{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:ZFMIFHSX4DA4YTV3DL6UWAPKRL","short_pith_number":"pith:ZFMIFHSX","schema_version":"1.0","canonical_sha256":"c958829e57e0c1cc4ebb1afd4b01ea8ae66a0d631305b7aebfaabcac5ac1829c","source":{"kind":"arxiv","id":"1501.06335","version":1},"attestation_state":"computed","paper":{"title":"Reverse Monte Carlo modelling: the two distinct routes of calculating the experimental structure factor","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.comp-ph"],"primary_cat":"cond-mat.soft","authors_text":"E.G. Noya, L. Pusztai, L. Temleitner, V. S\\'anchez-Gil","submitted_at":"2015-01-26T11:17:45Z","abstract_excerpt":"Two different Reverse Monte Carlo strategies, 'RMC++' and 'RMCPOW', have been compared for determining the microscopic structure of some liquid and amorphous solid systems on the basis of neutron diffraction measurements. The first, '$g(r)$ route', exploits the isotropic nature of liquids and calculates the total scattering structure factor, $S(Q)$, via a one-dimensional Fourier transform of the radial distribution function. The second, called 'crystallography' route, is based on the direct calculation of $S(Q)$ in the reciprocal space from the atomic positions in the simulation box. We descri"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1501.06335","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2015-01-26T11:17:45Z","cross_cats_sorted":["physics.comp-ph"],"title_canon_sha256":"ed0e16cff87b617d2d6ae2a066a4e24b3739c19ac9b34ec0bcd19a8e0d8a4def","abstract_canon_sha256":"71be1120a2494dcd447c14f4af788c4b24718f954ff82619823c98427f4ad285"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:28:41.735367Z","signature_b64":"GTWCDDfuPw3zcKGjIHFvnZkboB2kqMVS0bKVKYNQwFuSUSjc4d1HwPeQy+/SN4BaeU5zQB2uOsCAYKYvMH9WAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c958829e57e0c1cc4ebb1afd4b01ea8ae66a0d631305b7aebfaabcac5ac1829c","last_reissued_at":"2026-05-18T02:28:41.734913Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:28:41.734913Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Reverse Monte Carlo modelling: the two distinct routes of calculating the experimental structure factor","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.comp-ph"],"primary_cat":"cond-mat.soft","authors_text":"E.G. Noya, L. Pusztai, L. Temleitner, V. S\\'anchez-Gil","submitted_at":"2015-01-26T11:17:45Z","abstract_excerpt":"Two different Reverse Monte Carlo strategies, 'RMC++' and 'RMCPOW', have been compared for determining the microscopic structure of some liquid and amorphous solid systems on the basis of neutron diffraction measurements. The first, '$g(r)$ route', exploits the isotropic nature of liquids and calculates the total scattering structure factor, $S(Q)$, via a one-dimensional Fourier transform of the radial distribution function. The second, called 'crystallography' route, is based on the direct calculation of $S(Q)$ in the reciprocal space from the atomic positions in the simulation box. We descri"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1501.06335","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1501.06335","created_at":"2026-05-18T02:28:41.734981+00:00"},{"alias_kind":"arxiv_version","alias_value":"1501.06335v1","created_at":"2026-05-18T02:28:41.734981+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1501.06335","created_at":"2026-05-18T02:28:41.734981+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZFMIFHSX4DA4","created_at":"2026-05-18T12:29:52.810259+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZFMIFHSX4DA4YTV3","created_at":"2026-05-18T12:29:52.810259+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZFMIFHSX","created_at":"2026-05-18T12:29:52.810259+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZFMIFHSX4DA4YTV3DL6UWAPKRL","json":"https://pith.science/pith/ZFMIFHSX4DA4YTV3DL6UWAPKRL.json","graph_json":"https://pith.science/api/pith-number/ZFMIFHSX4DA4YTV3DL6UWAPKRL/graph.json","events_json":"https://pith.science/api/pith-number/ZFMIFHSX4DA4YTV3DL6UWAPKRL/events.json","paper":"https://pith.science/paper/ZFMIFHSX"},"agent_actions":{"view_html":"https://pith.science/pith/ZFMIFHSX4DA4YTV3DL6UWAPKRL","download_json":"https://pith.science/pith/ZFMIFHSX4DA4YTV3DL6UWAPKRL.json","view_paper":"https://pith.science/paper/ZFMIFHSX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1501.06335&json=true","fetch_graph":"https://pith.science/api/pith-number/ZFMIFHSX4DA4YTV3DL6UWAPKRL/graph.json","fetch_events":"https://pith.science/api/pith-number/ZFMIFHSX4DA4YTV3DL6UWAPKRL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZFMIFHSX4DA4YTV3DL6UWAPKRL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZFMIFHSX4DA4YTV3DL6UWAPKRL/action/storage_attestation","attest_author":"https://pith.science/pith/ZFMIFHSX4DA4YTV3DL6UWAPKRL/action/author_attestation","sign_citation":"https://pith.science/pith/ZFMIFHSX4DA4YTV3DL6UWAPKRL/action/citation_signature","submit_replication":"https://pith.science/pith/ZFMIFHSX4DA4YTV3DL6UWAPKRL/action/replication_record"}},"created_at":"2026-05-18T02:28:41.734981+00:00","updated_at":"2026-05-18T02:28:41.734981+00:00"}