{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:XAD55GYSRDMVIIIPVVAR4BZX6Q","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":"50a7b3f0fa6b0a7d9f86eb41e3ea2c3ce570e2a80c33c979c90db65f1c12202f","cross_cats_sorted":["cond-mat.mtrl-sci","physics.bio-ph"],"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"physics.comp-ph","submitted_at":"2022-07-12T16:06:18Z","title_canon_sha256":"73ff5e2c0e3d090e366baef8e5a331a87a45fc376206d36398823ef0f3e34435"},"schema_version":"1.0","source":{"id":"2207.05635","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2207.05635","created_at":"2026-07-05T04:39:44Z"},{"alias_kind":"arxiv_version","alias_value":"2207.05635v1","created_at":"2026-07-05T04:39:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2207.05635","created_at":"2026-07-05T04:39:44Z"},{"alias_kind":"pith_short_12","alias_value":"XAD55GYSRDMV","created_at":"2026-07-05T04:39:44Z"},{"alias_kind":"pith_short_16","alias_value":"XAD55GYSRDMVIIIP","created_at":"2026-07-05T04:39:44Z"},{"alias_kind":"pith_short_8","alias_value":"XAD55GYS","created_at":"2026-07-05T04:39:44Z"}],"graph_snapshots":[{"event_id":"sha256:5a0e8dd558ab36eb7886ffa83d151e8930ea994b60c054f5e8b0b0b40d2a1517","target":"graph","created_at":"2026-07-05T04:39:44Z","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/2207.05635/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The Martini 3 force field is a full re-parametrization of the Martini coarse-grained model for biomolecular simulations. Due to the improved interaction balance it allows for more accurate description of condensed phase systems. In the present work we develop a consistent strategy to parametrize carbohydrate molecules accurately within the framework of Martini 3. In particular, we develop a canonical mapping scheme that decomposes arbitrarily large carbohydrates into a limited number of fragments. Bead types for these fragments have been assigned by matching physicochemical properties of mono-","authors_text":"Elizabeth E. Jefferys, Fabian Gr\\\"unewald, Maarit Karonen, Mark S. P. Sansom, Mats H. Punt, Melanie K\\\"onig, Paulo C. T Souza, Petteri A. Vainikka, Siewert J. Marrink, Valtteri Virtanen, Weria Pezeshkian","cross_cats":["cond-mat.mtrl-sci","physics.bio-ph"],"headline":"","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"physics.comp-ph","submitted_at":"2022-07-12T16:06:18Z","title":"Martini 3 Coarse-Grained Force Field for Carbohydrates"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2207.05635","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:a91a2e2fa4e7f35aa98164d045e78b92a647b75a326665e1654f5ae12adb5d87","target":"record","created_at":"2026-07-05T04:39:44Z","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":"50a7b3f0fa6b0a7d9f86eb41e3ea2c3ce570e2a80c33c979c90db65f1c12202f","cross_cats_sorted":["cond-mat.mtrl-sci","physics.bio-ph"],"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"physics.comp-ph","submitted_at":"2022-07-12T16:06:18Z","title_canon_sha256":"73ff5e2c0e3d090e366baef8e5a331a87a45fc376206d36398823ef0f3e34435"},"schema_version":"1.0","source":{"id":"2207.05635","kind":"arxiv","version":1}},"canonical_sha256":"b807de9b1288d954210fad411e0737f43426a9374689bd3bb9b1f3aa706b4d5a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b807de9b1288d954210fad411e0737f43426a9374689bd3bb9b1f3aa706b4d5a","first_computed_at":"2026-07-05T04:39:44.754824Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:39:44.754824Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"gTiiBLi85xYv/lX6FOKQSLTPZlIWLRAlf4R4lZ0WpZibqVs6eqFEKkQ+lP9PVjj1SUiUuLFzNHJELTa7/2bCAA==","signature_status":"signed_v1","signed_at":"2026-07-05T04:39:44.755219Z","signed_message":"canonical_sha256_bytes"},"source_id":"2207.05635","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a91a2e2fa4e7f35aa98164d045e78b92a647b75a326665e1654f5ae12adb5d87","sha256:5a0e8dd558ab36eb7886ffa83d151e8930ea994b60c054f5e8b0b0b40d2a1517"],"state_sha256":"0ed362bdb798bb8c67b234cf6e2f8d745e21d6ecd4a892c223f14c189859c567"}