{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:6M4CP52JDVMMGPQD6YKQUHHY3K","short_pith_number":"pith:6M4CP52J","canonical_record":{"source":{"id":"1710.02283","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2017-10-06T06:06:53Z","cross_cats_sorted":[],"title_canon_sha256":"7eaaf69ff7749749e4af3b12439cab009cc739ee20eafbaac57ebfb17b8c0a6e","abstract_canon_sha256":"2a232c6ec5865dfa059456beefa3a2c2fd983618a369f0942d309ce3f55204ac"},"schema_version":"1.0"},"canonical_sha256":"f33827f7491d58c33e03f6150a1cf8da8a9cf2d6d91414627f777ea44554720c","source":{"kind":"arxiv","id":"1710.02283","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.02283","created_at":"2026-05-18T00:23:32Z"},{"alias_kind":"arxiv_version","alias_value":"1710.02283v1","created_at":"2026-05-18T00:23:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.02283","created_at":"2026-05-18T00:23:32Z"},{"alias_kind":"pith_short_12","alias_value":"6M4CP52JDVMM","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_16","alias_value":"6M4CP52JDVMMGPQD","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_8","alias_value":"6M4CP52J","created_at":"2026-05-18T12:31:03Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:6M4CP52JDVMMGPQD6YKQUHHY3K","target":"record","payload":{"canonical_record":{"source":{"id":"1710.02283","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2017-10-06T06:06:53Z","cross_cats_sorted":[],"title_canon_sha256":"7eaaf69ff7749749e4af3b12439cab009cc739ee20eafbaac57ebfb17b8c0a6e","abstract_canon_sha256":"2a232c6ec5865dfa059456beefa3a2c2fd983618a369f0942d309ce3f55204ac"},"schema_version":"1.0"},"canonical_sha256":"f33827f7491d58c33e03f6150a1cf8da8a9cf2d6d91414627f777ea44554720c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:23:32.743945Z","signature_b64":"TFWyRjYTKZA8BQ9PBJ5XnC/QU3ToMT4jiPWxYZLbTsMMP/q07Wvbls/mM6RWfX1o9PH/8PKaz6M5HYxIk9dXCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f33827f7491d58c33e03f6150a1cf8da8a9cf2d6d91414627f777ea44554720c","last_reissued_at":"2026-05-18T00:23:32.743433Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:23:32.743433Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1710.02283","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":"2026-05-18T00:23:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yu4FmPMVMiYaVi67N0yDtgCduefy4TfY5ybNMz+5nBPS8D3SMqTS4WkITcdfEIm+BxpWs7Cz6KURewJEiPXtDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T14:03:31.345080Z"},"content_sha256":"0a9b5f84a1e1851a4dd3e90e4e834ad3315ada7f69f6dfcea60903ee2062efe9","schema_version":"1.0","event_id":"sha256:0a9b5f84a1e1851a4dd3e90e4e834ad3315ada7f69f6dfcea60903ee2062efe9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:6M4CP52JDVMMGPQD6YKQUHHY3K","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Diffusion dynamics and steady states of systems of hard rods on the square lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.soft","authors_text":"Dibyendu Das, Mithun K. Mitra, R. Rajesh, Saugata Patra","submitted_at":"2017-10-06T06:06:53Z","abstract_excerpt":"It is known from grand canonical simulations of a system of hard rods on two dimensional lattices that an orientationally ordered nematic phase exists only when the length of the rods is at least seven. However, a recent microcanonical simulation with diffusion kinetics, conserving both total density and zero nematic order, reported the existence of a nematically phase segregated steady state with interfaces in the diagonal direction for rods of length six [Phys. Rev. E 95, 052130 (2017)], violating the equivalence of different ensembles for systems in equilibrium. We resolve this inconsistenc"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.02283","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":"2026-05-18T00:23:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vNIG51mfMbjro85vlMba0bcTy2IIn2WPwNH0ZZXQxjNMO2YG6j2JsJUFz9RXUtrAYex8aculpAIwMPUoZ8SrDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T14:03:31.345774Z"},"content_sha256":"3111d6db047633051c6f79740b1fdaded9c9d47b7b112fc1e031eee2ca87cd51","schema_version":"1.0","event_id":"sha256:3111d6db047633051c6f79740b1fdaded9c9d47b7b112fc1e031eee2ca87cd51"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6M4CP52JDVMMGPQD6YKQUHHY3K/bundle.json","state_url":"https://pith.science/pith/6M4CP52JDVMMGPQD6YKQUHHY3K/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6M4CP52JDVMMGPQD6YKQUHHY3K/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":"2026-05-30T14:03:31Z","links":{"resolver":"https://pith.science/pith/6M4CP52JDVMMGPQD6YKQUHHY3K","bundle":"https://pith.science/pith/6M4CP52JDVMMGPQD6YKQUHHY3K/bundle.json","state":"https://pith.science/pith/6M4CP52JDVMMGPQD6YKQUHHY3K/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6M4CP52JDVMMGPQD6YKQUHHY3K/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:6M4CP52JDVMMGPQD6YKQUHHY3K","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":"2a232c6ec5865dfa059456beefa3a2c2fd983618a369f0942d309ce3f55204ac","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2017-10-06T06:06:53Z","title_canon_sha256":"7eaaf69ff7749749e4af3b12439cab009cc739ee20eafbaac57ebfb17b8c0a6e"},"schema_version":"1.0","source":{"id":"1710.02283","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.02283","created_at":"2026-05-18T00:23:32Z"},{"alias_kind":"arxiv_version","alias_value":"1710.02283v1","created_at":"2026-05-18T00:23:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.02283","created_at":"2026-05-18T00:23:32Z"},{"alias_kind":"pith_short_12","alias_value":"6M4CP52JDVMM","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_16","alias_value":"6M4CP52JDVMMGPQD","created_at":"2026-05-18T12:31:03Z"},{"alias_kind":"pith_short_8","alias_value":"6M4CP52J","created_at":"2026-05-18T12:31:03Z"}],"graph_snapshots":[{"event_id":"sha256:3111d6db047633051c6f79740b1fdaded9c9d47b7b112fc1e031eee2ca87cd51","target":"graph","created_at":"2026-05-18T00:23:32Z","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":"It is known from grand canonical simulations of a system of hard rods on two dimensional lattices that an orientationally ordered nematic phase exists only when the length of the rods is at least seven. However, a recent microcanonical simulation with diffusion kinetics, conserving both total density and zero nematic order, reported the existence of a nematically phase segregated steady state with interfaces in the diagonal direction for rods of length six [Phys. Rev. E 95, 052130 (2017)], violating the equivalence of different ensembles for systems in equilibrium. We resolve this inconsistenc","authors_text":"Dibyendu Das, Mithun K. Mitra, R. Rajesh, Saugata Patra","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2017-10-06T06:06:53Z","title":"Diffusion dynamics and steady states of systems of hard rods on the square lattice"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.02283","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":"sha256:0a9b5f84a1e1851a4dd3e90e4e834ad3315ada7f69f6dfcea60903ee2062efe9","target":"record","created_at":"2026-05-18T00:23:32Z","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":"2a232c6ec5865dfa059456beefa3a2c2fd983618a369f0942d309ce3f55204ac","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2017-10-06T06:06:53Z","title_canon_sha256":"7eaaf69ff7749749e4af3b12439cab009cc739ee20eafbaac57ebfb17b8c0a6e"},"schema_version":"1.0","source":{"id":"1710.02283","kind":"arxiv","version":1}},"canonical_sha256":"f33827f7491d58c33e03f6150a1cf8da8a9cf2d6d91414627f777ea44554720c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f33827f7491d58c33e03f6150a1cf8da8a9cf2d6d91414627f777ea44554720c","first_computed_at":"2026-05-18T00:23:32.743433Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:23:32.743433Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"TFWyRjYTKZA8BQ9PBJ5XnC/QU3ToMT4jiPWxYZLbTsMMP/q07Wvbls/mM6RWfX1o9PH/8PKaz6M5HYxIk9dXCg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:23:32.743945Z","signed_message":"canonical_sha256_bytes"},"source_id":"1710.02283","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0a9b5f84a1e1851a4dd3e90e4e834ad3315ada7f69f6dfcea60903ee2062efe9","sha256:3111d6db047633051c6f79740b1fdaded9c9d47b7b112fc1e031eee2ca87cd51"],"state_sha256":"05e9840d11784d0124a043226e18a16c5e148a4e41ced83cf83ef323ac2acb74"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PIAHVnPCa/T8sIyzTgJFKuxUeA9jLIc6vp6GWQUodcUBmIeDjZGl03B5YlaS/FKHbj+t454xt7TF/RmmSshxBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T14:03:31.350446Z","bundle_sha256":"0173cf8e7534c96616df699886d26ffe5e669b36b0b031176f9c4146182535cb"}}