{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:EGPXP5TE5OHBOU53O33NRQQIL2","short_pith_number":"pith:EGPXP5TE","canonical_record":{"source":{"id":"1604.01390","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-04-05T19:59:42Z","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.supr-con"],"title_canon_sha256":"80b465cb160ca20a842a074df4cb730b9eb41089833bdce11c68a245bdad7434","abstract_canon_sha256":"563da91487505e9e462d08602c67b6bc0d668136b7477f9cc1d6634b2177025f"},"schema_version":"1.0"},"canonical_sha256":"219f77f664eb8e1753bb76f6d8c2085eac82716077f37743176a536228972b46","source":{"kind":"arxiv","id":"1604.01390","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.01390","created_at":"2026-05-18T00:43:18Z"},{"alias_kind":"arxiv_version","alias_value":"1604.01390v2","created_at":"2026-05-18T00:43:18Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.01390","created_at":"2026-05-18T00:43:18Z"},{"alias_kind":"pith_short_12","alias_value":"EGPXP5TE5OHB","created_at":"2026-05-18T12:30:12Z"},{"alias_kind":"pith_short_16","alias_value":"EGPXP5TE5OHBOU53","created_at":"2026-05-18T12:30:12Z"},{"alias_kind":"pith_short_8","alias_value":"EGPXP5TE","created_at":"2026-05-18T12:30:12Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:EGPXP5TE5OHBOU53O33NRQQIL2","target":"record","payload":{"canonical_record":{"source":{"id":"1604.01390","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-04-05T19:59:42Z","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.supr-con"],"title_canon_sha256":"80b465cb160ca20a842a074df4cb730b9eb41089833bdce11c68a245bdad7434","abstract_canon_sha256":"563da91487505e9e462d08602c67b6bc0d668136b7477f9cc1d6634b2177025f"},"schema_version":"1.0"},"canonical_sha256":"219f77f664eb8e1753bb76f6d8c2085eac82716077f37743176a536228972b46","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:43:18.607701Z","signature_b64":"6Ic7lWflDikJtTC5LtlVmiwwvnDm5sZ4Ubg03qevtRhJ4Ltqb1sCzCSI582TTx1pV+2crG76OMAJSvDIjvElAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"219f77f664eb8e1753bb76f6d8c2085eac82716077f37743176a536228972b46","last_reissued_at":"2026-05-18T00:43:18.607015Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:43:18.607015Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1604.01390","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":"2026-05-18T00:43:18Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"iXMVx5um60Zeq9P1lSPC3JcF7rEqnUn8BKIu/vSCRt9jQhZHy8G10o3Y1YKh3X0ZjukhqR/2tkCp3QzvSKM+BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T23:06:06.766802Z"},"content_sha256":"7d6f91a3441807b7477c2ecc0d03320a610b800eae149f71878100c2437f168e","schema_version":"1.0","event_id":"sha256:7d6f91a3441807b7477c2ecc0d03320a610b800eae149f71878100c2437f168e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:EGPXP5TE5OHBOU53O33NRQQIL2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Global phase diagram of a three dimensional dirty topological superconductor","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn","cond-mat.supr-con"],"primary_cat":"cond-mat.mes-hall","authors_text":"Bitan Roy, Jay D. Sau, Yahya Alavirad","submitted_at":"2016-04-05T19:59:42Z","abstract_excerpt":"We investigate the phase diagram of a three-dimensional, time-reversal symmetric topological superconductor in the presence of charge impurities and random $s$-wave pairing. Combining complimentary field theoretic and numerical methods, we show that the quantum phase transition between two topologically distinct paired states (or thermal insulators), described by thermal Dirac semimetal, remains unaffected in the presence of sufficiently weak generic randomness. At stronger disorder, however, these two phases are separated by an intervening thermal metallic phase of diffusive Majorana fermions"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.01390","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":"2026-05-18T00:43:18Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dD5RxE4Zk35Jk59Nk6UIK9Talm5WjI/OMix1N60TO8WmYx3UIo2f6FOKMthN6V7HshpAugtxPofz5j1GEQSWDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T23:06:06.767474Z"},"content_sha256":"0bd15a726210502f3fd3dcffae54f066eef7f5ea21ab125ee6bd21e37a4629fd","schema_version":"1.0","event_id":"sha256:0bd15a726210502f3fd3dcffae54f066eef7f5ea21ab125ee6bd21e37a4629fd"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/EGPXP5TE5OHBOU53O33NRQQIL2/bundle.json","state_url":"https://pith.science/pith/EGPXP5TE5OHBOU53O33NRQQIL2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/EGPXP5TE5OHBOU53O33NRQQIL2/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":"2026-05-26T23:06:06Z","links":{"resolver":"https://pith.science/pith/EGPXP5TE5OHBOU53O33NRQQIL2","bundle":"https://pith.science/pith/EGPXP5TE5OHBOU53O33NRQQIL2/bundle.json","state":"https://pith.science/pith/EGPXP5TE5OHBOU53O33NRQQIL2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/EGPXP5TE5OHBOU53O33NRQQIL2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:EGPXP5TE5OHBOU53O33NRQQIL2","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":"563da91487505e9e462d08602c67b6bc0d668136b7477f9cc1d6634b2177025f","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.supr-con"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-04-05T19:59:42Z","title_canon_sha256":"80b465cb160ca20a842a074df4cb730b9eb41089833bdce11c68a245bdad7434"},"schema_version":"1.0","source":{"id":"1604.01390","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.01390","created_at":"2026-05-18T00:43:18Z"},{"alias_kind":"arxiv_version","alias_value":"1604.01390v2","created_at":"2026-05-18T00:43:18Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.01390","created_at":"2026-05-18T00:43:18Z"},{"alias_kind":"pith_short_12","alias_value":"EGPXP5TE5OHB","created_at":"2026-05-18T12:30:12Z"},{"alias_kind":"pith_short_16","alias_value":"EGPXP5TE5OHBOU53","created_at":"2026-05-18T12:30:12Z"},{"alias_kind":"pith_short_8","alias_value":"EGPXP5TE","created_at":"2026-05-18T12:30:12Z"}],"graph_snapshots":[{"event_id":"sha256:0bd15a726210502f3fd3dcffae54f066eef7f5ea21ab125ee6bd21e37a4629fd","target":"graph","created_at":"2026-05-18T00:43:18Z","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 investigate the phase diagram of a three-dimensional, time-reversal symmetric topological superconductor in the presence of charge impurities and random $s$-wave pairing. Combining complimentary field theoretic and numerical methods, we show that the quantum phase transition between two topologically distinct paired states (or thermal insulators), described by thermal Dirac semimetal, remains unaffected in the presence of sufficiently weak generic randomness. At stronger disorder, however, these two phases are separated by an intervening thermal metallic phase of diffusive Majorana fermions","authors_text":"Bitan Roy, Jay D. Sau, Yahya Alavirad","cross_cats":["cond-mat.dis-nn","cond-mat.supr-con"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-04-05T19:59:42Z","title":"Global phase diagram of a three dimensional dirty topological superconductor"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.01390","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":"sha256:7d6f91a3441807b7477c2ecc0d03320a610b800eae149f71878100c2437f168e","target":"record","created_at":"2026-05-18T00:43:18Z","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":"563da91487505e9e462d08602c67b6bc0d668136b7477f9cc1d6634b2177025f","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.supr-con"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-04-05T19:59:42Z","title_canon_sha256":"80b465cb160ca20a842a074df4cb730b9eb41089833bdce11c68a245bdad7434"},"schema_version":"1.0","source":{"id":"1604.01390","kind":"arxiv","version":2}},"canonical_sha256":"219f77f664eb8e1753bb76f6d8c2085eac82716077f37743176a536228972b46","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"219f77f664eb8e1753bb76f6d8c2085eac82716077f37743176a536228972b46","first_computed_at":"2026-05-18T00:43:18.607015Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:43:18.607015Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"6Ic7lWflDikJtTC5LtlVmiwwvnDm5sZ4Ubg03qevtRhJ4Ltqb1sCzCSI582TTx1pV+2crG76OMAJSvDIjvElAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:43:18.607701Z","signed_message":"canonical_sha256_bytes"},"source_id":"1604.01390","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7d6f91a3441807b7477c2ecc0d03320a610b800eae149f71878100c2437f168e","sha256:0bd15a726210502f3fd3dcffae54f066eef7f5ea21ab125ee6bd21e37a4629fd"],"state_sha256":"d32d26ef3bec0ea111d22d90690a71257b679bc1dccbbf5036655fd76d3559aa"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XF0duk+6a6J1IFkiKO6cTCOTOTQMZtuNwVJfdoFOS057t2LRQSP7hI43HM/tm9mbmXkVWaCCoV/nYLYtNFpJAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T23:06:06.770985Z","bundle_sha256":"185cc32182aa05334a4970b9dcb67b97e3053b7991e17080c359e95c9bb2c628"}}