{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:IZ4MUTMDC4PX6EXUJISM2UBYLY","short_pith_number":"pith:IZ4MUTMD","canonical_record":{"source":{"id":"1702.03909","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-02-13T18:24:07Z","cross_cats_sorted":[],"title_canon_sha256":"0686c0953bc599d4a5282c5a02889af9b140fecf77626dcb07f1e3d11199c7a6","abstract_canon_sha256":"6e4f374c2636bcb5280085f521a3725930991768ab6f2d5ca0da12c773a40048"},"schema_version":"1.0"},"canonical_sha256":"4678ca4d83171f7f12f44a24cd50385e0c869e7c64564da36e671c71688ffd05","source":{"kind":"arxiv","id":"1702.03909","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1702.03909","created_at":"2026-05-18T00:38:03Z"},{"alias_kind":"arxiv_version","alias_value":"1702.03909v2","created_at":"2026-05-18T00:38:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.03909","created_at":"2026-05-18T00:38:03Z"},{"alias_kind":"pith_short_12","alias_value":"IZ4MUTMDC4PX","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_16","alias_value":"IZ4MUTMDC4PX6EXU","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_8","alias_value":"IZ4MUTMD","created_at":"2026-05-18T12:31:21Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:IZ4MUTMDC4PX6EXUJISM2UBYLY","target":"record","payload":{"canonical_record":{"source":{"id":"1702.03909","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-02-13T18:24:07Z","cross_cats_sorted":[],"title_canon_sha256":"0686c0953bc599d4a5282c5a02889af9b140fecf77626dcb07f1e3d11199c7a6","abstract_canon_sha256":"6e4f374c2636bcb5280085f521a3725930991768ab6f2d5ca0da12c773a40048"},"schema_version":"1.0"},"canonical_sha256":"4678ca4d83171f7f12f44a24cd50385e0c869e7c64564da36e671c71688ffd05","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:38:03.571592Z","signature_b64":"Q8BJ5F11fUYvIvi34wlD9lkozm1vLsNkBq900rGx5Kz1ggNcUQMEoSTpaTb0s34vihxSkT7vIFVzdw9OYA+GBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4678ca4d83171f7f12f44a24cd50385e0c869e7c64564da36e671c71688ffd05","last_reissued_at":"2026-05-18T00:38:03.571073Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:38:03.571073Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1702.03909","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":"2026-05-18T00:38:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7RUoeo478XIuQsOrT2DygVK6rq2BgGcr9Yp65HM4kSMUqANLPLqgMnfrjFrH3zHeOjfLeWpTJzc5h2C6MHtlAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T09:40:19.508556Z"},"content_sha256":"e6c9ee60fae4f4e649357bc45071e870d3497ab79898a49081ffebf18823e182","schema_version":"1.0","event_id":"sha256:e6c9ee60fae4f4e649357bc45071e870d3497ab79898a49081ffebf18823e182"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:IZ4MUTMDC4PX6EXUJISM2UBYLY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Fano Resonances in Majorana Bound States - Quantum Dot Hybrid Systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Alexander Schuray, Luzie Weithofer, Patrik Recher","submitted_at":"2017-02-13T18:24:07Z","abstract_excerpt":"We consider a quantum wire, containing two Majorana bound states (MBS) at its ends that are coupled to a current lead on one side and to a quantum dot (QD) on the other side. Using the method of full counting statistics we calculate the conductance and the zero-frequency noise. Using an effective low-energy model, we analyze in detail the Andreev reflection probability as a function of the various system parameters and show that it exhibits a Fano resonance (FR) line shape in the case of a weakly coupled QD as a function of the QD energy level when the two MBS overlap. The asymmetry parameter "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.03909","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":"2026-05-18T00:38:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LyBlvNVKu9fTuQUbDy4MXGjvKjb7GRHpQGMZTiUmaHVMyfq5q7R5cFrSUy54mRYj3OzjgiV3vUy8S30d90YDBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T09:40:19.508893Z"},"content_sha256":"6c70270436658f5df01475228dcdaed073bc4a89dca9727e6d55f7e9042247f9","schema_version":"1.0","event_id":"sha256:6c70270436658f5df01475228dcdaed073bc4a89dca9727e6d55f7e9042247f9"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/IZ4MUTMDC4PX6EXUJISM2UBYLY/bundle.json","state_url":"https://pith.science/pith/IZ4MUTMDC4PX6EXUJISM2UBYLY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/IZ4MUTMDC4PX6EXUJISM2UBYLY/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":"2026-06-09T09:40:19Z","links":{"resolver":"https://pith.science/pith/IZ4MUTMDC4PX6EXUJISM2UBYLY","bundle":"https://pith.science/pith/IZ4MUTMDC4PX6EXUJISM2UBYLY/bundle.json","state":"https://pith.science/pith/IZ4MUTMDC4PX6EXUJISM2UBYLY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/IZ4MUTMDC4PX6EXUJISM2UBYLY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:IZ4MUTMDC4PX6EXUJISM2UBYLY","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":"6e4f374c2636bcb5280085f521a3725930991768ab6f2d5ca0da12c773a40048","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-02-13T18:24:07Z","title_canon_sha256":"0686c0953bc599d4a5282c5a02889af9b140fecf77626dcb07f1e3d11199c7a6"},"schema_version":"1.0","source":{"id":"1702.03909","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1702.03909","created_at":"2026-05-18T00:38:03Z"},{"alias_kind":"arxiv_version","alias_value":"1702.03909v2","created_at":"2026-05-18T00:38:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.03909","created_at":"2026-05-18T00:38:03Z"},{"alias_kind":"pith_short_12","alias_value":"IZ4MUTMDC4PX","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_16","alias_value":"IZ4MUTMDC4PX6EXU","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_8","alias_value":"IZ4MUTMD","created_at":"2026-05-18T12:31:21Z"}],"graph_snapshots":[{"event_id":"sha256:6c70270436658f5df01475228dcdaed073bc4a89dca9727e6d55f7e9042247f9","target":"graph","created_at":"2026-05-18T00:38:03Z","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 consider a quantum wire, containing two Majorana bound states (MBS) at its ends that are coupled to a current lead on one side and to a quantum dot (QD) on the other side. Using the method of full counting statistics we calculate the conductance and the zero-frequency noise. Using an effective low-energy model, we analyze in detail the Andreev reflection probability as a function of the various system parameters and show that it exhibits a Fano resonance (FR) line shape in the case of a weakly coupled QD as a function of the QD energy level when the two MBS overlap. The asymmetry parameter ","authors_text":"Alexander Schuray, Luzie Weithofer, Patrik Recher","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-02-13T18:24:07Z","title":"Fano Resonances in Majorana Bound States - Quantum Dot Hybrid Systems"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.03909","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:e6c9ee60fae4f4e649357bc45071e870d3497ab79898a49081ffebf18823e182","target":"record","created_at":"2026-05-18T00:38:03Z","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":"6e4f374c2636bcb5280085f521a3725930991768ab6f2d5ca0da12c773a40048","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-02-13T18:24:07Z","title_canon_sha256":"0686c0953bc599d4a5282c5a02889af9b140fecf77626dcb07f1e3d11199c7a6"},"schema_version":"1.0","source":{"id":"1702.03909","kind":"arxiv","version":2}},"canonical_sha256":"4678ca4d83171f7f12f44a24cd50385e0c869e7c64564da36e671c71688ffd05","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4678ca4d83171f7f12f44a24cd50385e0c869e7c64564da36e671c71688ffd05","first_computed_at":"2026-05-18T00:38:03.571073Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:38:03.571073Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Q8BJ5F11fUYvIvi34wlD9lkozm1vLsNkBq900rGx5Kz1ggNcUQMEoSTpaTb0s34vihxSkT7vIFVzdw9OYA+GBA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:38:03.571592Z","signed_message":"canonical_sha256_bytes"},"source_id":"1702.03909","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e6c9ee60fae4f4e649357bc45071e870d3497ab79898a49081ffebf18823e182","sha256:6c70270436658f5df01475228dcdaed073bc4a89dca9727e6d55f7e9042247f9"],"state_sha256":"eca2c0e8530776660c31b45a4c80f9e55614617eccbda181b725afd528fbfc32"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nwRtyETOxFy/c8mVfL45VqLpZjxpCBMLlMp4Q0Qz9Zu5eEo+QXS1ER/8t1oh5Fd5CzWbk+Ai0tc2XYDdZgGkDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-09T09:40:19.510667Z","bundle_sha256":"468dd0c3c942c4f1056b8bf897309b48ffd5341042a2db584c1f46e4c6eeb121"}}