{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:PZRMCXE3HSMZPPHHX6G5XYKHTB","short_pith_number":"pith:PZRMCXE3","canonical_record":{"source":{"id":"2605.26069","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-05-25T17:33:26Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"3956127a704393dce91a52cf9ee306c8578f8fe11464392b5f3163a91a26a122","abstract_canon_sha256":"8c7615ea89ef466798329fa95c52b38f68dfcf6cbd73aae921a39a58baab5447"},"schema_version":"1.0"},"canonical_sha256":"7e62c15c9b3c9997bce7bf8ddbe1479866d4948c0290fff73dd2c7473d718f1c","source":{"kind":"arxiv","id":"2605.26069","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.26069","created_at":"2026-05-26T02:05:25Z"},{"alias_kind":"arxiv_version","alias_value":"2605.26069v1","created_at":"2026-05-26T02:05:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.26069","created_at":"2026-05-26T02:05:25Z"},{"alias_kind":"pith_short_12","alias_value":"PZRMCXE3HSMZ","created_at":"2026-05-26T02:05:25Z"},{"alias_kind":"pith_short_16","alias_value":"PZRMCXE3HSMZPPHH","created_at":"2026-05-26T02:05:25Z"},{"alias_kind":"pith_short_8","alias_value":"PZRMCXE3","created_at":"2026-05-26T02:05:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:PZRMCXE3HSMZPPHHX6G5XYKHTB","target":"record","payload":{"canonical_record":{"source":{"id":"2605.26069","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-05-25T17:33:26Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"3956127a704393dce91a52cf9ee306c8578f8fe11464392b5f3163a91a26a122","abstract_canon_sha256":"8c7615ea89ef466798329fa95c52b38f68dfcf6cbd73aae921a39a58baab5447"},"schema_version":"1.0"},"canonical_sha256":"7e62c15c9b3c9997bce7bf8ddbe1479866d4948c0290fff73dd2c7473d718f1c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-26T02:05:25.695749Z","signature_b64":"hBromI8SplrL0452BKnukmaOOG98wr7fnM9PMitQd5ALWLyse7K/ZrWyL32bYgw3waRfSdeJnfgsveqmiTxVAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7e62c15c9b3c9997bce7bf8ddbe1479866d4948c0290fff73dd2c7473d718f1c","last_reissued_at":"2026-05-26T02:05:25.695047Z","signature_status":"signed_v1","first_computed_at":"2026-05-26T02:05:25.695047Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2605.26069","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":"2026-05-26T02:05:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9ybpNFDJOnOKiJQbhl3QPb06LlSBDQZTz3Jc9JGL27+w8JJ27gGN/hbBQ7W37PAbUjDNSEHWlEcbIs2ASdgTAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T11:33:55.776649Z"},"content_sha256":"ec88b3966dc4a20dde3a0d4886248694265d2ec58cb7c9258b7203c1193772a0","schema_version":"1.0","event_id":"sha256:ec88b3966dc4a20dde3a0d4886248694265d2ec58cb7c9258b7203c1193772a0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:PZRMCXE3HSMZPPHHX6G5XYKHTB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Effect of slow bonds on current fluctuations in the symmetric simple exclusion process","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"cond-mat.stat-mech","authors_text":"Kapil Sharma, Sandeep Jangid, Soumyabrata Saha, Tridib Sadhu","submitted_at":"2026-05-25T17:33:26Z","abstract_excerpt":"The symmetric simple exclusion process (SSEP) is a paradigmatic model of classical non-equilibrium dynamics. Exact results for large deviations of particle current in the SSEP have been obtained in various settings using integrability-based methods. In this Article, we discuss how these results are modified in the presence of localized slow bonds. We consider three conventional geometries: (a) a finite one-dimensional lattice weakly coupled to unequal reservoirs at its boundaries, (b) a semi-infinite one-dimensional lattice weakly coupled to a boundary reservoir, and (c) an infinite one-dimens"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2605.26069","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2605.26069/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-05-26T02:05:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Y3OfVyiVbwjjwKZg0EiQNt69uV69AGK+2EeamWND/lypKgAzMhJQLp6x6eLIe0FTs3Plfn8/kI5roKUFw6xeBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T11:33:55.777007Z"},"content_sha256":"168eeebe9e10950699ae46433ef2e8a6b8260e7bda2d4439ccdb407dfe4ad956","schema_version":"1.0","event_id":"sha256:168eeebe9e10950699ae46433ef2e8a6b8260e7bda2d4439ccdb407dfe4ad956"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PZRMCXE3HSMZPPHHX6G5XYKHTB/bundle.json","state_url":"https://pith.science/pith/PZRMCXE3HSMZPPHHX6G5XYKHTB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PZRMCXE3HSMZPPHHX6G5XYKHTB/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":"2026-05-28T11:33:55Z","links":{"resolver":"https://pith.science/pith/PZRMCXE3HSMZPPHHX6G5XYKHTB","bundle":"https://pith.science/pith/PZRMCXE3HSMZPPHHX6G5XYKHTB/bundle.json","state":"https://pith.science/pith/PZRMCXE3HSMZPPHHX6G5XYKHTB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PZRMCXE3HSMZPPHHX6G5XYKHTB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:PZRMCXE3HSMZPPHHX6G5XYKHTB","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":"8c7615ea89ef466798329fa95c52b38f68dfcf6cbd73aae921a39a58baab5447","cross_cats_sorted":["math-ph","math.MP"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-05-25T17:33:26Z","title_canon_sha256":"3956127a704393dce91a52cf9ee306c8578f8fe11464392b5f3163a91a26a122"},"schema_version":"1.0","source":{"id":"2605.26069","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.26069","created_at":"2026-05-26T02:05:25Z"},{"alias_kind":"arxiv_version","alias_value":"2605.26069v1","created_at":"2026-05-26T02:05:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.26069","created_at":"2026-05-26T02:05:25Z"},{"alias_kind":"pith_short_12","alias_value":"PZRMCXE3HSMZ","created_at":"2026-05-26T02:05:25Z"},{"alias_kind":"pith_short_16","alias_value":"PZRMCXE3HSMZPPHH","created_at":"2026-05-26T02:05:25Z"},{"alias_kind":"pith_short_8","alias_value":"PZRMCXE3","created_at":"2026-05-26T02:05:25Z"}],"graph_snapshots":[{"event_id":"sha256:168eeebe9e10950699ae46433ef2e8a6b8260e7bda2d4439ccdb407dfe4ad956","target":"graph","created_at":"2026-05-26T02:05:25Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2605.26069/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The symmetric simple exclusion process (SSEP) is a paradigmatic model of classical non-equilibrium dynamics. Exact results for large deviations of particle current in the SSEP have been obtained in various settings using integrability-based methods. In this Article, we discuss how these results are modified in the presence of localized slow bonds. We consider three conventional geometries: (a) a finite one-dimensional lattice weakly coupled to unequal reservoirs at its boundaries, (b) a semi-infinite one-dimensional lattice weakly coupled to a boundary reservoir, and (c) an infinite one-dimens","authors_text":"Kapil Sharma, Sandeep Jangid, Soumyabrata Saha, Tridib Sadhu","cross_cats":["math-ph","math.MP"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-05-25T17:33:26Z","title":"Effect of slow bonds on current fluctuations in the symmetric simple exclusion process"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2605.26069","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:ec88b3966dc4a20dde3a0d4886248694265d2ec58cb7c9258b7203c1193772a0","target":"record","created_at":"2026-05-26T02:05:25Z","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":"8c7615ea89ef466798329fa95c52b38f68dfcf6cbd73aae921a39a58baab5447","cross_cats_sorted":["math-ph","math.MP"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-05-25T17:33:26Z","title_canon_sha256":"3956127a704393dce91a52cf9ee306c8578f8fe11464392b5f3163a91a26a122"},"schema_version":"1.0","source":{"id":"2605.26069","kind":"arxiv","version":1}},"canonical_sha256":"7e62c15c9b3c9997bce7bf8ddbe1479866d4948c0290fff73dd2c7473d718f1c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7e62c15c9b3c9997bce7bf8ddbe1479866d4948c0290fff73dd2c7473d718f1c","first_computed_at":"2026-05-26T02:05:25.695047Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-26T02:05:25.695047Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"hBromI8SplrL0452BKnukmaOOG98wr7fnM9PMitQd5ALWLyse7K/ZrWyL32bYgw3waRfSdeJnfgsveqmiTxVAg==","signature_status":"signed_v1","signed_at":"2026-05-26T02:05:25.695749Z","signed_message":"canonical_sha256_bytes"},"source_id":"2605.26069","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ec88b3966dc4a20dde3a0d4886248694265d2ec58cb7c9258b7203c1193772a0","sha256:168eeebe9e10950699ae46433ef2e8a6b8260e7bda2d4439ccdb407dfe4ad956"],"state_sha256":"72c43bc985b487ef93d8de96134c2c35012c94926343b0e17870d43d8e8a4cdd"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WZ3m3kzqkmZSS9b81SLhlI8VilBvkpMaw4aERVqE/qQNmIF7LVStRsnQZDHDGCF8ve153KAJgiWMDMNirZ/aBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T11:33:55.778940Z","bundle_sha256":"e263404206b197d9d318bde615a25f901f508242cb79076895fa37920470b2ea"}}