{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:6URJQRFBEVS3IJMQC7BDXAKKWN","short_pith_number":"pith:6URJQRFB","canonical_record":{"source":{"id":"1007.3605","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2010-07-21T10:29:19Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"fbe9726854957e6e7ba30e590088628187b19155fa09584055fd3adcfd01b8c7","abstract_canon_sha256":"fac8f20c4bf9a9b362a79f3f9c11d6e9e5a8cc8d70500278ca85230982dfb93e"},"schema_version":"1.0"},"canonical_sha256":"f5229844a12565b4259017c23b814ab37445b040c7e889abbfc46309f52e1ad1","source":{"kind":"arxiv","id":"1007.3605","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1007.3605","created_at":"2026-05-18T04:39:07Z"},{"alias_kind":"arxiv_version","alias_value":"1007.3605v2","created_at":"2026-05-18T04:39:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1007.3605","created_at":"2026-05-18T04:39:07Z"},{"alias_kind":"pith_short_12","alias_value":"6URJQRFBEVS3","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_16","alias_value":"6URJQRFBEVS3IJMQ","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_8","alias_value":"6URJQRFB","created_at":"2026-05-18T12:26:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:6URJQRFBEVS3IJMQC7BDXAKKWN","target":"record","payload":{"canonical_record":{"source":{"id":"1007.3605","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2010-07-21T10:29:19Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"fbe9726854957e6e7ba30e590088628187b19155fa09584055fd3adcfd01b8c7","abstract_canon_sha256":"fac8f20c4bf9a9b362a79f3f9c11d6e9e5a8cc8d70500278ca85230982dfb93e"},"schema_version":"1.0"},"canonical_sha256":"f5229844a12565b4259017c23b814ab37445b040c7e889abbfc46309f52e1ad1","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:39:07.917352Z","signature_b64":"uWWhvCUm6ZeX4oKeB0Pz9F/JoBVAe3vI3qi8libaYGcma3S/WApow56ep1GiXn1IYDux1Qel6wwXAux94b1vAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f5229844a12565b4259017c23b814ab37445b040c7e889abbfc46309f52e1ad1","last_reissued_at":"2026-05-18T04:39:07.916885Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:39:07.916885Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1007.3605","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":"2026-05-18T04:39:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1PcWRixlmlPrTMD8FWmoEyzGefrnI95zwLMl/+G6n+akP7Wczv/P3SMKxUsWKh04gNg80lBpYge0GEXHhUtsDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T00:34:25.716956Z"},"content_sha256":"a14062a4b0a37a2ecb12d86cedd95f6a44d100776e868d1161724be881f41726","schema_version":"1.0","event_id":"sha256:a14062a4b0a37a2ecb12d86cedd95f6a44d100776e868d1161724be881f41726"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:6URJQRFBEVS3IJMQC7BDXAKKWN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Spin and orbital fluctuations in non-equilibrium transport through quantum dots: A renormalisation-group analysis","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mes-hall","authors_text":"D. Schuricht, S. Andergassen, S. Y. Mueller, V. Koerting","submitted_at":"2010-07-21T10:29:19Z","abstract_excerpt":"We study non-equilibrium current and occupation probabilities of a two-orbital quantum dot. The couplings to the leads are allowed to be asymmetric and orbital dependent as it is generically the case in transport experiments on molecules and nanowires. Starting from a two-orbital Anderson model, we perform a generalised Schrieffer-Wolff transformation to derive an effective Kondo model. This generates an orbital potential scattering contribution which is of the same order as the spin exchange interaction. In a first perturbative analysis we identify a regime of negative differential conductanc"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1007.3605","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":"2026-05-18T04:39:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sKAOKyq9IPd2PfqWPLPBKJh3mUV71+VBOxsLdI4JxNg8bqPMK2cDArrRquqLJmpd1/P/TqKxQMoLeZ1wSGNpDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T00:34:25.717583Z"},"content_sha256":"091b0d1478b06aee75ca8e5c93e63350ffd5fab83c3bd23d0563a29d75a6b06c","schema_version":"1.0","event_id":"sha256:091b0d1478b06aee75ca8e5c93e63350ffd5fab83c3bd23d0563a29d75a6b06c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6URJQRFBEVS3IJMQC7BDXAKKWN/bundle.json","state_url":"https://pith.science/pith/6URJQRFBEVS3IJMQC7BDXAKKWN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6URJQRFBEVS3IJMQC7BDXAKKWN/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":"2026-05-27T00:34:25Z","links":{"resolver":"https://pith.science/pith/6URJQRFBEVS3IJMQC7BDXAKKWN","bundle":"https://pith.science/pith/6URJQRFBEVS3IJMQC7BDXAKKWN/bundle.json","state":"https://pith.science/pith/6URJQRFBEVS3IJMQC7BDXAKKWN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6URJQRFBEVS3IJMQC7BDXAKKWN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:6URJQRFBEVS3IJMQC7BDXAKKWN","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":"fac8f20c4bf9a9b362a79f3f9c11d6e9e5a8cc8d70500278ca85230982dfb93e","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2010-07-21T10:29:19Z","title_canon_sha256":"fbe9726854957e6e7ba30e590088628187b19155fa09584055fd3adcfd01b8c7"},"schema_version":"1.0","source":{"id":"1007.3605","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1007.3605","created_at":"2026-05-18T04:39:07Z"},{"alias_kind":"arxiv_version","alias_value":"1007.3605v2","created_at":"2026-05-18T04:39:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1007.3605","created_at":"2026-05-18T04:39:07Z"},{"alias_kind":"pith_short_12","alias_value":"6URJQRFBEVS3","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_16","alias_value":"6URJQRFBEVS3IJMQ","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_8","alias_value":"6URJQRFB","created_at":"2026-05-18T12:26:04Z"}],"graph_snapshots":[{"event_id":"sha256:091b0d1478b06aee75ca8e5c93e63350ffd5fab83c3bd23d0563a29d75a6b06c","target":"graph","created_at":"2026-05-18T04:39:07Z","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 non-equilibrium current and occupation probabilities of a two-orbital quantum dot. The couplings to the leads are allowed to be asymmetric and orbital dependent as it is generically the case in transport experiments on molecules and nanowires. Starting from a two-orbital Anderson model, we perform a generalised Schrieffer-Wolff transformation to derive an effective Kondo model. This generates an orbital potential scattering contribution which is of the same order as the spin exchange interaction. In a first perturbative analysis we identify a regime of negative differential conductanc","authors_text":"D. Schuricht, S. Andergassen, S. Y. Mueller, V. Koerting","cross_cats":["cond-mat.str-el"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2010-07-21T10:29:19Z","title":"Spin and orbital fluctuations in non-equilibrium transport through quantum dots: A renormalisation-group analysis"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1007.3605","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:a14062a4b0a37a2ecb12d86cedd95f6a44d100776e868d1161724be881f41726","target":"record","created_at":"2026-05-18T04:39:07Z","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":"fac8f20c4bf9a9b362a79f3f9c11d6e9e5a8cc8d70500278ca85230982dfb93e","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2010-07-21T10:29:19Z","title_canon_sha256":"fbe9726854957e6e7ba30e590088628187b19155fa09584055fd3adcfd01b8c7"},"schema_version":"1.0","source":{"id":"1007.3605","kind":"arxiv","version":2}},"canonical_sha256":"f5229844a12565b4259017c23b814ab37445b040c7e889abbfc46309f52e1ad1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f5229844a12565b4259017c23b814ab37445b040c7e889abbfc46309f52e1ad1","first_computed_at":"2026-05-18T04:39:07.916885Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:39:07.916885Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"uWWhvCUm6ZeX4oKeB0Pz9F/JoBVAe3vI3qi8libaYGcma3S/WApow56ep1GiXn1IYDux1Qel6wwXAux94b1vAA==","signature_status":"signed_v1","signed_at":"2026-05-18T04:39:07.917352Z","signed_message":"canonical_sha256_bytes"},"source_id":"1007.3605","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a14062a4b0a37a2ecb12d86cedd95f6a44d100776e868d1161724be881f41726","sha256:091b0d1478b06aee75ca8e5c93e63350ffd5fab83c3bd23d0563a29d75a6b06c"],"state_sha256":"2aef98103e7c356228045d8ec79ca80718aeb4bcf405df659613adfeca0f4a81"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sg8VDfGFxG8j0f20n5VugYXt+C2Io4sW8JQaO8Usq5IJGkBAUX9XWfDoMjZuTfHT4YG4eFnsx96+Se5NOMdQCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T00:34:25.720812Z","bundle_sha256":"379d38b3d2b72cd0d9b18f57b1490b6ef32494e6db0d6e439b72856a12fded49"}}