{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:5MMPFXMSFAV23543FSKPPHTIVY","short_pith_number":"pith:5MMPFXMS","canonical_record":{"source":{"id":"1312.2602","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2013-12-09T21:20:47Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.supr-con"],"title_canon_sha256":"bbd7dcb323e2530651b44e92b5f15977b3c6936ea94cf07a2519b7c0a94f844f","abstract_canon_sha256":"874eb1e310ddbd8b87eb54af215874020670cfbcd3233b851ccc608fa30e0ad1"},"schema_version":"1.0"},"canonical_sha256":"eb18f2dd92282badf79b2c94f79e68ae22250cb884f09341eb83cdc83ef49278","source":{"kind":"arxiv","id":"1312.2602","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1312.2602","created_at":"2026-05-18T02:41:24Z"},{"alias_kind":"arxiv_version","alias_value":"1312.2602v1","created_at":"2026-05-18T02:41:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.2602","created_at":"2026-05-18T02:41:24Z"},{"alias_kind":"pith_short_12","alias_value":"5MMPFXMSFAV2","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_16","alias_value":"5MMPFXMSFAV23543","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_8","alias_value":"5MMPFXMS","created_at":"2026-05-18T12:27:34Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:5MMPFXMSFAV23543FSKPPHTIVY","target":"record","payload":{"canonical_record":{"source":{"id":"1312.2602","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2013-12-09T21:20:47Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.supr-con"],"title_canon_sha256":"bbd7dcb323e2530651b44e92b5f15977b3c6936ea94cf07a2519b7c0a94f844f","abstract_canon_sha256":"874eb1e310ddbd8b87eb54af215874020670cfbcd3233b851ccc608fa30e0ad1"},"schema_version":"1.0"},"canonical_sha256":"eb18f2dd92282badf79b2c94f79e68ae22250cb884f09341eb83cdc83ef49278","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:41:24.870156Z","signature_b64":"NSbBaehx0ujBMXNjZj9CypkSP36YereKONK2n1Tr41eitCgNP76iRglHF9YJqbcLaH8s7nZyNJfuIxPKltTdBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"eb18f2dd92282badf79b2c94f79e68ae22250cb884f09341eb83cdc83ef49278","last_reissued_at":"2026-05-18T02:41:24.869766Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:41:24.869766Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1312.2602","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":"2026-05-18T02:41:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3tH5c08B9ztcBO0Hp7tLzc6UcsOBj5uMVIbdkaExLIzVu5jHV/x0LB9JgxiYBtGlhACVKi/NM2wyPdLeN8kWDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-22T11:59:42.721528Z"},"content_sha256":"e958d869d4c1be97dfdb3eac840682b40dd78958f960f8b4dfddd407cd8e32c4","schema_version":"1.0","event_id":"sha256:e958d869d4c1be97dfdb3eac840682b40dd78958f960f8b4dfddd407cd8e32c4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:5MMPFXMSFAV23543FSKPPHTIVY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Non-equilibrium theory of tunneling into localized state in superconductor","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.supr-con"],"primary_cat":"cond-mat.str-el","authors_text":"Dmitry Mozyrsky, Ivar Martin","submitted_at":"2013-12-09T21:20:47Z","abstract_excerpt":"A single static magnetic impurity in a fully-gapped superconductor leads to formation of an intragap quasiparticle bound state. At temperatures much below the superconducting transition, the energy relaxation and spin dephasing of the state are expected to be exponentially suppressed. The presence of such a state can be detected in electron tunneling experiments as a pair of conductance peaks at positive and negative biases. Here we show, that for an arbitrarily weak tunneling strength, the peaks have to be symmetric with respect to the applied bias. This is in contrast to the standard result "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.2602","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":"2026-05-18T02:41:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HBQaOi5rl3saN7+q/TRMXVrvsrXGhqdgCXkKDgEEjM6ou20WxYK/E03MsoYBSITsWwSwkNxa6/0k36AgEEWwAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-22T11:59:42.721901Z"},"content_sha256":"bc2f8376546b970b9f2106251a96484e1b8532490d43cfdbda056eadfeb4723e","schema_version":"1.0","event_id":"sha256:bc2f8376546b970b9f2106251a96484e1b8532490d43cfdbda056eadfeb4723e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5MMPFXMSFAV23543FSKPPHTIVY/bundle.json","state_url":"https://pith.science/pith/5MMPFXMSFAV23543FSKPPHTIVY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5MMPFXMSFAV23543FSKPPHTIVY/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":"2026-06-22T11:59:42Z","links":{"resolver":"https://pith.science/pith/5MMPFXMSFAV23543FSKPPHTIVY","bundle":"https://pith.science/pith/5MMPFXMSFAV23543FSKPPHTIVY/bundle.json","state":"https://pith.science/pith/5MMPFXMSFAV23543FSKPPHTIVY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5MMPFXMSFAV23543FSKPPHTIVY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:5MMPFXMSFAV23543FSKPPHTIVY","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":"874eb1e310ddbd8b87eb54af215874020670cfbcd3233b851ccc608fa30e0ad1","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.supr-con"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2013-12-09T21:20:47Z","title_canon_sha256":"bbd7dcb323e2530651b44e92b5f15977b3c6936ea94cf07a2519b7c0a94f844f"},"schema_version":"1.0","source":{"id":"1312.2602","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1312.2602","created_at":"2026-05-18T02:41:24Z"},{"alias_kind":"arxiv_version","alias_value":"1312.2602v1","created_at":"2026-05-18T02:41:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.2602","created_at":"2026-05-18T02:41:24Z"},{"alias_kind":"pith_short_12","alias_value":"5MMPFXMSFAV2","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_16","alias_value":"5MMPFXMSFAV23543","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_8","alias_value":"5MMPFXMS","created_at":"2026-05-18T12:27:34Z"}],"graph_snapshots":[{"event_id":"sha256:bc2f8376546b970b9f2106251a96484e1b8532490d43cfdbda056eadfeb4723e","target":"graph","created_at":"2026-05-18T02:41:24Z","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":"A single static magnetic impurity in a fully-gapped superconductor leads to formation of an intragap quasiparticle bound state. At temperatures much below the superconducting transition, the energy relaxation and spin dephasing of the state are expected to be exponentially suppressed. The presence of such a state can be detected in electron tunneling experiments as a pair of conductance peaks at positive and negative biases. Here we show, that for an arbitrarily weak tunneling strength, the peaks have to be symmetric with respect to the applied bias. This is in contrast to the standard result ","authors_text":"Dmitry Mozyrsky, Ivar Martin","cross_cats":["cond-mat.mes-hall","cond-mat.supr-con"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2013-12-09T21:20:47Z","title":"Non-equilibrium theory of tunneling into localized state in superconductor"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.2602","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:e958d869d4c1be97dfdb3eac840682b40dd78958f960f8b4dfddd407cd8e32c4","target":"record","created_at":"2026-05-18T02:41:24Z","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":"874eb1e310ddbd8b87eb54af215874020670cfbcd3233b851ccc608fa30e0ad1","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.supr-con"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2013-12-09T21:20:47Z","title_canon_sha256":"bbd7dcb323e2530651b44e92b5f15977b3c6936ea94cf07a2519b7c0a94f844f"},"schema_version":"1.0","source":{"id":"1312.2602","kind":"arxiv","version":1}},"canonical_sha256":"eb18f2dd92282badf79b2c94f79e68ae22250cb884f09341eb83cdc83ef49278","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"eb18f2dd92282badf79b2c94f79e68ae22250cb884f09341eb83cdc83ef49278","first_computed_at":"2026-05-18T02:41:24.869766Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:41:24.869766Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"NSbBaehx0ujBMXNjZj9CypkSP36YereKONK2n1Tr41eitCgNP76iRglHF9YJqbcLaH8s7nZyNJfuIxPKltTdBA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:41:24.870156Z","signed_message":"canonical_sha256_bytes"},"source_id":"1312.2602","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e958d869d4c1be97dfdb3eac840682b40dd78958f960f8b4dfddd407cd8e32c4","sha256:bc2f8376546b970b9f2106251a96484e1b8532490d43cfdbda056eadfeb4723e"],"state_sha256":"a29b46ffb17174d45f765213d38ba5939f5a50bf3c03bbacf2ed1ef763003f93"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YocWBCq0iMhls5XTzB27sCB6K3ROGoVObHSQxQ6PcxrwoFAouv/Ecc+z37tiURMKVpXFSujDcOTbsUoOIDEmCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-22T11:59:42.723757Z","bundle_sha256":"739808988d9afb6abdf540f577cbff393c20d712c20569f28e5e6605739d4362"}}