{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:44WUQSM2INSC4ODPOKHCDXJBIO","short_pith_number":"pith:44WUQSM2","canonical_record":{"source":{"id":"1708.05750","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-08-18T20:04:20Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"089486c859f69f130e9a61d9356a8c4162793990cf81fede739a8f596678053d","abstract_canon_sha256":"c06a1953a9038c6b0c61ae74ca7ed84a477ff5ccaa2b46db5ec791e099afc647"},"schema_version":"1.0"},"canonical_sha256":"e72d48499a43642e386f728e21dd2143b93b6ad40d989d7f5d35b8cb909cf438","source":{"kind":"arxiv","id":"1708.05750","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.05750","created_at":"2026-05-18T00:22:16Z"},{"alias_kind":"arxiv_version","alias_value":"1708.05750v3","created_at":"2026-05-18T00:22:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.05750","created_at":"2026-05-18T00:22:16Z"},{"alias_kind":"pith_short_12","alias_value":"44WUQSM2INSC","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_16","alias_value":"44WUQSM2INSC4ODP","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_8","alias_value":"44WUQSM2","created_at":"2026-05-18T12:30:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:44WUQSM2INSC4ODPOKHCDXJBIO","target":"record","payload":{"canonical_record":{"source":{"id":"1708.05750","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-08-18T20:04:20Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"089486c859f69f130e9a61d9356a8c4162793990cf81fede739a8f596678053d","abstract_canon_sha256":"c06a1953a9038c6b0c61ae74ca7ed84a477ff5ccaa2b46db5ec791e099afc647"},"schema_version":"1.0"},"canonical_sha256":"e72d48499a43642e386f728e21dd2143b93b6ad40d989d7f5d35b8cb909cf438","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:22:16.027324Z","signature_b64":"McCxv4jSNPUAuzK+sJtEEBpTAE0/DU3rgTKUDERYziRSt90Wk5ZBDDzhnDTi4XYq3kcX2S5eq/tGyg4eoICmCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e72d48499a43642e386f728e21dd2143b93b6ad40d989d7f5d35b8cb909cf438","last_reissued_at":"2026-05-18T00:22:16.026788Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:22:16.026788Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1708.05750","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:22:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gHqCXX4yVRZMmh13vWpsMcrZVnA9zBwyFyDRv2lwfXz+Nv0qgQkg9/x65Oo72zfqAzLS5u5H+RrL6f0vMyf8Aw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-22T13:51:13.078831Z"},"content_sha256":"6310764b2547d46cdbffc0f6aad12839686dcbe5d46db70dc80b50dee6681c87","schema_version":"1.0","event_id":"sha256:6310764b2547d46cdbffc0f6aad12839686dcbe5d46db70dc80b50dee6681c87"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:44WUQSM2INSC4ODPOKHCDXJBIO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Nonequilibrium Kondo effect in a magnetic field: Auxiliary master equation approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"Antonius Dorda, Delia M. Fugger, Enrico Arrigoni, Frauke Schwarz, Jan von Delft","submitted_at":"2017-08-18T20:04:20Z","abstract_excerpt":"We study the single-impurity Anderson model out of equilibrium under the influence of a bias voltage $\\phi$ and a magnetic field $B$. We investigate the interplay between the shift ($\\omega_B$) of the Kondo peak in the spin-resolved density of states (DOS) and the one ($\\phi_B$) of the conductance anomaly. In agreement with experiments and previous theoretical calculations we find that, while the latter displays a rather linear behavior with an almost constant slope as a function of $B$ down to the Kondo scale, the DOS shift first features a slower increase reaching the same behavior as $\\phi_"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.05750","kind":"arxiv","version":3},"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":"2026-05-18T00:22:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hFueDZwuccYirsDqDsUteY3xIx0+nHqj2uURUO8GoN1u4smEe0hyXlxBd5XSzUI8aNVzUactoL3ACLafue/NBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-22T13:51:13.079258Z"},"content_sha256":"ae28dd600dc750ed5c9fa5e58f4e5af80c2648e5be607bfa63fcf95270cd55dc","schema_version":"1.0","event_id":"sha256:ae28dd600dc750ed5c9fa5e58f4e5af80c2648e5be607bfa63fcf95270cd55dc"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/44WUQSM2INSC4ODPOKHCDXJBIO/bundle.json","state_url":"https://pith.science/pith/44WUQSM2INSC4ODPOKHCDXJBIO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/44WUQSM2INSC4ODPOKHCDXJBIO/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":"2026-06-22T13:51:13Z","links":{"resolver":"https://pith.science/pith/44WUQSM2INSC4ODPOKHCDXJBIO","bundle":"https://pith.science/pith/44WUQSM2INSC4ODPOKHCDXJBIO/bundle.json","state":"https://pith.science/pith/44WUQSM2INSC4ODPOKHCDXJBIO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/44WUQSM2INSC4ODPOKHCDXJBIO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:44WUQSM2INSC4ODPOKHCDXJBIO","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":"c06a1953a9038c6b0c61ae74ca7ed84a477ff5ccaa2b46db5ec791e099afc647","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-08-18T20:04:20Z","title_canon_sha256":"089486c859f69f130e9a61d9356a8c4162793990cf81fede739a8f596678053d"},"schema_version":"1.0","source":{"id":"1708.05750","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.05750","created_at":"2026-05-18T00:22:16Z"},{"alias_kind":"arxiv_version","alias_value":"1708.05750v3","created_at":"2026-05-18T00:22:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.05750","created_at":"2026-05-18T00:22:16Z"},{"alias_kind":"pith_short_12","alias_value":"44WUQSM2INSC","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_16","alias_value":"44WUQSM2INSC4ODP","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_8","alias_value":"44WUQSM2","created_at":"2026-05-18T12:30:58Z"}],"graph_snapshots":[{"event_id":"sha256:ae28dd600dc750ed5c9fa5e58f4e5af80c2648e5be607bfa63fcf95270cd55dc","target":"graph","created_at":"2026-05-18T00:22:16Z","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 study the single-impurity Anderson model out of equilibrium under the influence of a bias voltage $\\phi$ and a magnetic field $B$. We investigate the interplay between the shift ($\\omega_B$) of the Kondo peak in the spin-resolved density of states (DOS) and the one ($\\phi_B$) of the conductance anomaly. In agreement with experiments and previous theoretical calculations we find that, while the latter displays a rather linear behavior with an almost constant slope as a function of $B$ down to the Kondo scale, the DOS shift first features a slower increase reaching the same behavior as $\\phi_","authors_text":"Antonius Dorda, Delia M. Fugger, Enrico Arrigoni, Frauke Schwarz, Jan von Delft","cross_cats":["cond-mat.mes-hall"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-08-18T20:04:20Z","title":"Nonequilibrium Kondo effect in a magnetic field: Auxiliary master equation approach"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.05750","kind":"arxiv","version":3},"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":"sha256:6310764b2547d46cdbffc0f6aad12839686dcbe5d46db70dc80b50dee6681c87","target":"record","created_at":"2026-05-18T00:22:16Z","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":"c06a1953a9038c6b0c61ae74ca7ed84a477ff5ccaa2b46db5ec791e099afc647","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-08-18T20:04:20Z","title_canon_sha256":"089486c859f69f130e9a61d9356a8c4162793990cf81fede739a8f596678053d"},"schema_version":"1.0","source":{"id":"1708.05750","kind":"arxiv","version":3}},"canonical_sha256":"e72d48499a43642e386f728e21dd2143b93b6ad40d989d7f5d35b8cb909cf438","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e72d48499a43642e386f728e21dd2143b93b6ad40d989d7f5d35b8cb909cf438","first_computed_at":"2026-05-18T00:22:16.026788Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:22:16.026788Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"McCxv4jSNPUAuzK+sJtEEBpTAE0/DU3rgTKUDERYziRSt90Wk5ZBDDzhnDTi4XYq3kcX2S5eq/tGyg4eoICmCA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:22:16.027324Z","signed_message":"canonical_sha256_bytes"},"source_id":"1708.05750","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6310764b2547d46cdbffc0f6aad12839686dcbe5d46db70dc80b50dee6681c87","sha256:ae28dd600dc750ed5c9fa5e58f4e5af80c2648e5be607bfa63fcf95270cd55dc"],"state_sha256":"123b940870261c20b10476ab2285ffa7f221c3dd6427ef63b90ac87f4be98bdf"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/1+XNl0U3vrk5j256qdZ9yEuPFEQUf3tzEPeehPng1urhoYErO+4Z6qodIJ0xi9mUFzLF/DGjvuOxppzqv3jCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-22T13:51:13.081243Z","bundle_sha256":"0ff7973e7ead21ddbaa0e09b7383dd13f8c2fe5c353305ef645f1105171c53a9"}}