{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:637DUXNQ3ATIFLZWQ4H4PTUOEG","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":"75b03dd7d01dd6444b3912fb330686307eca8499d37d36e79334a1d2876eec51","cross_cats_sorted":["cond-mat.soft","q-bio.BM"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.bio-ph","submitted_at":"2016-07-26T17:11:11Z","title_canon_sha256":"4363ede9a11b08dce4769cb6561249b31a66bb3d44ecd5d278ee3f30772c2686"},"schema_version":"1.0","source":{"id":"1607.07809","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1607.07809","created_at":"2026-05-18T01:10:25Z"},{"alias_kind":"arxiv_version","alias_value":"1607.07809v1","created_at":"2026-05-18T01:10:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1607.07809","created_at":"2026-05-18T01:10:25Z"},{"alias_kind":"pith_short_12","alias_value":"637DUXNQ3ATI","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_16","alias_value":"637DUXNQ3ATIFLZW","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_8","alias_value":"637DUXNQ","created_at":"2026-05-18T12:30:01Z"}],"graph_snapshots":[{"event_id":"sha256:9f36a763913a78d32afc275b486da052b3570d217a5a90ad5503407b1b5bab72","target":"graph","created_at":"2026-05-18T01:10:25Z","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"},"paper":{"abstract_excerpt":"We assume that the protein folding process follows two autonomous steps: the conformational search for the native, mainly ruled by the hydrophobic effect; and, the final adjustment stage, which eventually gives stability to the native. Our main tool of investigation is a 3D lattice model provided with a ten-letter alphabet, the stereochemical model. This model was conceived for Monte Carlo (MC) simulations when one keeps in mind the kinetic behavior of protein-like chains in solution. In order to characterize the folding characteristic time ({\\tau}) by two distinct sampling methods, first we p","authors_text":"A. Caliri, J.P. Dal Molin","cross_cats":["cond-mat.soft","q-bio.BM"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.bio-ph","submitted_at":"2016-07-26T17:11:11Z","title":"Entropic formulation for the protein folding process: hydrophobic stability correlates with folding rates"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1607.07809","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:c752837862f1414bc27dfdaa68a4e5a0047f7b53386dbf821dc3e87132e7cb71","target":"record","created_at":"2026-05-18T01:10:25Z","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":"75b03dd7d01dd6444b3912fb330686307eca8499d37d36e79334a1d2876eec51","cross_cats_sorted":["cond-mat.soft","q-bio.BM"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.bio-ph","submitted_at":"2016-07-26T17:11:11Z","title_canon_sha256":"4363ede9a11b08dce4769cb6561249b31a66bb3d44ecd5d278ee3f30772c2686"},"schema_version":"1.0","source":{"id":"1607.07809","kind":"arxiv","version":1}},"canonical_sha256":"f6fe3a5db0d82682af36870fc7ce8e218516dd73d07d8960e657dbf8870128db","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f6fe3a5db0d82682af36870fc7ce8e218516dd73d07d8960e657dbf8870128db","first_computed_at":"2026-05-18T01:10:25.115980Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:10:25.115980Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"pcx7jtmw4ERrVwX/opz1BeZORojRDnZnLyBtAew0EcT2xm+cO6LsEUK7TDavNV70dM2p50IXQ+Dgb+KQjRM6CA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:10:25.116543Z","signed_message":"canonical_sha256_bytes"},"source_id":"1607.07809","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c752837862f1414bc27dfdaa68a4e5a0047f7b53386dbf821dc3e87132e7cb71","sha256:9f36a763913a78d32afc275b486da052b3570d217a5a90ad5503407b1b5bab72"],"state_sha256":"d43e89917a008d44ad1c92416b1c2be46949b897f3833a74a193c5f05d502f9d"}