{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:A5TYTHMC3BGIBOOK5U2OQA5OWE","short_pith_number":"pith:A5TYTHMC","canonical_record":{"source":{"id":"1604.05546","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-04-19T12:52:47Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"c9763e83b3a866049d5c485b293b69eafa004a87c2437a2f5d68eb387c20eaa0","abstract_canon_sha256":"0e4507427bea7551da7382651a6c877b8d7de2e5b848d950cc16f0f6c0101364"},"schema_version":"1.0"},"canonical_sha256":"0767899d82d84c80b9caed34e803aeb11fefd0e6a12ac586431e3476eaf72ead","source":{"kind":"arxiv","id":"1604.05546","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.05546","created_at":"2026-05-18T01:10:59Z"},{"alias_kind":"arxiv_version","alias_value":"1604.05546v2","created_at":"2026-05-18T01:10:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.05546","created_at":"2026-05-18T01:10:59Z"},{"alias_kind":"pith_short_12","alias_value":"A5TYTHMC3BGI","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_16","alias_value":"A5TYTHMC3BGIBOOK","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_8","alias_value":"A5TYTHMC","created_at":"2026-05-18T12:30:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:A5TYTHMC3BGIBOOK5U2OQA5OWE","target":"record","payload":{"canonical_record":{"source":{"id":"1604.05546","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-04-19T12:52:47Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"c9763e83b3a866049d5c485b293b69eafa004a87c2437a2f5d68eb387c20eaa0","abstract_canon_sha256":"0e4507427bea7551da7382651a6c877b8d7de2e5b848d950cc16f0f6c0101364"},"schema_version":"1.0"},"canonical_sha256":"0767899d82d84c80b9caed34e803aeb11fefd0e6a12ac586431e3476eaf72ead","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:10:59.122230Z","signature_b64":"OWxzkE6QMiGACeNuZyyWUrLMBf3/oJgCIjXlSjwNIEgBjSY1EevjMzm5toK83ZOn1EYPzW/rd3xXODBSNlReAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0767899d82d84c80b9caed34e803aeb11fefd0e6a12ac586431e3476eaf72ead","last_reissued_at":"2026-05-18T01:10:59.121584Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:10:59.121584Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1604.05546","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":"2026-05-18T01:10:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qCEd14FM1VtYLX8ZJK37rEyzLhYdjCiA9NCXjl16AKizv8BqzCsTjjNYt5Ah+WrKvs9s9A5d6KF+vjxGfTu/Bg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-19T07:21:34.402987Z"},"content_sha256":"0eb73c50abc1bf1e4220cd44826ade7c1670e97f4d99c5172dc9ad7a005e2341","schema_version":"1.0","event_id":"sha256:0eb73c50abc1bf1e4220cd44826ade7c1670e97f4d99c5172dc9ad7a005e2341"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:A5TYTHMC3BGIBOOK5U2OQA5OWE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Transport through a quantum spin Hall antidot as a spectroscopic probe of spin textures","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mes-hall","authors_text":"Alexia Rod, Giacomo Dolcetto, Stephan Rachel, Thomas L. Schmidt","submitted_at":"2016-04-19T12:52:47Z","abstract_excerpt":"We investigate electron transport through an antidot embedded in a narrow strip of two-dimensional topological insulator. We focus on the most generic and experimentally relevant case with broken axial spin symmetry. Spin-non-conservation allows additional scattering processes which change the transport properties profoundly. We start from an analytical model for noninteracting transport, which we also compare with a numerical tight-binding simulation. We then extend this model by including Coulomb repulsion on the antidot, and we study the transport in the Coulomb-blockade limit. We investiga"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.05546","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":"2026-05-18T01:10:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"O3hNOrPwKCNJOy6wzFbdhIzC7mTBE1EHCzHrCEO7j+nN2XAl9T/lvO1dLvCNKws51359cUV4xdPcwAQBJVRSDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-19T07:21:34.403399Z"},"content_sha256":"e5556e95468c56d5f521422f1097a954058cf86da133874ba8ec13b1eb436109","schema_version":"1.0","event_id":"sha256:e5556e95468c56d5f521422f1097a954058cf86da133874ba8ec13b1eb436109"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/A5TYTHMC3BGIBOOK5U2OQA5OWE/bundle.json","state_url":"https://pith.science/pith/A5TYTHMC3BGIBOOK5U2OQA5OWE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/A5TYTHMC3BGIBOOK5U2OQA5OWE/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":"2026-05-19T07:21:34Z","links":{"resolver":"https://pith.science/pith/A5TYTHMC3BGIBOOK5U2OQA5OWE","bundle":"https://pith.science/pith/A5TYTHMC3BGIBOOK5U2OQA5OWE/bundle.json","state":"https://pith.science/pith/A5TYTHMC3BGIBOOK5U2OQA5OWE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/A5TYTHMC3BGIBOOK5U2OQA5OWE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:A5TYTHMC3BGIBOOK5U2OQA5OWE","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":"0e4507427bea7551da7382651a6c877b8d7de2e5b848d950cc16f0f6c0101364","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-04-19T12:52:47Z","title_canon_sha256":"c9763e83b3a866049d5c485b293b69eafa004a87c2437a2f5d68eb387c20eaa0"},"schema_version":"1.0","source":{"id":"1604.05546","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.05546","created_at":"2026-05-18T01:10:59Z"},{"alias_kind":"arxiv_version","alias_value":"1604.05546v2","created_at":"2026-05-18T01:10:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.05546","created_at":"2026-05-18T01:10:59Z"},{"alias_kind":"pith_short_12","alias_value":"A5TYTHMC3BGI","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_16","alias_value":"A5TYTHMC3BGIBOOK","created_at":"2026-05-18T12:30:04Z"},{"alias_kind":"pith_short_8","alias_value":"A5TYTHMC","created_at":"2026-05-18T12:30:04Z"}],"graph_snapshots":[{"event_id":"sha256:e5556e95468c56d5f521422f1097a954058cf86da133874ba8ec13b1eb436109","target":"graph","created_at":"2026-05-18T01:10:59Z","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 investigate electron transport through an antidot embedded in a narrow strip of two-dimensional topological insulator. We focus on the most generic and experimentally relevant case with broken axial spin symmetry. Spin-non-conservation allows additional scattering processes which change the transport properties profoundly. We start from an analytical model for noninteracting transport, which we also compare with a numerical tight-binding simulation. We then extend this model by including Coulomb repulsion on the antidot, and we study the transport in the Coulomb-blockade limit. We investiga","authors_text":"Alexia Rod, Giacomo Dolcetto, Stephan Rachel, Thomas L. Schmidt","cross_cats":["cond-mat.str-el"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-04-19T12:52:47Z","title":"Transport through a quantum spin Hall antidot as a spectroscopic probe of spin textures"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.05546","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":"sha256:0eb73c50abc1bf1e4220cd44826ade7c1670e97f4d99c5172dc9ad7a005e2341","target":"record","created_at":"2026-05-18T01:10:59Z","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":"0e4507427bea7551da7382651a6c877b8d7de2e5b848d950cc16f0f6c0101364","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-04-19T12:52:47Z","title_canon_sha256":"c9763e83b3a866049d5c485b293b69eafa004a87c2437a2f5d68eb387c20eaa0"},"schema_version":"1.0","source":{"id":"1604.05546","kind":"arxiv","version":2}},"canonical_sha256":"0767899d82d84c80b9caed34e803aeb11fefd0e6a12ac586431e3476eaf72ead","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0767899d82d84c80b9caed34e803aeb11fefd0e6a12ac586431e3476eaf72ead","first_computed_at":"2026-05-18T01:10:59.121584Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:10:59.121584Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"OWxzkE6QMiGACeNuZyyWUrLMBf3/oJgCIjXlSjwNIEgBjSY1EevjMzm5toK83ZOn1EYPzW/rd3xXODBSNlReAw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:10:59.122230Z","signed_message":"canonical_sha256_bytes"},"source_id":"1604.05546","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0eb73c50abc1bf1e4220cd44826ade7c1670e97f4d99c5172dc9ad7a005e2341","sha256:e5556e95468c56d5f521422f1097a954058cf86da133874ba8ec13b1eb436109"],"state_sha256":"ad3219ec8c9684dbcfe79500c64869ca1d91a90eb84a76dd9e9a76df201620da"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Un7sdUuMNUqAXFPkISGPzsw5uiYuPanHsLO9WayCvDVHyZ//wyBsEVdhvCpqCgvNbNmuUf6rfphEC2B8lk3kDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-19T07:21:34.405586Z","bundle_sha256":"5d838b7f762d01ecae4e20cbdb75ff6faf925f7ddebb91a919ac636cdbaccc9b"}}