{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:TI626JX6D222RK266KHLIRF3W5","short_pith_number":"pith:TI626JX6","schema_version":"1.0","canonical_sha256":"9a3daf26fe1eb5a8ab5ef28eb444bbb778c6283e50088f5bc5dc7370ebf9dd98","source":{"kind":"arxiv","id":"1607.01938","version":1},"attestation_state":"computed","paper":{"title":"Calculation of x-ray scattering patterns from nanocrystals at high x-ray intensity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atm-clus","authors_text":"Malik Muhammad Abdullah, Robin Santra, Sang-Kil Son, Zoltan Jurek","submitted_at":"2016-07-07T09:45:04Z","abstract_excerpt":"We present a generalized method to describe the x-ray scattering intensity of the Bragg spots in a diffraction pattern from nanocrystals exposed to intense x-ray pulses. Our method involves the subdivision of a crystal into smaller units. In order to calculate the dynamics within every unit we employ a Monte-Carlo (MC)-molecular dynamics (MD)-ab-initio hybrid framework using real space periodic boundary conditions. By combining all the units we simulate the diffraction pattern of a crystal larger than the transverse x-ray beam profile, a situation commonly encountered in femtosecond nanocrysta"},"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":"1607.01938","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atm-clus","submitted_at":"2016-07-07T09:45:04Z","cross_cats_sorted":[],"title_canon_sha256":"a6390bd3bbbfc62e1b814efc27039981337b12a866a21de98ba9f35209b9c570","abstract_canon_sha256":"7e82c8f99db8da0351b58fb5d123e0a13f23dc4684bd6a0e14bdb5c5fa7344b0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:36:51.595223Z","signature_b64":"3xs9v0hUs7XcrbAyH5pBZGms9xyaMYgckwBJ9COx9/y+ROL1lv6Vx91FGpd+qR7j8CVh3e1v2LI13MCRCM7ZCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9a3daf26fe1eb5a8ab5ef28eb444bbb778c6283e50088f5bc5dc7370ebf9dd98","last_reissued_at":"2026-05-18T00:36:51.594604Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:36:51.594604Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Calculation of x-ray scattering patterns from nanocrystals at high x-ray intensity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atm-clus","authors_text":"Malik Muhammad Abdullah, Robin Santra, Sang-Kil Son, Zoltan Jurek","submitted_at":"2016-07-07T09:45:04Z","abstract_excerpt":"We present a generalized method to describe the x-ray scattering intensity of the Bragg spots in a diffraction pattern from nanocrystals exposed to intense x-ray pulses. Our method involves the subdivision of a crystal into smaller units. In order to calculate the dynamics within every unit we employ a Monte-Carlo (MC)-molecular dynamics (MD)-ab-initio hybrid framework using real space periodic boundary conditions. By combining all the units we simulate the diffraction pattern of a crystal larger than the transverse x-ray beam profile, a situation commonly encountered in femtosecond nanocrysta"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1607.01938","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":"1607.01938","created_at":"2026-05-18T00:36:51.594712+00:00"},{"alias_kind":"arxiv_version","alias_value":"1607.01938v1","created_at":"2026-05-18T00:36:51.594712+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1607.01938","created_at":"2026-05-18T00:36:51.594712+00:00"},{"alias_kind":"pith_short_12","alias_value":"TI626JX6D222","created_at":"2026-05-18T12:30:44.179134+00:00"},{"alias_kind":"pith_short_16","alias_value":"TI626JX6D222RK26","created_at":"2026-05-18T12:30:44.179134+00:00"},{"alias_kind":"pith_short_8","alias_value":"TI626JX6","created_at":"2026-05-18T12:30:44.179134+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/TI626JX6D222RK266KHLIRF3W5","json":"https://pith.science/pith/TI626JX6D222RK266KHLIRF3W5.json","graph_json":"https://pith.science/api/pith-number/TI626JX6D222RK266KHLIRF3W5/graph.json","events_json":"https://pith.science/api/pith-number/TI626JX6D222RK266KHLIRF3W5/events.json","paper":"https://pith.science/paper/TI626JX6"},"agent_actions":{"view_html":"https://pith.science/pith/TI626JX6D222RK266KHLIRF3W5","download_json":"https://pith.science/pith/TI626JX6D222RK266KHLIRF3W5.json","view_paper":"https://pith.science/paper/TI626JX6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1607.01938&json=true","fetch_graph":"https://pith.science/api/pith-number/TI626JX6D222RK266KHLIRF3W5/graph.json","fetch_events":"https://pith.science/api/pith-number/TI626JX6D222RK266KHLIRF3W5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TI626JX6D222RK266KHLIRF3W5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TI626JX6D222RK266KHLIRF3W5/action/storage_attestation","attest_author":"https://pith.science/pith/TI626JX6D222RK266KHLIRF3W5/action/author_attestation","sign_citation":"https://pith.science/pith/TI626JX6D222RK266KHLIRF3W5/action/citation_signature","submit_replication":"https://pith.science/pith/TI626JX6D222RK266KHLIRF3W5/action/replication_record"}},"created_at":"2026-05-18T00:36:51.594712+00:00","updated_at":"2026-05-18T00:36:51.594712+00:00"}