{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:ASFPAIR4X5JNRDEWFBXFILTIFQ","short_pith_number":"pith:ASFPAIR4","canonical_record":{"source":{"id":"1303.4144","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2013-03-18T02:58:02Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.mtrl-sci","cond-mat.str-el"],"title_canon_sha256":"b0f4bb43db423fe90757e8f95bad5086c3e52e3a516e666fe847faf1821dfcfe","abstract_canon_sha256":"a0543bf50d6abc14d9c9c6771ebd4a2c0de4929b24c979297d8d576540ede972"},"schema_version":"1.0"},"canonical_sha256":"048af0223cbf52d88c96286e542e682c313e9c2b9163825f6a7d7956bfd39825","source":{"kind":"arxiv","id":"1303.4144","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.4144","created_at":"2026-05-18T03:16:49Z"},{"alias_kind":"arxiv_version","alias_value":"1303.4144v2","created_at":"2026-05-18T03:16:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.4144","created_at":"2026-05-18T03:16:49Z"},{"alias_kind":"pith_short_12","alias_value":"ASFPAIR4X5JN","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_16","alias_value":"ASFPAIR4X5JNRDEW","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_8","alias_value":"ASFPAIR4","created_at":"2026-05-18T12:27:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:ASFPAIR4X5JNRDEWFBXFILTIFQ","target":"record","payload":{"canonical_record":{"source":{"id":"1303.4144","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2013-03-18T02:58:02Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.mtrl-sci","cond-mat.str-el"],"title_canon_sha256":"b0f4bb43db423fe90757e8f95bad5086c3e52e3a516e666fe847faf1821dfcfe","abstract_canon_sha256":"a0543bf50d6abc14d9c9c6771ebd4a2c0de4929b24c979297d8d576540ede972"},"schema_version":"1.0"},"canonical_sha256":"048af0223cbf52d88c96286e542e682c313e9c2b9163825f6a7d7956bfd39825","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:16:49.345403Z","signature_b64":"G3visKUKRJQZssfWqgeHP7WMmvPwZoeR76yolBFWjNnslfUXCXF9p+TCKT/QR5T+YC1KCUie4k2QOuGLWTIVAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"048af0223cbf52d88c96286e542e682c313e9c2b9163825f6a7d7956bfd39825","last_reissued_at":"2026-05-18T03:16:49.344862Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:16:49.344862Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1303.4144","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":"2026-05-18T03:16:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1Ml4PdTSAkcEgVD1paQ1V5SFsQ7tHygGwqBABWIHlKFPz9X9MKS7EtRtqfSl+PpCeonxvwFFBbub4AxvPwYJAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T20:04:19.865984Z"},"content_sha256":"ba093c279f51e4c03ab80d5c006bb86347a44e14ed92bca77764cc90ac69c6c8","schema_version":"1.0","event_id":"sha256:ba093c279f51e4c03ab80d5c006bb86347a44e14ed92bca77764cc90ac69c6c8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:ASFPAIR4X5JNRDEWFBXFILTIFQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Topological Mirror Superconductivity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.mtrl-sci","cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"C. L. Kane, E. J. Mele, Fan Zhang","submitted_at":"2013-03-18T02:58:02Z","abstract_excerpt":"We demonstrate the existence of topological superconductors (SC) protected by mirror and time reversal (TR) symmetries. D-dimensional (D=1,2,3) crystalline SCs are characterized by 2^(D-1) independent integer topological invariants, which take the form of mirror Berry phases. These invariants determine the distribution of Majorana modes on a mirror symmetric boundary. The parity of total mirror Berry phase is the Z_2 index of a class DIII SC, implying that a DIII topological SC with a mirror line must also be a topological mirror SC but not vice versa, and that a DIII SC with a mirror plane is"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.4144","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":"2026-05-18T03:16:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"80VrOcDwiPq/N8yzpoV2gM9vWKVkxstabkMqxngCmM4WIOXI7qHZmBGCdTrLP2dNCYKkBDj+fJSy56NNt7sAAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T20:04:19.866693Z"},"content_sha256":"e8c10bc96e7b802e6aa25e4281dc32826a821a396075051c0ca413900e77305e","schema_version":"1.0","event_id":"sha256:e8c10bc96e7b802e6aa25e4281dc32826a821a396075051c0ca413900e77305e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ASFPAIR4X5JNRDEWFBXFILTIFQ/bundle.json","state_url":"https://pith.science/pith/ASFPAIR4X5JNRDEWFBXFILTIFQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ASFPAIR4X5JNRDEWFBXFILTIFQ/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":"2026-05-28T20:04:19Z","links":{"resolver":"https://pith.science/pith/ASFPAIR4X5JNRDEWFBXFILTIFQ","bundle":"https://pith.science/pith/ASFPAIR4X5JNRDEWFBXFILTIFQ/bundle.json","state":"https://pith.science/pith/ASFPAIR4X5JNRDEWFBXFILTIFQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ASFPAIR4X5JNRDEWFBXFILTIFQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:ASFPAIR4X5JNRDEWFBXFILTIFQ","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":"a0543bf50d6abc14d9c9c6771ebd4a2c0de4929b24c979297d8d576540ede972","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.mtrl-sci","cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2013-03-18T02:58:02Z","title_canon_sha256":"b0f4bb43db423fe90757e8f95bad5086c3e52e3a516e666fe847faf1821dfcfe"},"schema_version":"1.0","source":{"id":"1303.4144","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.4144","created_at":"2026-05-18T03:16:49Z"},{"alias_kind":"arxiv_version","alias_value":"1303.4144v2","created_at":"2026-05-18T03:16:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.4144","created_at":"2026-05-18T03:16:49Z"},{"alias_kind":"pith_short_12","alias_value":"ASFPAIR4X5JN","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_16","alias_value":"ASFPAIR4X5JNRDEW","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_8","alias_value":"ASFPAIR4","created_at":"2026-05-18T12:27:38Z"}],"graph_snapshots":[{"event_id":"sha256:e8c10bc96e7b802e6aa25e4281dc32826a821a396075051c0ca413900e77305e","target":"graph","created_at":"2026-05-18T03:16:49Z","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 demonstrate the existence of topological superconductors (SC) protected by mirror and time reversal (TR) symmetries. D-dimensional (D=1,2,3) crystalline SCs are characterized by 2^(D-1) independent integer topological invariants, which take the form of mirror Berry phases. These invariants determine the distribution of Majorana modes on a mirror symmetric boundary. The parity of total mirror Berry phase is the Z_2 index of a class DIII SC, implying that a DIII topological SC with a mirror line must also be a topological mirror SC but not vice versa, and that a DIII SC with a mirror plane is","authors_text":"C. L. Kane, E. J. Mele, Fan Zhang","cross_cats":["cond-mat.mes-hall","cond-mat.mtrl-sci","cond-mat.str-el"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2013-03-18T02:58:02Z","title":"Topological Mirror Superconductivity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.4144","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:ba093c279f51e4c03ab80d5c006bb86347a44e14ed92bca77764cc90ac69c6c8","target":"record","created_at":"2026-05-18T03:16:49Z","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":"a0543bf50d6abc14d9c9c6771ebd4a2c0de4929b24c979297d8d576540ede972","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.mtrl-sci","cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2013-03-18T02:58:02Z","title_canon_sha256":"b0f4bb43db423fe90757e8f95bad5086c3e52e3a516e666fe847faf1821dfcfe"},"schema_version":"1.0","source":{"id":"1303.4144","kind":"arxiv","version":2}},"canonical_sha256":"048af0223cbf52d88c96286e542e682c313e9c2b9163825f6a7d7956bfd39825","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"048af0223cbf52d88c96286e542e682c313e9c2b9163825f6a7d7956bfd39825","first_computed_at":"2026-05-18T03:16:49.344862Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:16:49.344862Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"G3visKUKRJQZssfWqgeHP7WMmvPwZoeR76yolBFWjNnslfUXCXF9p+TCKT/QR5T+YC1KCUie4k2QOuGLWTIVAA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:16:49.345403Z","signed_message":"canonical_sha256_bytes"},"source_id":"1303.4144","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ba093c279f51e4c03ab80d5c006bb86347a44e14ed92bca77764cc90ac69c6c8","sha256:e8c10bc96e7b802e6aa25e4281dc32826a821a396075051c0ca413900e77305e"],"state_sha256":"8c8c7beecd6c944d7b29a030385fec3ae10afcec3d94feaacb4939b565d05358"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YDX8vPpNh9K4xFIYFAnpJQpjaWVLoNwvr0UteJuDVJXzDJa0yT8Q2ny/QX5kRmqpvtsofJjnw/8PDAtErjGwDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T20:04:19.870503Z","bundle_sha256":"940da56c41208651e294927fb40125ed102039316f57812b9ef016caff89785f"}}