{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:BASBYYRUNVRE4QUFQB4KRN2BTX","short_pith_number":"pith:BASBYYRU","canonical_record":{"source":{"id":"1803.09300","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2018-03-25T18:06:16Z","cross_cats_sorted":["physics.chem-ph"],"title_canon_sha256":"0fc3d30dc8eec3bc9aadf9a781566a37358e15e3e222cf74c2bc45086502374f","abstract_canon_sha256":"df530eff267ac6c5acd01b7c3e58ce1f94a67341a598b385ed7c750f72b699a2"},"schema_version":"1.0"},"canonical_sha256":"08241c62346d624e42858078a8b7419dc146f9da3718cf0655c96384b29e5811","source":{"kind":"arxiv","id":"1803.09300","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1803.09300","created_at":"2026-05-17T23:59:09Z"},{"alias_kind":"arxiv_version","alias_value":"1803.09300v1","created_at":"2026-05-17T23:59:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1803.09300","created_at":"2026-05-17T23:59:09Z"},{"alias_kind":"pith_short_12","alias_value":"BASBYYRUNVRE","created_at":"2026-05-18T12:32:13Z"},{"alias_kind":"pith_short_16","alias_value":"BASBYYRUNVRE4QUF","created_at":"2026-05-18T12:32:13Z"},{"alias_kind":"pith_short_8","alias_value":"BASBYYRU","created_at":"2026-05-18T12:32:13Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:BASBYYRUNVRE4QUFQB4KRN2BTX","target":"record","payload":{"canonical_record":{"source":{"id":"1803.09300","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2018-03-25T18:06:16Z","cross_cats_sorted":["physics.chem-ph"],"title_canon_sha256":"0fc3d30dc8eec3bc9aadf9a781566a37358e15e3e222cf74c2bc45086502374f","abstract_canon_sha256":"df530eff267ac6c5acd01b7c3e58ce1f94a67341a598b385ed7c750f72b699a2"},"schema_version":"1.0"},"canonical_sha256":"08241c62346d624e42858078a8b7419dc146f9da3718cf0655c96384b29e5811","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:59:09.443719Z","signature_b64":"FgNw+P2gxm5dIuie/NYj1ois9LA2k/OKL3gAnB6ighTMJ/G0WPdpNBJhh0fXrGvPurnWc2JSEFispPZ5TbaeDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"08241c62346d624e42858078a8b7419dc146f9da3718cf0655c96384b29e5811","last_reissued_at":"2026-05-17T23:59:09.443202Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:59:09.443202Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1803.09300","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":"2026-05-17T23:59:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zgmj9l7TUCZLAygW75Y1qfIHtJgLVcXy6T4jPpJbZCQ0/JxkT40RWCJlh3QMGTq8/l2ZDebs/8Z85cXzYf1+BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-21T21:49:29.056378Z"},"content_sha256":"7868bbe2e92398efcc0ee9d2cca70d920d98e3c18e47448fbd71b807a6c25e6d","schema_version":"1.0","event_id":"sha256:7868bbe2e92398efcc0ee9d2cca70d920d98e3c18e47448fbd71b807a6c25e6d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:BASBYYRUNVRE4QUFQB4KRN2BTX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Monte Carlo Simulations of Novel Biaxial Ordering in Systems of Uniaxially Interacting Rod-like Ellipsoids","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.chem-ph"],"primary_cat":"cond-mat.soft","authors_text":"Tushar Kanti Bose","submitted_at":"2018-03-25T18:06:16Z","abstract_excerpt":"The minimal ingredient to generate a biaxial liquid crystalline ordering is usually considered to be the strongly biaxial interactions breaking the cylindrical symmetry of the uniaxial molecules. Although there is no fundamental reason to forbid a biaxial ordering of pure uniaxial origin, it has been a long standing problem to find a robust demonstration of such phenomenon in systems of rod-like particles. We report here off-lattice Monte Carlo simulations of some new model systems of polar achiral rodlike ellipsoids which spontaneously exhibit novel biaxial smectic phases of pure uniaxial ori"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1803.09300","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":"2026-05-17T23:59:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JwdYl1YbVt8Re3KMeg09ayDoYGz5BNlt8d0By8BqiWeJIW7nU/GjbZBRY1ilPoXSuDhP9TN61wMdU40hA3x7Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-21T21:49:29.056731Z"},"content_sha256":"fff1c9edbfe6a3e07cefb1730f769090b2b0c3d47e93ca66c88c25783ed8de41","schema_version":"1.0","event_id":"sha256:fff1c9edbfe6a3e07cefb1730f769090b2b0c3d47e93ca66c88c25783ed8de41"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/BASBYYRUNVRE4QUFQB4KRN2BTX/bundle.json","state_url":"https://pith.science/pith/BASBYYRUNVRE4QUFQB4KRN2BTX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/BASBYYRUNVRE4QUFQB4KRN2BTX/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":"2026-06-21T21:49:29Z","links":{"resolver":"https://pith.science/pith/BASBYYRUNVRE4QUFQB4KRN2BTX","bundle":"https://pith.science/pith/BASBYYRUNVRE4QUFQB4KRN2BTX/bundle.json","state":"https://pith.science/pith/BASBYYRUNVRE4QUFQB4KRN2BTX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/BASBYYRUNVRE4QUFQB4KRN2BTX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:BASBYYRUNVRE4QUFQB4KRN2BTX","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":"df530eff267ac6c5acd01b7c3e58ce1f94a67341a598b385ed7c750f72b699a2","cross_cats_sorted":["physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2018-03-25T18:06:16Z","title_canon_sha256":"0fc3d30dc8eec3bc9aadf9a781566a37358e15e3e222cf74c2bc45086502374f"},"schema_version":"1.0","source":{"id":"1803.09300","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1803.09300","created_at":"2026-05-17T23:59:09Z"},{"alias_kind":"arxiv_version","alias_value":"1803.09300v1","created_at":"2026-05-17T23:59:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1803.09300","created_at":"2026-05-17T23:59:09Z"},{"alias_kind":"pith_short_12","alias_value":"BASBYYRUNVRE","created_at":"2026-05-18T12:32:13Z"},{"alias_kind":"pith_short_16","alias_value":"BASBYYRUNVRE4QUF","created_at":"2026-05-18T12:32:13Z"},{"alias_kind":"pith_short_8","alias_value":"BASBYYRU","created_at":"2026-05-18T12:32:13Z"}],"graph_snapshots":[{"event_id":"sha256:fff1c9edbfe6a3e07cefb1730f769090b2b0c3d47e93ca66c88c25783ed8de41","target":"graph","created_at":"2026-05-17T23:59:09Z","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":"The minimal ingredient to generate a biaxial liquid crystalline ordering is usually considered to be the strongly biaxial interactions breaking the cylindrical symmetry of the uniaxial molecules. Although there is no fundamental reason to forbid a biaxial ordering of pure uniaxial origin, it has been a long standing problem to find a robust demonstration of such phenomenon in systems of rod-like particles. We report here off-lattice Monte Carlo simulations of some new model systems of polar achiral rodlike ellipsoids which spontaneously exhibit novel biaxial smectic phases of pure uniaxial ori","authors_text":"Tushar Kanti Bose","cross_cats":["physics.chem-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2018-03-25T18:06:16Z","title":"Monte Carlo Simulations of Novel Biaxial Ordering in Systems of Uniaxially Interacting Rod-like Ellipsoids"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1803.09300","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":"sha256:7868bbe2e92398efcc0ee9d2cca70d920d98e3c18e47448fbd71b807a6c25e6d","target":"record","created_at":"2026-05-17T23:59:09Z","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":"df530eff267ac6c5acd01b7c3e58ce1f94a67341a598b385ed7c750f72b699a2","cross_cats_sorted":["physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2018-03-25T18:06:16Z","title_canon_sha256":"0fc3d30dc8eec3bc9aadf9a781566a37358e15e3e222cf74c2bc45086502374f"},"schema_version":"1.0","source":{"id":"1803.09300","kind":"arxiv","version":1}},"canonical_sha256":"08241c62346d624e42858078a8b7419dc146f9da3718cf0655c96384b29e5811","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"08241c62346d624e42858078a8b7419dc146f9da3718cf0655c96384b29e5811","first_computed_at":"2026-05-17T23:59:09.443202Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:59:09.443202Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"FgNw+P2gxm5dIuie/NYj1ois9LA2k/OKL3gAnB6ighTMJ/G0WPdpNBJhh0fXrGvPurnWc2JSEFispPZ5TbaeDA==","signature_status":"signed_v1","signed_at":"2026-05-17T23:59:09.443719Z","signed_message":"canonical_sha256_bytes"},"source_id":"1803.09300","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7868bbe2e92398efcc0ee9d2cca70d920d98e3c18e47448fbd71b807a6c25e6d","sha256:fff1c9edbfe6a3e07cefb1730f769090b2b0c3d47e93ca66c88c25783ed8de41"],"state_sha256":"13a14318c6e413f0ba679ecba54ce9a6721ab7296e1868ac03311afb8949d9a6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3LpMQ/+kZ5vtc8/2WCt7IQCWydVC0IN9XMf3IJ2GetHL9uB4GpJ7tJGzFP70A6kEzC6gFlsyFWdRw76ha2uwBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-21T21:49:29.058655Z","bundle_sha256":"b6458439ba47d03da3178935a72afff6954c0f271f1c1998e41ccac569f7852f"}}