{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:FVEBEHJKK3DFPAKV3L6NILPEFV","short_pith_number":"pith:FVEBEHJK","canonical_record":{"source":{"id":"1810.06166","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2018-10-15T02:58:38Z","cross_cats_sorted":[],"title_canon_sha256":"8edfee1d14b8a9a6c19c8249c390284d4909bfddf410f32db782aed926f5c064","abstract_canon_sha256":"6ebbdf51c00730a3a132e4ae3f334b70a8fde460062f5bcbb6da9bcc3526c31e"},"schema_version":"1.0"},"canonical_sha256":"2d48121d2a56c6578155dafcd42de42d5bc814a6f3f11e50de8e085128c6c08c","source":{"kind":"arxiv","id":"1810.06166","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1810.06166","created_at":"2026-05-18T00:03:21Z"},{"alias_kind":"arxiv_version","alias_value":"1810.06166v1","created_at":"2026-05-18T00:03:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1810.06166","created_at":"2026-05-18T00:03:21Z"},{"alias_kind":"pith_short_12","alias_value":"FVEBEHJKK3DF","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_16","alias_value":"FVEBEHJKK3DFPAKV","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_8","alias_value":"FVEBEHJK","created_at":"2026-05-18T12:32:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:FVEBEHJKK3DFPAKV3L6NILPEFV","target":"record","payload":{"canonical_record":{"source":{"id":"1810.06166","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2018-10-15T02:58:38Z","cross_cats_sorted":[],"title_canon_sha256":"8edfee1d14b8a9a6c19c8249c390284d4909bfddf410f32db782aed926f5c064","abstract_canon_sha256":"6ebbdf51c00730a3a132e4ae3f334b70a8fde460062f5bcbb6da9bcc3526c31e"},"schema_version":"1.0"},"canonical_sha256":"2d48121d2a56c6578155dafcd42de42d5bc814a6f3f11e50de8e085128c6c08c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:03:21.219480Z","signature_b64":"BpQ4DuhXdotHQ48QpOPd2/zsVaTpsyIVHQljCM91XdbOyB8cxCWSKLYQyuaKWMQSF1l6h6FslrFbA1ZoFOOGAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2d48121d2a56c6578155dafcd42de42d5bc814a6f3f11e50de8e085128c6c08c","last_reissued_at":"2026-05-18T00:03:21.218992Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:03:21.218992Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1810.06166","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":"2026-05-18T00:03:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1wsA7xVzDrYYUwQBBKgT75mndscsFGq9FEFwCBy23go3LxoBA0yFaxvsJWdejzrfJIt6w0n1jCMvU/pOI4ijCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T17:46:35.256452Z"},"content_sha256":"240f315518e2eb22a0f1f9c44ff0af8b27be429e9c694895f609404d9a634c92","schema_version":"1.0","event_id":"sha256:240f315518e2eb22a0f1f9c44ff0af8b27be429e9c694895f609404d9a634c92"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:FVEBEHJKK3DFPAKV3L6NILPEFV","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Distribution of S-matrix poles for one-dimensional disordered wires","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.dis-nn","authors_text":"F. M. Izrailev, I. F. Herrera-Gonz\\'alez, J. A. M\\'endez-Berm\\'udez","submitted_at":"2018-10-15T02:58:38Z","abstract_excerpt":"By the use of the effective non-Hermitian Hamiltonian approach to scattering we study the distribution of the scattering matrix (S-matrix) poles in one-dimensional (1D) models with various types of diagonal disorder. We consider the case of 1D tight-binding wires, with both on-site uncorrelated and correlated disorder, coupled to the continuum through leads attached to the wire edges. In particular, we focus on the location of the S-matrix poles in the complex plane as a function of the coupling strength and the disorder strength. Specific interest is paid to the super-radiance transition emer"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1810.06166","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":""},"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":"2026-05-18T00:03:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qkHNwbh0mEMpscS/3tET+3DNjzibXFs9MyrXuKFqU2YyjwtZDqZfL1078kfscYftI02t76Qy7YIlAQIUa+UUBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T17:46:35.257124Z"},"content_sha256":"c6671549729664c8cecfdd7facf1c6882ded49f381aa3ee15210d61cab5dd2f0","schema_version":"1.0","event_id":"sha256:c6671549729664c8cecfdd7facf1c6882ded49f381aa3ee15210d61cab5dd2f0"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FVEBEHJKK3DFPAKV3L6NILPEFV/bundle.json","state_url":"https://pith.science/pith/FVEBEHJKK3DFPAKV3L6NILPEFV/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FVEBEHJKK3DFPAKV3L6NILPEFV/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":"2026-05-30T17:46:35Z","links":{"resolver":"https://pith.science/pith/FVEBEHJKK3DFPAKV3L6NILPEFV","bundle":"https://pith.science/pith/FVEBEHJKK3DFPAKV3L6NILPEFV/bundle.json","state":"https://pith.science/pith/FVEBEHJKK3DFPAKV3L6NILPEFV/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FVEBEHJKK3DFPAKV3L6NILPEFV/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:FVEBEHJKK3DFPAKV3L6NILPEFV","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":"6ebbdf51c00730a3a132e4ae3f334b70a8fde460062f5bcbb6da9bcc3526c31e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2018-10-15T02:58:38Z","title_canon_sha256":"8edfee1d14b8a9a6c19c8249c390284d4909bfddf410f32db782aed926f5c064"},"schema_version":"1.0","source":{"id":"1810.06166","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1810.06166","created_at":"2026-05-18T00:03:21Z"},{"alias_kind":"arxiv_version","alias_value":"1810.06166v1","created_at":"2026-05-18T00:03:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1810.06166","created_at":"2026-05-18T00:03:21Z"},{"alias_kind":"pith_short_12","alias_value":"FVEBEHJKK3DF","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_16","alias_value":"FVEBEHJKK3DFPAKV","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_8","alias_value":"FVEBEHJK","created_at":"2026-05-18T12:32:25Z"}],"graph_snapshots":[{"event_id":"sha256:c6671549729664c8cecfdd7facf1c6882ded49f381aa3ee15210d61cab5dd2f0","target":"graph","created_at":"2026-05-18T00:03:21Z","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":"By the use of the effective non-Hermitian Hamiltonian approach to scattering we study the distribution of the scattering matrix (S-matrix) poles in one-dimensional (1D) models with various types of diagonal disorder. We consider the case of 1D tight-binding wires, with both on-site uncorrelated and correlated disorder, coupled to the continuum through leads attached to the wire edges. In particular, we focus on the location of the S-matrix poles in the complex plane as a function of the coupling strength and the disorder strength. Specific interest is paid to the super-radiance transition emer","authors_text":"F. M. Izrailev, I. F. Herrera-Gonz\\'alez, J. A. M\\'endez-Berm\\'udez","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2018-10-15T02:58:38Z","title":"Distribution of S-matrix poles for one-dimensional disordered wires"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1810.06166","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":"sha256:240f315518e2eb22a0f1f9c44ff0af8b27be429e9c694895f609404d9a634c92","target":"record","created_at":"2026-05-18T00:03:21Z","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":"6ebbdf51c00730a3a132e4ae3f334b70a8fde460062f5bcbb6da9bcc3526c31e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2018-10-15T02:58:38Z","title_canon_sha256":"8edfee1d14b8a9a6c19c8249c390284d4909bfddf410f32db782aed926f5c064"},"schema_version":"1.0","source":{"id":"1810.06166","kind":"arxiv","version":1}},"canonical_sha256":"2d48121d2a56c6578155dafcd42de42d5bc814a6f3f11e50de8e085128c6c08c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2d48121d2a56c6578155dafcd42de42d5bc814a6f3f11e50de8e085128c6c08c","first_computed_at":"2026-05-18T00:03:21.218992Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:03:21.218992Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"BpQ4DuhXdotHQ48QpOPd2/zsVaTpsyIVHQljCM91XdbOyB8cxCWSKLYQyuaKWMQSF1l6h6FslrFbA1ZoFOOGAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:03:21.219480Z","signed_message":"canonical_sha256_bytes"},"source_id":"1810.06166","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:240f315518e2eb22a0f1f9c44ff0af8b27be429e9c694895f609404d9a634c92","sha256:c6671549729664c8cecfdd7facf1c6882ded49f381aa3ee15210d61cab5dd2f0"],"state_sha256":"079600864cf96b2b355d1e012eb421091ab2565409f12cd4ea31a9de2e7b9a8f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HsrZc95ZSMsTps/gVHq/dM5b4FKeDy9JCmfIc2QZIUg2thu8rrjwdzdQTmhk/nF86X383jgdHBlQY8OEkxdEBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T17:46:35.260296Z","bundle_sha256":"dbd628fd2ef248420c502c8c9cee98b25fd88e663c084a3a4a4c35d6f134d60e"}}