{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:PIUALV422AWAADKXUQ2Y4FQVLZ","short_pith_number":"pith:PIUALV42","canonical_record":{"source":{"id":"1803.00484","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2018-03-01T16:30:54Z","cross_cats_sorted":[],"title_canon_sha256":"e3d825fae0d6cad238ba12ebcfc73c29b375a031f8ddcf94fdf97383b599450b","abstract_canon_sha256":"43609d30eed71012358311b8a3bb94e3e6132a4a8517b8841f96996c977a56e7"},"schema_version":"1.0"},"canonical_sha256":"7a2805d79ad02c000d57a4358e16155e73724fbbc6e0ee0c9ca8ebaf6e3416b9","source":{"kind":"arxiv","id":"1803.00484","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1803.00484","created_at":"2026-05-18T00:22:11Z"},{"alias_kind":"arxiv_version","alias_value":"1803.00484v1","created_at":"2026-05-18T00:22:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1803.00484","created_at":"2026-05-18T00:22:11Z"},{"alias_kind":"pith_short_12","alias_value":"PIUALV422AWA","created_at":"2026-05-18T12:32:43Z"},{"alias_kind":"pith_short_16","alias_value":"PIUALV422AWAADKX","created_at":"2026-05-18T12:32:43Z"},{"alias_kind":"pith_short_8","alias_value":"PIUALV42","created_at":"2026-05-18T12:32:43Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:PIUALV422AWAADKXUQ2Y4FQVLZ","target":"record","payload":{"canonical_record":{"source":{"id":"1803.00484","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2018-03-01T16:30:54Z","cross_cats_sorted":[],"title_canon_sha256":"e3d825fae0d6cad238ba12ebcfc73c29b375a031f8ddcf94fdf97383b599450b","abstract_canon_sha256":"43609d30eed71012358311b8a3bb94e3e6132a4a8517b8841f96996c977a56e7"},"schema_version":"1.0"},"canonical_sha256":"7a2805d79ad02c000d57a4358e16155e73724fbbc6e0ee0c9ca8ebaf6e3416b9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:22:11.606404Z","signature_b64":"btliqInq2MWZS1CBfBkigBJOt2C0quksZhtzFrbtuBN5Fk73+XO7emvfOfMH0JDRfIbN0jMPq8Vt7doSEUE3CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7a2805d79ad02c000d57a4358e16155e73724fbbc6e0ee0c9ca8ebaf6e3416b9","last_reissued_at":"2026-05-18T00:22:11.605778Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:22:11.605778Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1803.00484","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":"2026-05-18T00:22:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/xadJjceZ0OKp/1QFg8t0Pp92fGv8PPqE1QFj6Cy+s2/XFgl55n0qepNBzYuNQZigh7lFhjiRMSkAEKWfHarCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T14:51:11.158983Z"},"content_sha256":"972f6b194c32bdd91110c360af40ba2377aeda9cbaf3a55a7df27ec0bb26fc80","schema_version":"1.0","event_id":"sha256:972f6b194c32bdd91110c360af40ba2377aeda9cbaf3a55a7df27ec0bb26fc80"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:PIUALV422AWAADKXUQ2Y4FQVLZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"DL_MONTE: A multipurpose code for Monte Carlo simulation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.comp-ph","authors_text":"Andrey V. Brukhno, James Grant, John A. Purton, Kevin Stratford, Nigel B. Wilding, Stephen C. Parker, Tom L. Underwood","submitted_at":"2018-03-01T16:30:54Z","abstract_excerpt":"DL_MONTE is an open source, general-purpose software package for performing Monte Carlo simulations. It includes a wide variety of force fields and MC techniques, and thus is applicable to a broad range of problems in molecular simulation. Here we provide an overview of DL_MONTE, focusing on key features recently added to the package. These include the ability to treat systems confined to a planar pore (i.e. `slit' or `slab' boundary conditions); the lattice-switch Monte Carlo (LSMC) method for evaluating precise free energy differences between competing polymorphs; various commonly-used metho"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1803.00484","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":"2026-05-18T00:22:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UfMRTU9KGQHa2uvelyu38c1CK32dJI2eHNSVHMLZQNzatqa6tyxlKa0fPyi3ppqJp7swZqb0y7BA1JWbu+jfCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T14:51:11.159363Z"},"content_sha256":"44931de76831d99056c0abb4018c9891eb329a20d55879212a142d2e8e12f1ab","schema_version":"1.0","event_id":"sha256:44931de76831d99056c0abb4018c9891eb329a20d55879212a142d2e8e12f1ab"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PIUALV422AWAADKXUQ2Y4FQVLZ/bundle.json","state_url":"https://pith.science/pith/PIUALV422AWAADKXUQ2Y4FQVLZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PIUALV422AWAADKXUQ2Y4FQVLZ/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":"2026-05-28T14:51:11Z","links":{"resolver":"https://pith.science/pith/PIUALV422AWAADKXUQ2Y4FQVLZ","bundle":"https://pith.science/pith/PIUALV422AWAADKXUQ2Y4FQVLZ/bundle.json","state":"https://pith.science/pith/PIUALV422AWAADKXUQ2Y4FQVLZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PIUALV422AWAADKXUQ2Y4FQVLZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:PIUALV422AWAADKXUQ2Y4FQVLZ","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":"43609d30eed71012358311b8a3bb94e3e6132a4a8517b8841f96996c977a56e7","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2018-03-01T16:30:54Z","title_canon_sha256":"e3d825fae0d6cad238ba12ebcfc73c29b375a031f8ddcf94fdf97383b599450b"},"schema_version":"1.0","source":{"id":"1803.00484","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1803.00484","created_at":"2026-05-18T00:22:11Z"},{"alias_kind":"arxiv_version","alias_value":"1803.00484v1","created_at":"2026-05-18T00:22:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1803.00484","created_at":"2026-05-18T00:22:11Z"},{"alias_kind":"pith_short_12","alias_value":"PIUALV422AWA","created_at":"2026-05-18T12:32:43Z"},{"alias_kind":"pith_short_16","alias_value":"PIUALV422AWAADKX","created_at":"2026-05-18T12:32:43Z"},{"alias_kind":"pith_short_8","alias_value":"PIUALV42","created_at":"2026-05-18T12:32:43Z"}],"graph_snapshots":[{"event_id":"sha256:44931de76831d99056c0abb4018c9891eb329a20d55879212a142d2e8e12f1ab","target":"graph","created_at":"2026-05-18T00:22:11Z","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":"DL_MONTE is an open source, general-purpose software package for performing Monte Carlo simulations. It includes a wide variety of force fields and MC techniques, and thus is applicable to a broad range of problems in molecular simulation. Here we provide an overview of DL_MONTE, focusing on key features recently added to the package. These include the ability to treat systems confined to a planar pore (i.e. `slit' or `slab' boundary conditions); the lattice-switch Monte Carlo (LSMC) method for evaluating precise free energy differences between competing polymorphs; various commonly-used metho","authors_text":"Andrey V. Brukhno, James Grant, John A. Purton, Kevin Stratford, Nigel B. Wilding, Stephen C. Parker, Tom L. Underwood","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2018-03-01T16:30:54Z","title":"DL_MONTE: A multipurpose code for Monte Carlo simulation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1803.00484","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":"sha256:972f6b194c32bdd91110c360af40ba2377aeda9cbaf3a55a7df27ec0bb26fc80","target":"record","created_at":"2026-05-18T00:22:11Z","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":"43609d30eed71012358311b8a3bb94e3e6132a4a8517b8841f96996c977a56e7","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2018-03-01T16:30:54Z","title_canon_sha256":"e3d825fae0d6cad238ba12ebcfc73c29b375a031f8ddcf94fdf97383b599450b"},"schema_version":"1.0","source":{"id":"1803.00484","kind":"arxiv","version":1}},"canonical_sha256":"7a2805d79ad02c000d57a4358e16155e73724fbbc6e0ee0c9ca8ebaf6e3416b9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7a2805d79ad02c000d57a4358e16155e73724fbbc6e0ee0c9ca8ebaf6e3416b9","first_computed_at":"2026-05-18T00:22:11.605778Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:22:11.605778Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"btliqInq2MWZS1CBfBkigBJOt2C0quksZhtzFrbtuBN5Fk73+XO7emvfOfMH0JDRfIbN0jMPq8Vt7doSEUE3CQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:22:11.606404Z","signed_message":"canonical_sha256_bytes"},"source_id":"1803.00484","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:972f6b194c32bdd91110c360af40ba2377aeda9cbaf3a55a7df27ec0bb26fc80","sha256:44931de76831d99056c0abb4018c9891eb329a20d55879212a142d2e8e12f1ab"],"state_sha256":"91b18ea355236c6827da70eff17a0437e4dab26d64771f88c37cb5918bddd7d2"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GghHO1wmGuK67eFJ2nYuKhob+WJanmacP4gI2Ld1U8xzQQtXsVdVQsM2ybysHZ72u47I6VmakXjilpHSou1YBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T14:51:11.161338Z","bundle_sha256":"6213d0cc482c204c725a6400c21971b2dc2daf2f524606df1e89b2977cfb151f"}}