{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:UEN3AEUP2MUVVK7C2VEADUEQ75","short_pith_number":"pith:UEN3AEUP","canonical_record":{"source":{"id":"1101.5239","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-01-27T09:57:10Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"322cccd77f6cacfcb90c5086065b3a1cfd0afd9dfeeb02ed31a7358be22e95da","abstract_canon_sha256":"667dbfe16be1f92252986eaf40c34d797d9142d42d6ab951de82bf994bc41466"},"schema_version":"1.0"},"canonical_sha256":"a11bb0128fd3295aabe2d54801d090ff41faf1b0ea689f919063ca6c87cb9aea","source":{"kind":"arxiv","id":"1101.5239","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1101.5239","created_at":"2026-05-18T02:22:49Z"},{"alias_kind":"arxiv_version","alias_value":"1101.5239v1","created_at":"2026-05-18T02:22:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1101.5239","created_at":"2026-05-18T02:22:49Z"},{"alias_kind":"pith_short_12","alias_value":"UEN3AEUP2MUV","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_16","alias_value":"UEN3AEUP2MUVVK7C","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_8","alias_value":"UEN3AEUP","created_at":"2026-05-18T12:26:42Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:UEN3AEUP2MUVVK7C2VEADUEQ75","target":"record","payload":{"canonical_record":{"source":{"id":"1101.5239","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-01-27T09:57:10Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"322cccd77f6cacfcb90c5086065b3a1cfd0afd9dfeeb02ed31a7358be22e95da","abstract_canon_sha256":"667dbfe16be1f92252986eaf40c34d797d9142d42d6ab951de82bf994bc41466"},"schema_version":"1.0"},"canonical_sha256":"a11bb0128fd3295aabe2d54801d090ff41faf1b0ea689f919063ca6c87cb9aea","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:22:49.200249Z","signature_b64":"uQQ+D4uVuQ0J4qAg9ICcLGfIHIaQy9w7vaGRwaPo0y05Dh1txDAkBgESdDf3bGISQWS1KccCakjClkNXuF9NAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a11bb0128fd3295aabe2d54801d090ff41faf1b0ea689f919063ca6c87cb9aea","last_reissued_at":"2026-05-18T02:22:49.199579Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:22:49.199579Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1101.5239","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":"2026-05-18T02:22:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"m//jjN2ditoMjjNJK6wnEnWQ8kWiU1mVXS/IOoHYjcJ1qCNA4lbzt2dnrQEoP9DVhF6qkl+stXQXZVkuufJQAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T04:29:37.972442Z"},"content_sha256":"abf973c04af809f61c4d99301da96100d8f2c38622c453bf3816dbc3e85f956b","schema_version":"1.0","event_id":"sha256:abf973c04af809f61c4d99301da96100d8f2c38622c453bf3816dbc3e85f956b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:UEN3AEUP2MUVVK7C2VEADUEQ75","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Interplay of Kondo and superconducting correlations in the nonequilibrium Andreev transport through a quantum dot","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mes-hall","authors_text":"Norio Kawakami, Yasuhiro Yamada, Yoichi Tanaka","submitted_at":"2011-01-27T09:57:10Z","abstract_excerpt":"Using the modified perturbation theory, we theoretically study the nonequilibrium Andreev transport through a quantum dot coupled to normal and superconducting leads (N-QD-S), which is strongly influenced by the Kondo and superconducting correlations. From the numerical calculation, we find that the renormalized couplings between the leads and the dot in the equilibrium states characterize the peak formation in the nonequilibrium differential conductance. In particular, in the Kondo regime, the enhancement of the Andreev transport via a Kondo resonance occurs in the differential conductance at"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1101.5239","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":"2026-05-18T02:22:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yc1B7LAGHCgG2rCti0/61MzTi4dUqR25KgY5Zb1MOEWglAz70xo8ZaJkTB5emfQ5VTd3lMOxJcgXb0wayM/8AQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T04:29:37.972795Z"},"content_sha256":"e55ffdc2d19dbd059c7488b436e59062f5adddda8ce3c69fc12cdc561e5df867","schema_version":"1.0","event_id":"sha256:e55ffdc2d19dbd059c7488b436e59062f5adddda8ce3c69fc12cdc561e5df867"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UEN3AEUP2MUVVK7C2VEADUEQ75/bundle.json","state_url":"https://pith.science/pith/UEN3AEUP2MUVVK7C2VEADUEQ75/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UEN3AEUP2MUVVK7C2VEADUEQ75/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":"2026-05-28T04:29:37Z","links":{"resolver":"https://pith.science/pith/UEN3AEUP2MUVVK7C2VEADUEQ75","bundle":"https://pith.science/pith/UEN3AEUP2MUVVK7C2VEADUEQ75/bundle.json","state":"https://pith.science/pith/UEN3AEUP2MUVVK7C2VEADUEQ75/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UEN3AEUP2MUVVK7C2VEADUEQ75/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:UEN3AEUP2MUVVK7C2VEADUEQ75","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":"667dbfe16be1f92252986eaf40c34d797d9142d42d6ab951de82bf994bc41466","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-01-27T09:57:10Z","title_canon_sha256":"322cccd77f6cacfcb90c5086065b3a1cfd0afd9dfeeb02ed31a7358be22e95da"},"schema_version":"1.0","source":{"id":"1101.5239","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1101.5239","created_at":"2026-05-18T02:22:49Z"},{"alias_kind":"arxiv_version","alias_value":"1101.5239v1","created_at":"2026-05-18T02:22:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1101.5239","created_at":"2026-05-18T02:22:49Z"},{"alias_kind":"pith_short_12","alias_value":"UEN3AEUP2MUV","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_16","alias_value":"UEN3AEUP2MUVVK7C","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_8","alias_value":"UEN3AEUP","created_at":"2026-05-18T12:26:42Z"}],"graph_snapshots":[{"event_id":"sha256:e55ffdc2d19dbd059c7488b436e59062f5adddda8ce3c69fc12cdc561e5df867","target":"graph","created_at":"2026-05-18T02:22:49Z","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":"Using the modified perturbation theory, we theoretically study the nonequilibrium Andreev transport through a quantum dot coupled to normal and superconducting leads (N-QD-S), which is strongly influenced by the Kondo and superconducting correlations. From the numerical calculation, we find that the renormalized couplings between the leads and the dot in the equilibrium states characterize the peak formation in the nonequilibrium differential conductance. In particular, in the Kondo regime, the enhancement of the Andreev transport via a Kondo resonance occurs in the differential conductance at","authors_text":"Norio Kawakami, Yasuhiro Yamada, Yoichi Tanaka","cross_cats":["cond-mat.str-el"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-01-27T09:57:10Z","title":"Interplay of Kondo and superconducting correlations in the nonequilibrium Andreev transport through a quantum dot"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1101.5239","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:abf973c04af809f61c4d99301da96100d8f2c38622c453bf3816dbc3e85f956b","target":"record","created_at":"2026-05-18T02:22:49Z","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":"667dbfe16be1f92252986eaf40c34d797d9142d42d6ab951de82bf994bc41466","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-01-27T09:57:10Z","title_canon_sha256":"322cccd77f6cacfcb90c5086065b3a1cfd0afd9dfeeb02ed31a7358be22e95da"},"schema_version":"1.0","source":{"id":"1101.5239","kind":"arxiv","version":1}},"canonical_sha256":"a11bb0128fd3295aabe2d54801d090ff41faf1b0ea689f919063ca6c87cb9aea","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a11bb0128fd3295aabe2d54801d090ff41faf1b0ea689f919063ca6c87cb9aea","first_computed_at":"2026-05-18T02:22:49.199579Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:22:49.199579Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"uQQ+D4uVuQ0J4qAg9ICcLGfIHIaQy9w7vaGRwaPo0y05Dh1txDAkBgESdDf3bGISQWS1KccCakjClkNXuF9NAA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:22:49.200249Z","signed_message":"canonical_sha256_bytes"},"source_id":"1101.5239","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:abf973c04af809f61c4d99301da96100d8f2c38622c453bf3816dbc3e85f956b","sha256:e55ffdc2d19dbd059c7488b436e59062f5adddda8ce3c69fc12cdc561e5df867"],"state_sha256":"da46983259dcfa93172fd549ec554f80f15056400ad8f72dff65ca71297129a3"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GW30bTiJNFNr/ewHoL7r1VkQOfRC1TbokreVsEHVL4MiDhaLBUsKQjqfS78yVjMqpH2xNh/wbOb3VbHtUQ3kBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T04:29:37.974764Z","bundle_sha256":"6f702ce3020a4a40c20ce56fcb7efda1349bfa9bfac878faa58802a3b2aaa2da"}}