{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:HJDBB2JU37LQ2VE66C5TQHJF4A","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":"1c95348d6b60425a6dc7e65ac19e23de4577e8e85c9ef9f0218bca78b850beb0","cross_cats_sorted":["cond-mat.other"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2012-01-11T22:41:06Z","title_canon_sha256":"07bbf2667225484c4389727e8be2dc07708a38ed06355757ef4e43fbab891ad1"},"schema_version":"1.0","source":{"id":"1201.2437","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.2437","created_at":"2026-05-18T04:04:44Z"},{"alias_kind":"arxiv_version","alias_value":"1201.2437v1","created_at":"2026-05-18T04:04:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.2437","created_at":"2026-05-18T04:04:44Z"},{"alias_kind":"pith_short_12","alias_value":"HJDBB2JU37LQ","created_at":"2026-05-18T12:27:09Z"},{"alias_kind":"pith_short_16","alias_value":"HJDBB2JU37LQ2VE6","created_at":"2026-05-18T12:27:09Z"},{"alias_kind":"pith_short_8","alias_value":"HJDBB2JU","created_at":"2026-05-18T12:27:09Z"}],"graph_snapshots":[{"event_id":"sha256:c949ce1214ecd26ed0c2a0950ef2b5ec5d4d117ecd68d533c66f4d7cdfa40332","target":"graph","created_at":"2026-05-18T04:04:44Z","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"},"paper":{"abstract_excerpt":"High energy materials such as polymer bonded explosives are commonly used as propellants. These particulate composites contain explosive crystals suspended in a rubbery binder. However, the explosive nature of these materials limits the determination of their mechanical properties by experimental means. Therefore micromechanics-based methods for the determination of the effective thermoelastic properties of polymer bonded explosives are investigated in this research. Polymer bonded explosives are two-component particulate composites with high volume fractions of particles (volume fraction $>$ ","authors_text":"Biswajit Banerjee, Daniel O. Adams","cross_cats":["cond-mat.other"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2012-01-11T22:41:06Z","title":"Micromechanics-based prediction of thermoelastic properties of high energy materials"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.2437","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:e9b08b5005d703edafe8417f78826023cef71b48fd40791829603f2f747443f3","target":"record","created_at":"2026-05-18T04:04:44Z","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":"1c95348d6b60425a6dc7e65ac19e23de4577e8e85c9ef9f0218bca78b850beb0","cross_cats_sorted":["cond-mat.other"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2012-01-11T22:41:06Z","title_canon_sha256":"07bbf2667225484c4389727e8be2dc07708a38ed06355757ef4e43fbab891ad1"},"schema_version":"1.0","source":{"id":"1201.2437","kind":"arxiv","version":1}},"canonical_sha256":"3a4610e934dfd70d549ef0bb381d25e00cf6e960064994dc6976405c099d0cf0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3a4610e934dfd70d549ef0bb381d25e00cf6e960064994dc6976405c099d0cf0","first_computed_at":"2026-05-18T04:04:44.425722Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:04:44.425722Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"SBNnyayNC1YStT+tqxs5qdmk0ehFL8lmnQYR0Zbh1Xggps6e82oDFu+MXeMj74Kddpym6EeBtnQL9NfvmR4FAA==","signature_status":"signed_v1","signed_at":"2026-05-18T04:04:44.426457Z","signed_message":"canonical_sha256_bytes"},"source_id":"1201.2437","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e9b08b5005d703edafe8417f78826023cef71b48fd40791829603f2f747443f3","sha256:c949ce1214ecd26ed0c2a0950ef2b5ec5d4d117ecd68d533c66f4d7cdfa40332"],"state_sha256":"886f79ac8e707845ca143905674a1c0eae3215607049c39def7f269405ca5d6c"}