{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:34RGIPCCY3Q32KZA67DGF5QYMN","short_pith_number":"pith:34RGIPCC","canonical_record":{"source":{"id":"1002.0316","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2010-02-01T19:45:16Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"2870ccf4a3bf205a39114b18e117bce65f749ec64af1d92b76dbda09742d3c44","abstract_canon_sha256":"d6990f4394694d0c4c514e5135217d52f918e34325e57559780411841cf5aef4"},"schema_version":"1.0"},"canonical_sha256":"df22643c42c6e1bd2b20f7c662f618634321a01e0fec9c7bb3ffa3538e92a0eb","source":{"kind":"arxiv","id":"1002.0316","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1002.0316","created_at":"2026-05-18T02:09:21Z"},{"alias_kind":"arxiv_version","alias_value":"1002.0316v2","created_at":"2026-05-18T02:09:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1002.0316","created_at":"2026-05-18T02:09:21Z"},{"alias_kind":"pith_short_12","alias_value":"34RGIPCCY3Q3","created_at":"2026-05-18T12:26:03Z"},{"alias_kind":"pith_short_16","alias_value":"34RGIPCCY3Q32KZA","created_at":"2026-05-18T12:26:03Z"},{"alias_kind":"pith_short_8","alias_value":"34RGIPCC","created_at":"2026-05-18T12:26:03Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:34RGIPCCY3Q32KZA67DGF5QYMN","target":"record","payload":{"canonical_record":{"source":{"id":"1002.0316","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2010-02-01T19:45:16Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"2870ccf4a3bf205a39114b18e117bce65f749ec64af1d92b76dbda09742d3c44","abstract_canon_sha256":"d6990f4394694d0c4c514e5135217d52f918e34325e57559780411841cf5aef4"},"schema_version":"1.0"},"canonical_sha256":"df22643c42c6e1bd2b20f7c662f618634321a01e0fec9c7bb3ffa3538e92a0eb","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:09:21.339725Z","signature_b64":"FR8HkTTxEh7iM7iB+QALxd+HQtVwkVNv9DopFYpMcvG9uF/QZU3ecteRK/4i3oxjewwFb70Ipds0pYqNG/3pBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"df22643c42c6e1bd2b20f7c662f618634321a01e0fec9c7bb3ffa3538e92a0eb","last_reissued_at":"2026-05-18T02:09:21.339084Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:09:21.339084Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1002.0316","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:09:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+Bb7i5sUDCpb+nZqhGk+D7GSDC02mhOKtcTNr+EBQvmtXyK1aLmNo/2aRy2lY+AMbVv/JBDvoKoI5D+U/xWJDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T05:04:35.331221Z"},"content_sha256":"baf2c75cb9989eb5b972b557eba05f7e24f61fbbbe474476b6fb115cb9909346","schema_version":"1.0","event_id":"sha256:baf2c75cb9989eb5b972b557eba05f7e24f61fbbbe474476b6fb115cb9909346"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:34RGIPCCY3Q32KZA67DGF5QYMN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Crystallization of hard aspherical particles","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.soft","authors_text":"Angelo Cacciuto, Behnaz Bozorgui, William L. Miller","submitted_at":"2010-02-01T19:45:16Z","abstract_excerpt":"We use numerical simulations to study the crystallization of monodisperse systems of hard aspherical particles. We find that particle shape and crystallizability can be easily related to each other when particles are characterized in terms of two simple and experimentally accessible order parameters: one based on the particle surface-to-volume ratio, and the other on the angular distribution of the perturbations away from the ideal spherical shape. We present a phase diagram obtained by exploring the crystallizability of 487 different particle shapes across the two-order-parameter spectrum. Fi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1002.0316","kind":"arxiv","version":2},"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":"2026-05-18T02:09:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kRoVPwM7/GbxGrysMgm86JvSlrUP9Jr6/lqSQ87RcBF7jYhnTPkUA0yK6sE3nwdTIEhu+VOPh5fDTGUlI9EiDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T05:04:35.331935Z"},"content_sha256":"d84e16cb0fcfc053b15c572649d479cee9e1db1b579ecec77c0cbbad0fb864f7","schema_version":"1.0","event_id":"sha256:d84e16cb0fcfc053b15c572649d479cee9e1db1b579ecec77c0cbbad0fb864f7"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/34RGIPCCY3Q32KZA67DGF5QYMN/bundle.json","state_url":"https://pith.science/pith/34RGIPCCY3Q32KZA67DGF5QYMN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/34RGIPCCY3Q32KZA67DGF5QYMN/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":"2026-05-27T05:04:35Z","links":{"resolver":"https://pith.science/pith/34RGIPCCY3Q32KZA67DGF5QYMN","bundle":"https://pith.science/pith/34RGIPCCY3Q32KZA67DGF5QYMN/bundle.json","state":"https://pith.science/pith/34RGIPCCY3Q32KZA67DGF5QYMN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/34RGIPCCY3Q32KZA67DGF5QYMN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:34RGIPCCY3Q32KZA67DGF5QYMN","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":"d6990f4394694d0c4c514e5135217d52f918e34325e57559780411841cf5aef4","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2010-02-01T19:45:16Z","title_canon_sha256":"2870ccf4a3bf205a39114b18e117bce65f749ec64af1d92b76dbda09742d3c44"},"schema_version":"1.0","source":{"id":"1002.0316","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1002.0316","created_at":"2026-05-18T02:09:21Z"},{"alias_kind":"arxiv_version","alias_value":"1002.0316v2","created_at":"2026-05-18T02:09:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1002.0316","created_at":"2026-05-18T02:09:21Z"},{"alias_kind":"pith_short_12","alias_value":"34RGIPCCY3Q3","created_at":"2026-05-18T12:26:03Z"},{"alias_kind":"pith_short_16","alias_value":"34RGIPCCY3Q32KZA","created_at":"2026-05-18T12:26:03Z"},{"alias_kind":"pith_short_8","alias_value":"34RGIPCC","created_at":"2026-05-18T12:26:03Z"}],"graph_snapshots":[{"event_id":"sha256:d84e16cb0fcfc053b15c572649d479cee9e1db1b579ecec77c0cbbad0fb864f7","target":"graph","created_at":"2026-05-18T02:09:21Z","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 use numerical simulations to study the crystallization of monodisperse systems of hard aspherical particles. We find that particle shape and crystallizability can be easily related to each other when particles are characterized in terms of two simple and experimentally accessible order parameters: one based on the particle surface-to-volume ratio, and the other on the angular distribution of the perturbations away from the ideal spherical shape. We present a phase diagram obtained by exploring the crystallizability of 487 different particle shapes across the two-order-parameter spectrum. Fi","authors_text":"Angelo Cacciuto, Behnaz Bozorgui, William L. Miller","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2010-02-01T19:45:16Z","title":"Crystallization of hard aspherical particles"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1002.0316","kind":"arxiv","version":2},"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:baf2c75cb9989eb5b972b557eba05f7e24f61fbbbe474476b6fb115cb9909346","target":"record","created_at":"2026-05-18T02:09:21Z","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":"d6990f4394694d0c4c514e5135217d52f918e34325e57559780411841cf5aef4","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2010-02-01T19:45:16Z","title_canon_sha256":"2870ccf4a3bf205a39114b18e117bce65f749ec64af1d92b76dbda09742d3c44"},"schema_version":"1.0","source":{"id":"1002.0316","kind":"arxiv","version":2}},"canonical_sha256":"df22643c42c6e1bd2b20f7c662f618634321a01e0fec9c7bb3ffa3538e92a0eb","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"df22643c42c6e1bd2b20f7c662f618634321a01e0fec9c7bb3ffa3538e92a0eb","first_computed_at":"2026-05-18T02:09:21.339084Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:09:21.339084Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"FR8HkTTxEh7iM7iB+QALxd+HQtVwkVNv9DopFYpMcvG9uF/QZU3ecteRK/4i3oxjewwFb70Ipds0pYqNG/3pBA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:09:21.339725Z","signed_message":"canonical_sha256_bytes"},"source_id":"1002.0316","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:baf2c75cb9989eb5b972b557eba05f7e24f61fbbbe474476b6fb115cb9909346","sha256:d84e16cb0fcfc053b15c572649d479cee9e1db1b579ecec77c0cbbad0fb864f7"],"state_sha256":"edb4b9309aed0171fd93105ce61ee825c9b81baabf7f50884ddc29732e5813e3"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9T4pHD8vQwIb72Sm4RK4InjIKk4OC/zrKoY8UGa3Pr85X4elb26pG5808nB2C/2YEbKy6vQO6tFtfnaOAGK9BQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T05:04:35.335596Z","bundle_sha256":"0fda022240625cfc5d3341bb52defe9a7cd8ade3729582170ccc6629789f70d7"}}