{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:KXCH3XYN4FJ37NICWGEFAMDBYD","short_pith_number":"pith:KXCH3XYN","canonical_record":{"source":{"id":"1310.3733","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-10-14T16:11:11Z","cross_cats_sorted":[],"title_canon_sha256":"83456857c7b7072f2d609701b8fca267c0a4efc8d66f339b1e3a18761171f7f6","abstract_canon_sha256":"7be586d70fc3b379b0dbd0577ea1c724bb8dce908e13f293252e61157d3ae4ef"},"schema_version":"1.0"},"canonical_sha256":"55c47ddf0de153bfb502b188503061c0d532a8ba91fac3576bceaeaa527196b6","source":{"kind":"arxiv","id":"1310.3733","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1310.3733","created_at":"2026-05-18T03:06:21Z"},{"alias_kind":"arxiv_version","alias_value":"1310.3733v2","created_at":"2026-05-18T03:06:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.3733","created_at":"2026-05-18T03:06:21Z"},{"alias_kind":"pith_short_12","alias_value":"KXCH3XYN4FJ3","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_16","alias_value":"KXCH3XYN4FJ37NIC","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_8","alias_value":"KXCH3XYN","created_at":"2026-05-18T12:27:51Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:KXCH3XYN4FJ37NICWGEFAMDBYD","target":"record","payload":{"canonical_record":{"source":{"id":"1310.3733","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-10-14T16:11:11Z","cross_cats_sorted":[],"title_canon_sha256":"83456857c7b7072f2d609701b8fca267c0a4efc8d66f339b1e3a18761171f7f6","abstract_canon_sha256":"7be586d70fc3b379b0dbd0577ea1c724bb8dce908e13f293252e61157d3ae4ef"},"schema_version":"1.0"},"canonical_sha256":"55c47ddf0de153bfb502b188503061c0d532a8ba91fac3576bceaeaa527196b6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:06:21.551776Z","signature_b64":"UZPakk8SsJ5Rr7n0sz8b/LF/gUi2dvYWms6RUAaumTVmUD4QhmSZzoqTLTBgJr7KLRUn0mWVBU+AFLB8WU84CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"55c47ddf0de153bfb502b188503061c0d532a8ba91fac3576bceaeaa527196b6","last_reissued_at":"2026-05-18T03:06:21.551254Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:06:21.551254Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1310.3733","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":"2026-05-18T03:06:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2kDQl6gK3UrsmfgiB3WgSD0tI2j3McWwxB89oOxPJHiQ/JueZQy8GMyHBs7ui3qC/p34BWh4w2MUlnnhjgGLCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T15:40:37.986604Z"},"content_sha256":"05cd9b9c1e72a6972faad2e72eadfaddb19d7d54e25d2f56a4716cadfde9ab13","schema_version":"1.0","event_id":"sha256:05cd9b9c1e72a6972faad2e72eadfaddb19d7d54e25d2f56a4716cadfde9ab13"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:KXCH3XYN4FJ37NICWGEFAMDBYD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Standard form of the scattering matrix for time reversal symmetric system","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Feng Zhai, Xiaoli Lu, Yongjin Jiang","submitted_at":"2013-10-14T16:11:11Z","abstract_excerpt":"In this paper, we present the standard form of the scattering matrix of mesocopic system with spin-orbital coupling which preserves time reversal symmetry. We found some analytical structure of the scattering matrix related to the sub-matrices between arbitrary two channels. In particular, we proved that in the two-terminal mono-channel scattering problem, the transmission matrix is proportional to a SU(2) matrix. We obtained these properties through direct and elementary way and found it in agreement with polar decomposition known before."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.3733","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":"2026-05-18T03:06:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"MpBfi/QmJDde4Fl8xIE2L5Hgjv7xwgETl8UhYh1+dRl4eSzTy0zNKFO61qg/vLBCj0MK7vr9A3KcsvWX1uYBDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T15:40:37.986945Z"},"content_sha256":"0cb63e2e553ea74ab3a86c09e1e9534cee932ccf8b9b006a9d5b6ba6e77bfb0b","schema_version":"1.0","event_id":"sha256:0cb63e2e553ea74ab3a86c09e1e9534cee932ccf8b9b006a9d5b6ba6e77bfb0b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KXCH3XYN4FJ37NICWGEFAMDBYD/bundle.json","state_url":"https://pith.science/pith/KXCH3XYN4FJ37NICWGEFAMDBYD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KXCH3XYN4FJ37NICWGEFAMDBYD/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":"2026-05-31T15:40:37Z","links":{"resolver":"https://pith.science/pith/KXCH3XYN4FJ37NICWGEFAMDBYD","bundle":"https://pith.science/pith/KXCH3XYN4FJ37NICWGEFAMDBYD/bundle.json","state":"https://pith.science/pith/KXCH3XYN4FJ37NICWGEFAMDBYD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KXCH3XYN4FJ37NICWGEFAMDBYD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:KXCH3XYN4FJ37NICWGEFAMDBYD","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":"7be586d70fc3b379b0dbd0577ea1c724bb8dce908e13f293252e61157d3ae4ef","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-10-14T16:11:11Z","title_canon_sha256":"83456857c7b7072f2d609701b8fca267c0a4efc8d66f339b1e3a18761171f7f6"},"schema_version":"1.0","source":{"id":"1310.3733","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1310.3733","created_at":"2026-05-18T03:06:21Z"},{"alias_kind":"arxiv_version","alias_value":"1310.3733v2","created_at":"2026-05-18T03:06:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.3733","created_at":"2026-05-18T03:06:21Z"},{"alias_kind":"pith_short_12","alias_value":"KXCH3XYN4FJ3","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_16","alias_value":"KXCH3XYN4FJ37NIC","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_8","alias_value":"KXCH3XYN","created_at":"2026-05-18T12:27:51Z"}],"graph_snapshots":[{"event_id":"sha256:0cb63e2e553ea74ab3a86c09e1e9534cee932ccf8b9b006a9d5b6ba6e77bfb0b","target":"graph","created_at":"2026-05-18T03:06:21Z","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":"In this paper, we present the standard form of the scattering matrix of mesocopic system with spin-orbital coupling which preserves time reversal symmetry. We found some analytical structure of the scattering matrix related to the sub-matrices between arbitrary two channels. In particular, we proved that in the two-terminal mono-channel scattering problem, the transmission matrix is proportional to a SU(2) matrix. We obtained these properties through direct and elementary way and found it in agreement with polar decomposition known before.","authors_text":"Feng Zhai, Xiaoli Lu, Yongjin Jiang","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-10-14T16:11:11Z","title":"Standard form of the scattering matrix for time reversal symmetric system"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.3733","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":"sha256:05cd9b9c1e72a6972faad2e72eadfaddb19d7d54e25d2f56a4716cadfde9ab13","target":"record","created_at":"2026-05-18T03:06:21Z","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":"7be586d70fc3b379b0dbd0577ea1c724bb8dce908e13f293252e61157d3ae4ef","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-10-14T16:11:11Z","title_canon_sha256":"83456857c7b7072f2d609701b8fca267c0a4efc8d66f339b1e3a18761171f7f6"},"schema_version":"1.0","source":{"id":"1310.3733","kind":"arxiv","version":2}},"canonical_sha256":"55c47ddf0de153bfb502b188503061c0d532a8ba91fac3576bceaeaa527196b6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"55c47ddf0de153bfb502b188503061c0d532a8ba91fac3576bceaeaa527196b6","first_computed_at":"2026-05-18T03:06:21.551254Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:06:21.551254Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"UZPakk8SsJ5Rr7n0sz8b/LF/gUi2dvYWms6RUAaumTVmUD4QhmSZzoqTLTBgJr7KLRUn0mWVBU+AFLB8WU84CA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:06:21.551776Z","signed_message":"canonical_sha256_bytes"},"source_id":"1310.3733","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:05cd9b9c1e72a6972faad2e72eadfaddb19d7d54e25d2f56a4716cadfde9ab13","sha256:0cb63e2e553ea74ab3a86c09e1e9534cee932ccf8b9b006a9d5b6ba6e77bfb0b"],"state_sha256":"9392667afdc3c07ff35fead50863cb1b250a6b15e36dd8d116fcd5abe6040ac7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"i0xMwK7NSVKS7HJjaWk8bz5/pAzsSlvyartAq6bZHLxVV1GQ9Sez6KCWHSsPJjtgLPdhm9EuAlPn2avHypASCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T15:40:37.988868Z","bundle_sha256":"0d0dd1b445a431b65c7ecd0181a8989074aca5147224f0ee8940bfb4fdc13b97"}}