at":"2026-07-04T14:22:38Z","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":"861e8e473f2183230ded26a4f2ccb63d3a68714e7cbce7634ea5fd65c4f0acc8","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat","submitted_at":"1994-05-27T15:23:03Z","title_canon_sha256":"ac40491c26a391e38025e114e7d910ee020c285464d6562bb416d61221818ae9"},"schema_version":"1.0","source":{"id":"cond-mat/9405084","kind":"arxiv","version":1}},"canonical_sha256":"9d6aec6e82c6c876b8228a3efbf1834cff5021a05555fbfbe259537487afed87","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9d6aec6e82c6c876b8228a3efbf1834cff5021a05555fbfbe259537487afed87","first_computed_at":"2026-07-04T14:22:38.760674Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T14:22:38.760674Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"dKXaYqXhvOdtZsNn8dYRuDgPMOcwJRkm98AbVgWBcOmuuSBiP5MRShaX10O0R1lvAZZmBV5GmcQGFjks9PGEBw==","signature_status":"signed_v1","signed_at":"2026-07-04T14:22:38.761081Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/9405084","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3e5669f36f44f2b53791464dfa6f7587164da80f6f9c68cf3f1553a0b23b098a","sha256:08509f5bee4682df07d9f9a2306ab7b657eaf232a6898272acf04d37091878e1"],"state_sha256":"faf277c5c3ceedfeebb56782604d3f670f8a5ff88f65661b41c4af9e18235d1c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"agLvoikOWpPEASGuxABQ2D4MFIVhRr6XOwCvHp77U6r3aeIRwchWeXeGN5Oa4OoaxZsPxvyIDfZyOU+dTwjdAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-11T17:29:07.487718Z","bundle_sha256":"55918a41ac533b0090edca251f99ed5d5d17f59f70f8c4a153dd175274f05166"}}