{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:V2ZEISTHYIXWZXYOPDLRT4PKVW","short_pith_number":"pith:V2ZEISTH","canonical_record":{"source":{"id":"1106.0980","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-06-06T08:13:11Z","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP"],"title_canon_sha256":"12b28ab054197840db8bd6f14ee53eeb70fd9ab8402486d726290ac5ea5d4cfd","abstract_canon_sha256":"c441cab1fe274c0d70a021390c84845c32471a6ae39bae00f57fedb56abe34d4"},"schema_version":"1.0"},"canonical_sha256":"aeb2444a67c22f6cdf0e78d719f1eaad9876d3bc9e1f68a7eda01738995a0d35","source":{"kind":"arxiv","id":"1106.0980","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1106.0980","created_at":"2026-05-18T04:09:36Z"},{"alias_kind":"arxiv_version","alias_value":"1106.0980v2","created_at":"2026-05-18T04:09:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.0980","created_at":"2026-05-18T04:09:36Z"},{"alias_kind":"pith_short_12","alias_value":"V2ZEISTHYIXW","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_16","alias_value":"V2ZEISTHYIXWZXYO","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_8","alias_value":"V2ZEISTH","created_at":"2026-05-18T12:26:42Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:V2ZEISTHYIXWZXYOPDLRT4PKVW","target":"record","payload":{"canonical_record":{"source":{"id":"1106.0980","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-06-06T08:13:11Z","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP"],"title_canon_sha256":"12b28ab054197840db8bd6f14ee53eeb70fd9ab8402486d726290ac5ea5d4cfd","abstract_canon_sha256":"c441cab1fe274c0d70a021390c84845c32471a6ae39bae00f57fedb56abe34d4"},"schema_version":"1.0"},"canonical_sha256":"aeb2444a67c22f6cdf0e78d719f1eaad9876d3bc9e1f68a7eda01738995a0d35","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:09:36.295757Z","signature_b64":"QV0bvqZehMexez25LaRdNwz8W+yEUwa0Y4+RglP/tkr874XMXAhzEGGTui6gXHaFcsVeZDxFoPYsbabjNAdTBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"aeb2444a67c22f6cdf0e78d719f1eaad9876d3bc9e1f68a7eda01738995a0d35","last_reissued_at":"2026-05-18T04:09:36.295193Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:09:36.295193Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1106.0980","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":"2026-05-18T04:09:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fWlfE3BXWV3Y+DmOBzEzOrPGLYJIMPmKJXiLlL69F5JEmW0oQijLtxD3J36Gh/zEBbVvXk5oAhlBJeV3Fr5JDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T13:47:50.887620Z"},"content_sha256":"138edbb76e4cd3a7979d777ce424a807ee103178979bff4f45bd2dc8db313617","schema_version":"1.0","event_id":"sha256:138edbb76e4cd3a7979d777ce424a807ee103178979bff4f45bd2dc8db313617"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:V2ZEISTHYIXWZXYOPDLRT4PKVW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Phase transitions in the distribution of the Andreev conductance of superconductor-metal junctions with multiple transverse modes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","math-ph","math.MP"],"primary_cat":"cond-mat.mes-hall","authors_text":"Kedar Damle, Pierpaolo Vivo, Satya N. Majumdar, Vikram Tripathi","submitted_at":"2011-06-06T08:13:11Z","abstract_excerpt":"We compute analytically the full distribution of Andreev conductance $G_{\\mathrm{NS}}$ of a metal-superconductor interface with a large number $N_c$ of transverse modes, using a random matrix approach. The probability distribution $\\mathcal{P}(G_{\\mathrm{NS}},N_c)$ in the limit of large $N_c$ displays a Gaussian behavior near the average value $<G_{\\mathrm{NS}}>= (2-\\sqrt{2}) N_c$ and asymmetric power-law tails in the two limits of very small and very large $G_{\\mathrm{NS}}$. In addition, we find a novel third regime sandwiched between the central Gaussian peak and the power law tail for large"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.0980","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":"2026-05-18T04:09:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+fXL7LTzALyyVhuwvlEogKF8GZKwavpn9XvskD1jqhY7fZ7qV5IHhrAX4mHabvxZgbqKSCwh2cgTKMaj1xEdAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T13:47:50.887968Z"},"content_sha256":"a17e0d9e0cf31a04619d40f4c729592f5b5fb6ef8ca145667bafbdd57e33b2b8","schema_version":"1.0","event_id":"sha256:a17e0d9e0cf31a04619d40f4c729592f5b5fb6ef8ca145667bafbdd57e33b2b8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/V2ZEISTHYIXWZXYOPDLRT4PKVW/bundle.json","state_url":"https://pith.science/pith/V2ZEISTHYIXWZXYOPDLRT4PKVW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/V2ZEISTHYIXWZXYOPDLRT4PKVW/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":"2026-06-04T13:47:50Z","links":{"resolver":"https://pith.science/pith/V2ZEISTHYIXWZXYOPDLRT4PKVW","bundle":"https://pith.science/pith/V2ZEISTHYIXWZXYOPDLRT4PKVW/bundle.json","state":"https://pith.science/pith/V2ZEISTHYIXWZXYOPDLRT4PKVW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/V2ZEISTHYIXWZXYOPDLRT4PKVW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:V2ZEISTHYIXWZXYOPDLRT4PKVW","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":"c441cab1fe274c0d70a021390c84845c32471a6ae39bae00f57fedb56abe34d4","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-06-06T08:13:11Z","title_canon_sha256":"12b28ab054197840db8bd6f14ee53eeb70fd9ab8402486d726290ac5ea5d4cfd"},"schema_version":"1.0","source":{"id":"1106.0980","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1106.0980","created_at":"2026-05-18T04:09:36Z"},{"alias_kind":"arxiv_version","alias_value":"1106.0980v2","created_at":"2026-05-18T04:09:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.0980","created_at":"2026-05-18T04:09:36Z"},{"alias_kind":"pith_short_12","alias_value":"V2ZEISTHYIXW","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_16","alias_value":"V2ZEISTHYIXWZXYO","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_8","alias_value":"V2ZEISTH","created_at":"2026-05-18T12:26:42Z"}],"graph_snapshots":[{"event_id":"sha256:a17e0d9e0cf31a04619d40f4c729592f5b5fb6ef8ca145667bafbdd57e33b2b8","target":"graph","created_at":"2026-05-18T04:09:36Z","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 compute analytically the full distribution of Andreev conductance $G_{\\mathrm{NS}}$ of a metal-superconductor interface with a large number $N_c$ of transverse modes, using a random matrix approach. The probability distribution $\\mathcal{P}(G_{\\mathrm{NS}},N_c)$ in the limit of large $N_c$ displays a Gaussian behavior near the average value $<G_{\\mathrm{NS}}>= (2-\\sqrt{2}) N_c$ and asymmetric power-law tails in the two limits of very small and very large $G_{\\mathrm{NS}}$. In addition, we find a novel third regime sandwiched between the central Gaussian peak and the power law tail for large","authors_text":"Kedar Damle, Pierpaolo Vivo, Satya N. Majumdar, Vikram Tripathi","cross_cats":["cond-mat.stat-mech","math-ph","math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-06-06T08:13:11Z","title":"Phase transitions in the distribution of the Andreev conductance of superconductor-metal junctions with multiple transverse modes"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.0980","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":"sha256:138edbb76e4cd3a7979d777ce424a807ee103178979bff4f45bd2dc8db313617","target":"record","created_at":"2026-05-18T04:09:36Z","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":"c441cab1fe274c0d70a021390c84845c32471a6ae39bae00f57fedb56abe34d4","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-06-06T08:13:11Z","title_canon_sha256":"12b28ab054197840db8bd6f14ee53eeb70fd9ab8402486d726290ac5ea5d4cfd"},"schema_version":"1.0","source":{"id":"1106.0980","kind":"arxiv","version":2}},"canonical_sha256":"aeb2444a67c22f6cdf0e78d719f1eaad9876d3bc9e1f68a7eda01738995a0d35","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"aeb2444a67c22f6cdf0e78d719f1eaad9876d3bc9e1f68a7eda01738995a0d35","first_computed_at":"2026-05-18T04:09:36.295193Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:09:36.295193Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"QV0bvqZehMexez25LaRdNwz8W+yEUwa0Y4+RglP/tkr874XMXAhzEGGTui6gXHaFcsVeZDxFoPYsbabjNAdTBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T04:09:36.295757Z","signed_message":"canonical_sha256_bytes"},"source_id":"1106.0980","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:138edbb76e4cd3a7979d777ce424a807ee103178979bff4f45bd2dc8db313617","sha256:a17e0d9e0cf31a04619d40f4c729592f5b5fb6ef8ca145667bafbdd57e33b2b8"],"state_sha256":"1940e9069f2571019c246b603f16c40f464683b6142905bc1b7d3b9ac12b5e8e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ApIPMgIEWsHs5LxdliPCVtsio8TwpuZwzIuuf0RLP4onJ3iBKcll/8I7ZP/FEShlTc3buBRMx8t0izKsNf3vDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-04T13:47:50.890049Z","bundle_sha256":"e9a2b5adf585ba9463bf34a7ea9c514a2d162c43f8485b7d0e7db279460caded"}}