{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:M6TWZ3GWTRLRUHONBACLXADFWE","short_pith_number":"pith:M6TWZ3GW","canonical_record":{"source":{"id":"1207.2387","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2012-07-10T15:16:41Z","cross_cats_sorted":[],"title_canon_sha256":"455ca68e238fbc7570fcac50bb6d18b54e4e7a4257927e6d99dab0fdb43940c8","abstract_canon_sha256":"6547544bab1fc4452a64004fdb87aef3421ac50f06e5547b4e0070861f3fedbf"},"schema_version":"1.0"},"canonical_sha256":"67a76cecd69c571a1dcd0804bb8065b11f67d939affd27f6e173b3c1d535f718","source":{"kind":"arxiv","id":"1207.2387","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1207.2387","created_at":"2026-05-18T03:51:24Z"},{"alias_kind":"arxiv_version","alias_value":"1207.2387v1","created_at":"2026-05-18T03:51:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.2387","created_at":"2026-05-18T03:51:24Z"},{"alias_kind":"pith_short_12","alias_value":"M6TWZ3GWTRLR","created_at":"2026-05-18T12:27:14Z"},{"alias_kind":"pith_short_16","alias_value":"M6TWZ3GWTRLRUHON","created_at":"2026-05-18T12:27:14Z"},{"alias_kind":"pith_short_8","alias_value":"M6TWZ3GW","created_at":"2026-05-18T12:27:14Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:M6TWZ3GWTRLRUHONBACLXADFWE","target":"record","payload":{"canonical_record":{"source":{"id":"1207.2387","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2012-07-10T15:16:41Z","cross_cats_sorted":[],"title_canon_sha256":"455ca68e238fbc7570fcac50bb6d18b54e4e7a4257927e6d99dab0fdb43940c8","abstract_canon_sha256":"6547544bab1fc4452a64004fdb87aef3421ac50f06e5547b4e0070861f3fedbf"},"schema_version":"1.0"},"canonical_sha256":"67a76cecd69c571a1dcd0804bb8065b11f67d939affd27f6e173b3c1d535f718","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:51:24.238949Z","signature_b64":"01NWHWRMHQcVKqm+VTIpX8+QQHVxqd7Tskvp7LOsybQUe+tmzmrgDnwSSJPeXfdvn4Y4pemtnTMmlmotBpULDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"67a76cecd69c571a1dcd0804bb8065b11f67d939affd27f6e173b3c1d535f718","last_reissued_at":"2026-05-18T03:51:24.238492Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:51:24.238492Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1207.2387","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":"2026-05-18T03:51:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jVIIrD2wi9cFA1Bq+LrYvalDqMVve7iYsOfszh9Va/HuyrnXWV4fziLqpEz00JuW2OLUgII5BYmyY0XuHvgkBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T08:11:49.198297Z"},"content_sha256":"df6521029dd0753436123851a103edd9112e5d0316ac7f2230838571fe6a1b24","schema_version":"1.0","event_id":"sha256:df6521029dd0753436123851a103edd9112e5d0316ac7f2230838571fe6a1b24"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:M6TWZ3GWTRLRUHONBACLXADFWE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Pair Scattering of Electrons in Edge Channels of Opposite Chiralities in the Presence of a Disorder Potential","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"M. G. Prokudina, V. S. Khrapai","submitted_at":"2012-07-10T15:16:41Z","abstract_excerpt":"The nonequilibrium transfer of the energy between electrons of counter-propagating quasi-one-dimensional systems has been perturbatively calculated for edge channels in a two-dimensional system in the integer quantum Hall effect. The processes involving two electrons that are allowed only in the system with disorder have been taken into account. Expressions for the cases of Coulomb scattering and transfer of nonequilibrium phonons have been obtained. The energy transferred per unit time has a quasi-threshold dependence on the degree of nonequilibrium of the hot channel. According to numerical "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.2387","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":"2026-05-18T03:51:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PiFYMW/RWipKTTV5vFlCYMCN8ZPxWsDTOEo8QH84clDHmE5BrswNmMUvopVt5WhAwTG2Lz8fRyQImNtaj4QjDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T08:11:49.198962Z"},"content_sha256":"31e6da544561133a4b6f41a450564a186dfa4d7cfe47dc2c4ba978825887e32e","schema_version":"1.0","event_id":"sha256:31e6da544561133a4b6f41a450564a186dfa4d7cfe47dc2c4ba978825887e32e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/M6TWZ3GWTRLRUHONBACLXADFWE/bundle.json","state_url":"https://pith.science/pith/M6TWZ3GWTRLRUHONBACLXADFWE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/M6TWZ3GWTRLRUHONBACLXADFWE/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":"2026-05-27T08:11:49Z","links":{"resolver":"https://pith.science/pith/M6TWZ3GWTRLRUHONBACLXADFWE","bundle":"https://pith.science/pith/M6TWZ3GWTRLRUHONBACLXADFWE/bundle.json","state":"https://pith.science/pith/M6TWZ3GWTRLRUHONBACLXADFWE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/M6TWZ3GWTRLRUHONBACLXADFWE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:M6TWZ3GWTRLRUHONBACLXADFWE","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":"6547544bab1fc4452a64004fdb87aef3421ac50f06e5547b4e0070861f3fedbf","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2012-07-10T15:16:41Z","title_canon_sha256":"455ca68e238fbc7570fcac50bb6d18b54e4e7a4257927e6d99dab0fdb43940c8"},"schema_version":"1.0","source":{"id":"1207.2387","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1207.2387","created_at":"2026-05-18T03:51:24Z"},{"alias_kind":"arxiv_version","alias_value":"1207.2387v1","created_at":"2026-05-18T03:51:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.2387","created_at":"2026-05-18T03:51:24Z"},{"alias_kind":"pith_short_12","alias_value":"M6TWZ3GWTRLR","created_at":"2026-05-18T12:27:14Z"},{"alias_kind":"pith_short_16","alias_value":"M6TWZ3GWTRLRUHON","created_at":"2026-05-18T12:27:14Z"},{"alias_kind":"pith_short_8","alias_value":"M6TWZ3GW","created_at":"2026-05-18T12:27:14Z"}],"graph_snapshots":[{"event_id":"sha256:31e6da544561133a4b6f41a450564a186dfa4d7cfe47dc2c4ba978825887e32e","target":"graph","created_at":"2026-05-18T03:51:24Z","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":"The nonequilibrium transfer of the energy between electrons of counter-propagating quasi-one-dimensional systems has been perturbatively calculated for edge channels in a two-dimensional system in the integer quantum Hall effect. The processes involving two electrons that are allowed only in the system with disorder have been taken into account. Expressions for the cases of Coulomb scattering and transfer of nonequilibrium phonons have been obtained. The energy transferred per unit time has a quasi-threshold dependence on the degree of nonequilibrium of the hot channel. According to numerical ","authors_text":"M. G. Prokudina, V. S. Khrapai","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2012-07-10T15:16:41Z","title":"Pair Scattering of Electrons in Edge Channels of Opposite Chiralities in the Presence of a Disorder Potential"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.2387","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:df6521029dd0753436123851a103edd9112e5d0316ac7f2230838571fe6a1b24","target":"record","created_at":"2026-05-18T03:51:24Z","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":"6547544bab1fc4452a64004fdb87aef3421ac50f06e5547b4e0070861f3fedbf","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2012-07-10T15:16:41Z","title_canon_sha256":"455ca68e238fbc7570fcac50bb6d18b54e4e7a4257927e6d99dab0fdb43940c8"},"schema_version":"1.0","source":{"id":"1207.2387","kind":"arxiv","version":1}},"canonical_sha256":"67a76cecd69c571a1dcd0804bb8065b11f67d939affd27f6e173b3c1d535f718","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"67a76cecd69c571a1dcd0804bb8065b11f67d939affd27f6e173b3c1d535f718","first_computed_at":"2026-05-18T03:51:24.238492Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:51:24.238492Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"01NWHWRMHQcVKqm+VTIpX8+QQHVxqd7Tskvp7LOsybQUe+tmzmrgDnwSSJPeXfdvn4Y4pemtnTMmlmotBpULDw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:51:24.238949Z","signed_message":"canonical_sha256_bytes"},"source_id":"1207.2387","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:df6521029dd0753436123851a103edd9112e5d0316ac7f2230838571fe6a1b24","sha256:31e6da544561133a4b6f41a450564a186dfa4d7cfe47dc2c4ba978825887e32e"],"state_sha256":"6b1417bd713a3d3a16f8973b2b4bab5a5c0f2132bb63ade50086f698386b5f34"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8durNsJo19WkYShyM/g+WN/PDhUveXsuSBG1CL83uI19D/0rZj8FW/onkC5J2O1AOKyjAbRqRXOfx+tunE2bBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T08:11:49.202279Z","bundle_sha256":"642ad0397d85141d5320a7c1e969a632571fb798ed13926d5a8c7cf0fc0c1115"}}