{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:GJIJBGV7VEMRXNA463XP2T74EU","short_pith_number":"pith:GJIJBGV7","canonical_record":{"source":{"id":"1802.01154","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-02-04T16:28:52Z","cross_cats_sorted":["cond-mat.str-el","hep-th"],"title_canon_sha256":"dd4856969753e61be1ad37707b4f41aca7d2cb17bc3dd1322bc7f836dca75b63","abstract_canon_sha256":"167a22c1bc3c75fba2db85a6c1e586f8757dba12b2f85e3015132810b61fd4e4"},"schema_version":"1.0"},"canonical_sha256":"3250909abfa9191bb41cf6eefd4ffc2500c755734c550337c83b4dd33078f4e9","source":{"kind":"arxiv","id":"1802.01154","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1802.01154","created_at":"2026-05-18T00:00:57Z"},{"alias_kind":"arxiv_version","alias_value":"1802.01154v2","created_at":"2026-05-18T00:00:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1802.01154","created_at":"2026-05-18T00:00:57Z"},{"alias_kind":"pith_short_12","alias_value":"GJIJBGV7VEMR","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_16","alias_value":"GJIJBGV7VEMRXNA4","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_8","alias_value":"GJIJBGV7","created_at":"2026-05-18T12:32:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:GJIJBGV7VEMRXNA463XP2T74EU","target":"record","payload":{"canonical_record":{"source":{"id":"1802.01154","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-02-04T16:28:52Z","cross_cats_sorted":["cond-mat.str-el","hep-th"],"title_canon_sha256":"dd4856969753e61be1ad37707b4f41aca7d2cb17bc3dd1322bc7f836dca75b63","abstract_canon_sha256":"167a22c1bc3c75fba2db85a6c1e586f8757dba12b2f85e3015132810b61fd4e4"},"schema_version":"1.0"},"canonical_sha256":"3250909abfa9191bb41cf6eefd4ffc2500c755734c550337c83b4dd33078f4e9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:00:57.548678Z","signature_b64":"m2dGmwZz9sJ4LXowNc8xTv7XrBt/XRcNTGplkjytRXnO8EmBUx0+6huNBfHYKEjGTwsgsQKnFeRauyykJNzAAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3250909abfa9191bb41cf6eefd4ffc2500c755734c550337c83b4dd33078f4e9","last_reissued_at":"2026-05-18T00:00:57.548119Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:00:57.548119Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1802.01154","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":"2026-05-18T00:00:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9xmtyb3nkppCaTGS3FEUdB1b8BJ/CCa1J9C2UkLltymFyK0FNFNDhNRR/saVdbuTtv1r/DJmpGsBm3neKx2lCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T16:17:03.324928Z"},"content_sha256":"08e1ce36c7205e83f77398a30924fd761abf11d354dadad57a7ab502a06b947d","schema_version":"1.0","event_id":"sha256:08e1ce36c7205e83f77398a30924fd761abf11d354dadad57a7ab502a06b947d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:GJIJBGV7VEMRXNA463XP2T74EU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Full counting statistics in the free Dirac theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","hep-th"],"primary_cat":"cond-mat.stat-mech","authors_text":"Takato Yoshimura","submitted_at":"2018-02-04T16:28:52Z","abstract_excerpt":"We study charge transport and fluctuations of the (3+1)-dimensional massive free Dirac theory. In particular, we focus on the steady state that emerges following a local quench whereby two independently thermalized halves of the system are connected and let to evolve unitarily for a long time. Based on the two-time von Neumann measurement statistics and exact computations, the scaled cumulant generating function associated with the charge transport is derived. We find that it can be written as a generalization of Levitov-Lesovik formula to the case in three spatial dimensions. In the massless "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1802.01154","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":"2026-05-18T00:00:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NCNaQ2pMerZX/fksjzo1hDDOlfYu32yBx7iSX7Jifq+q/G9G/Rs2e7B0TikVyYMzT5wUo0UmhD6OBqXXgmBUDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T16:17:03.325375Z"},"content_sha256":"604650fad6ff58e1d72a4c72edc1742dcf64ee4fb3b51e6edc4371dd5656a0e1","schema_version":"1.0","event_id":"sha256:604650fad6ff58e1d72a4c72edc1742dcf64ee4fb3b51e6edc4371dd5656a0e1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GJIJBGV7VEMRXNA463XP2T74EU/bundle.json","state_url":"https://pith.science/pith/GJIJBGV7VEMRXNA463XP2T74EU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GJIJBGV7VEMRXNA463XP2T74EU/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":"2026-08-04T16:17:03Z","links":{"resolver":"https://pith.science/pith/GJIJBGV7VEMRXNA463XP2T74EU","bundle":"https://pith.science/pith/GJIJBGV7VEMRXNA463XP2T74EU/bundle.json","state":"https://pith.science/pith/GJIJBGV7VEMRXNA463XP2T74EU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GJIJBGV7VEMRXNA463XP2T74EU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:GJIJBGV7VEMRXNA463XP2T74EU","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":"167a22c1bc3c75fba2db85a6c1e586f8757dba12b2f85e3015132810b61fd4e4","cross_cats_sorted":["cond-mat.str-el","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-02-04T16:28:52Z","title_canon_sha256":"dd4856969753e61be1ad37707b4f41aca7d2cb17bc3dd1322bc7f836dca75b63"},"schema_version":"1.0","source":{"id":"1802.01154","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1802.01154","created_at":"2026-05-18T00:00:57Z"},{"alias_kind":"arxiv_version","alias_value":"1802.01154v2","created_at":"2026-05-18T00:00:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1802.01154","created_at":"2026-05-18T00:00:57Z"},{"alias_kind":"pith_short_12","alias_value":"GJIJBGV7VEMR","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_16","alias_value":"GJIJBGV7VEMRXNA4","created_at":"2026-05-18T12:32:25Z"},{"alias_kind":"pith_short_8","alias_value":"GJIJBGV7","created_at":"2026-05-18T12:32:25Z"}],"graph_snapshots":[{"event_id":"sha256:604650fad6ff58e1d72a4c72edc1742dcf64ee4fb3b51e6edc4371dd5656a0e1","target":"graph","created_at":"2026-05-18T00:00:57Z","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 charge transport and fluctuations of the (3+1)-dimensional massive free Dirac theory. In particular, we focus on the steady state that emerges following a local quench whereby two independently thermalized halves of the system are connected and let to evolve unitarily for a long time. Based on the two-time von Neumann measurement statistics and exact computations, the scaled cumulant generating function associated with the charge transport is derived. We find that it can be written as a generalization of Levitov-Lesovik formula to the case in three spatial dimensions. In the massless ","authors_text":"Takato Yoshimura","cross_cats":["cond-mat.str-el","hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-02-04T16:28:52Z","title":"Full counting statistics in the free Dirac theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1802.01154","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":"sha256:08e1ce36c7205e83f77398a30924fd761abf11d354dadad57a7ab502a06b947d","target":"record","created_at":"2026-05-18T00:00:57Z","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":"167a22c1bc3c75fba2db85a6c1e586f8757dba12b2f85e3015132810b61fd4e4","cross_cats_sorted":["cond-mat.str-el","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-02-04T16:28:52Z","title_canon_sha256":"dd4856969753e61be1ad37707b4f41aca7d2cb17bc3dd1322bc7f836dca75b63"},"schema_version":"1.0","source":{"id":"1802.01154","kind":"arxiv","version":2}},"canonical_sha256":"3250909abfa9191bb41cf6eefd4ffc2500c755734c550337c83b4dd33078f4e9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3250909abfa9191bb41cf6eefd4ffc2500c755734c550337c83b4dd33078f4e9","first_computed_at":"2026-05-18T00:00:57.548119Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:00:57.548119Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"m2dGmwZz9sJ4LXowNc8xTv7XrBt/XRcNTGplkjytRXnO8EmBUx0+6huNBfHYKEjGTwsgsQKnFeRauyykJNzAAA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:00:57.548678Z","signed_message":"canonical_sha256_bytes"},"source_id":"1802.01154","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:08e1ce36c7205e83f77398a30924fd761abf11d354dadad57a7ab502a06b947d","sha256:604650fad6ff58e1d72a4c72edc1742dcf64ee4fb3b51e6edc4371dd5656a0e1"],"state_sha256":"7a0041a76e4aba389b13e730e4c32ed9e62a806b83d59d4ac7bb625bf4124300"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XruPIH13TJz6sZDMqdDa9RTBJR8JW9XRRIFkdk5C6K9f8yEo9bo/uFSOphTElscIgVR5HPBUdi4nlszXM536Cg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T16:17:03.329643Z","bundle_sha256":"b7ee346b49b15a40569a19c3311b85851e7afe9a1b5b7110494c301ec5c44466"}}