{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:IQWJG774UNMBK66U6BGEZJIAAI","short_pith_number":"pith:IQWJG774","canonical_record":{"source":{"id":"1109.6068","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2011-09-28T01:03:45Z","cross_cats_sorted":[],"title_canon_sha256":"c6c68e7ab5ef3151d3b6171c49678b9b7f12f83854243c89a27c2e47487cfd44","abstract_canon_sha256":"cdff361eb8be6eae92c0313e28753c27921ad6d73c7d773c3c42948d3df92cd7"},"schema_version":"1.0"},"canonical_sha256":"442c937ffca358157bd4f04c4ca500021e2659a05f97874bbdd4b144eca3c6ac","source":{"kind":"arxiv","id":"1109.6068","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1109.6068","created_at":"2026-05-18T02:00:22Z"},{"alias_kind":"arxiv_version","alias_value":"1109.6068v1","created_at":"2026-05-18T02:00:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1109.6068","created_at":"2026-05-18T02:00:22Z"},{"alias_kind":"pith_short_12","alias_value":"IQWJG774UNMB","created_at":"2026-05-18T12:26:32Z"},{"alias_kind":"pith_short_16","alias_value":"IQWJG774UNMBK66U","created_at":"2026-05-18T12:26:32Z"},{"alias_kind":"pith_short_8","alias_value":"IQWJG774","created_at":"2026-05-18T12:26:32Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:IQWJG774UNMBK66U6BGEZJIAAI","target":"record","payload":{"canonical_record":{"source":{"id":"1109.6068","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2011-09-28T01:03:45Z","cross_cats_sorted":[],"title_canon_sha256":"c6c68e7ab5ef3151d3b6171c49678b9b7f12f83854243c89a27c2e47487cfd44","abstract_canon_sha256":"cdff361eb8be6eae92c0313e28753c27921ad6d73c7d773c3c42948d3df92cd7"},"schema_version":"1.0"},"canonical_sha256":"442c937ffca358157bd4f04c4ca500021e2659a05f97874bbdd4b144eca3c6ac","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:00:22.383120Z","signature_b64":"qXXttYRDzkpHIAqBPQfrTwW7QZ1xQu22lXqu9SFDMPGuxUm7SagLN9w3D5XvjH5AJqSTVKq7uUF/cQUsCamwBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"442c937ffca358157bd4f04c4ca500021e2659a05f97874bbdd4b144eca3c6ac","last_reissued_at":"2026-05-18T02:00:22.382482Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:00:22.382482Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1109.6068","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":"2026-05-18T02:00:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5rMLHpAqnMZiVlNDUkwMNoNXHPkZ8HlncWJMgQ8d+C/n35A5RzUiTxZWukPxbtCAZ2pZjY2d3SGDAYYbjdi5CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T06:47:55.235416Z"},"content_sha256":"0df9fa901344952c50850c2b9822904979ad10cc73b79f201a83e147c25764b4","schema_version":"1.0","event_id":"sha256:0df9fa901344952c50850c2b9822904979ad10cc73b79f201a83e147c25764b4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:IQWJG774UNMBK66U6BGEZJIAAI","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Sub-gap in the Edge States of 2-D Chiral Superconductor with Rough Surface","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"K. Nagai, S. Higashitani, Y. Nagato","submitted_at":"2011-09-28T01:03:45Z","abstract_excerpt":"We discuss the rough surface effects on a two-dimensional chiral $k_x+ik_y$ superconductor. The atomic scale roughness at the surface is considered using the random $S$ matrix model. The roughness effects on the self-consistent order parameter, the surface mass current and the surface density of states are studied using the quasi-classical theory. We find that the surface mass current is suppressed by the surface roughness. The surface density of states shows a quite similar behavior to that of superfluid ${}^3$He B phase. When the surface is specular, the surface Andreev bound states form a b"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1109.6068","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":"2026-05-18T02:00:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ArSq1QQJRf29p7tbw8M3mrb0MQ5xxLtLuAIoF15M0kBUIveXo82UdcZrjG/fEQmUuinORYzABOu7gm5qZYlNCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T06:47:55.235768Z"},"content_sha256":"7d2d58d063502febe5ea90419c3e3de7181a93cff42c1a7a9c104f454f41b6bf","schema_version":"1.0","event_id":"sha256:7d2d58d063502febe5ea90419c3e3de7181a93cff42c1a7a9c104f454f41b6bf"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/IQWJG774UNMBK66U6BGEZJIAAI/bundle.json","state_url":"https://pith.science/pith/IQWJG774UNMBK66U6BGEZJIAAI/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/IQWJG774UNMBK66U6BGEZJIAAI/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":"2026-06-02T06:47:55Z","links":{"resolver":"https://pith.science/pith/IQWJG774UNMBK66U6BGEZJIAAI","bundle":"https://pith.science/pith/IQWJG774UNMBK66U6BGEZJIAAI/bundle.json","state":"https://pith.science/pith/IQWJG774UNMBK66U6BGEZJIAAI/state.json","well_known_bundle":"https://pith.science/.well-known/pith/IQWJG774UNMBK66U6BGEZJIAAI/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:IQWJG774UNMBK66U6BGEZJIAAI","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":"cdff361eb8be6eae92c0313e28753c27921ad6d73c7d773c3c42948d3df92cd7","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2011-09-28T01:03:45Z","title_canon_sha256":"c6c68e7ab5ef3151d3b6171c49678b9b7f12f83854243c89a27c2e47487cfd44"},"schema_version":"1.0","source":{"id":"1109.6068","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1109.6068","created_at":"2026-05-18T02:00:22Z"},{"alias_kind":"arxiv_version","alias_value":"1109.6068v1","created_at":"2026-05-18T02:00:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1109.6068","created_at":"2026-05-18T02:00:22Z"},{"alias_kind":"pith_short_12","alias_value":"IQWJG774UNMB","created_at":"2026-05-18T12:26:32Z"},{"alias_kind":"pith_short_16","alias_value":"IQWJG774UNMBK66U","created_at":"2026-05-18T12:26:32Z"},{"alias_kind":"pith_short_8","alias_value":"IQWJG774","created_at":"2026-05-18T12:26:32Z"}],"graph_snapshots":[{"event_id":"sha256:7d2d58d063502febe5ea90419c3e3de7181a93cff42c1a7a9c104f454f41b6bf","target":"graph","created_at":"2026-05-18T02:00:22Z","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 discuss the rough surface effects on a two-dimensional chiral $k_x+ik_y$ superconductor. The atomic scale roughness at the surface is considered using the random $S$ matrix model. The roughness effects on the self-consistent order parameter, the surface mass current and the surface density of states are studied using the quasi-classical theory. We find that the surface mass current is suppressed by the surface roughness. The surface density of states shows a quite similar behavior to that of superfluid ${}^3$He B phase. When the surface is specular, the surface Andreev bound states form a b","authors_text":"K. Nagai, S. Higashitani, Y. Nagato","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2011-09-28T01:03:45Z","title":"Sub-gap in the Edge States of 2-D Chiral Superconductor with Rough Surface"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1109.6068","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":"sha256:0df9fa901344952c50850c2b9822904979ad10cc73b79f201a83e147c25764b4","target":"record","created_at":"2026-05-18T02:00:22Z","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":"cdff361eb8be6eae92c0313e28753c27921ad6d73c7d773c3c42948d3df92cd7","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2011-09-28T01:03:45Z","title_canon_sha256":"c6c68e7ab5ef3151d3b6171c49678b9b7f12f83854243c89a27c2e47487cfd44"},"schema_version":"1.0","source":{"id":"1109.6068","kind":"arxiv","version":1}},"canonical_sha256":"442c937ffca358157bd4f04c4ca500021e2659a05f97874bbdd4b144eca3c6ac","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"442c937ffca358157bd4f04c4ca500021e2659a05f97874bbdd4b144eca3c6ac","first_computed_at":"2026-05-18T02:00:22.382482Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:00:22.382482Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"qXXttYRDzkpHIAqBPQfrTwW7QZ1xQu22lXqu9SFDMPGuxUm7SagLN9w3D5XvjH5AJqSTVKq7uUF/cQUsCamwBw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:00:22.383120Z","signed_message":"canonical_sha256_bytes"},"source_id":"1109.6068","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0df9fa901344952c50850c2b9822904979ad10cc73b79f201a83e147c25764b4","sha256:7d2d58d063502febe5ea90419c3e3de7181a93cff42c1a7a9c104f454f41b6bf"],"state_sha256":"7df9f9aafde558f80eedefa850288928586e3599324037ba1d84d14f94cf6623"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"94NlpZlhgh6jf1tTte6e4xzwhxikMw1DG/Yp68hy0vOcPQqyBa2ibN9ugMeYvMjavrgH5/lIM+PKJObo98oEDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T06:47:55.237709Z","bundle_sha256":"9c45ed77af599e1495d4163e1959fe144fd60c8a0e402d8e4b6ad10ed8f4e801"}}