{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:NTOBSSKI3LUTZRO6XJGCDR3KV3","short_pith_number":"pith:NTOBSSKI","schema_version":"1.0","canonical_sha256":"6cdc194948dae93cc5deba4c21c76aaedfa39a31aee9988223f8d267ad24d6b7","source":{"kind":"arxiv","id":"1805.01356","version":1},"attestation_state":"computed","paper":{"title":"Scale-Free Crystallization of two-dimensional Complex Plasmas: Domain Analysis using Minkowski Tensors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.data-an"],"primary_cat":"cond-mat.soft","authors_text":"A. B\\\"obel, C. A. Knapek, C. R\\\"ath","submitted_at":"2018-04-23T07:58:31Z","abstract_excerpt":"Experiments of the recrystallization processes in two-dimensional complex plasmas are analyzed in order to rigorously test a recently developed scale-free phase transition theory. The \"Fractal-Domain-Structure\" (FDS) theory is based on the kinetic theory of Frenkel. It assumes the formation of homogeneous domains, separated by defect lines, during crystallization and a fractal relationship between domain area and boundary length. For the defect number fraction and system energy a scale free power-law relation is predicted. The long range scaling behavior of the bond order correlation function "},"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":"1805.01356","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2018-04-23T07:58:31Z","cross_cats_sorted":["physics.data-an"],"title_canon_sha256":"58d92869efcef1cc364a7a103c421236fa6a31399e372ea5f08b1da129a8f8d3","abstract_canon_sha256":"f07eca9948619f1bae336dafd1d865d1837adb18664947ef3639effd57229f2c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:15:13.651469Z","signature_b64":"5xG+dsPF/aUp+KOWRt6HcCwXrieepfnCOEZiaCQJ7uzUz9X4iPVtglvZ7AX0jLlOJBHj2rOkYJMZkP/lbOvoAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6cdc194948dae93cc5deba4c21c76aaedfa39a31aee9988223f8d267ad24d6b7","last_reissued_at":"2026-05-18T00:15:13.650753Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:15:13.650753Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Scale-Free Crystallization of two-dimensional Complex Plasmas: Domain Analysis using Minkowski Tensors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.data-an"],"primary_cat":"cond-mat.soft","authors_text":"A. B\\\"obel, C. A. Knapek, C. R\\\"ath","submitted_at":"2018-04-23T07:58:31Z","abstract_excerpt":"Experiments of the recrystallization processes in two-dimensional complex plasmas are analyzed in order to rigorously test a recently developed scale-free phase transition theory. The \"Fractal-Domain-Structure\" (FDS) theory is based on the kinetic theory of Frenkel. It assumes the formation of homogeneous domains, separated by defect lines, during crystallization and a fractal relationship between domain area and boundary length. For the defect number fraction and system energy a scale free power-law relation is predicted. The long range scaling behavior of the bond order correlation function "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.01356","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":"1805.01356","created_at":"2026-05-18T00:15:13.650883+00:00"},{"alias_kind":"arxiv_version","alias_value":"1805.01356v1","created_at":"2026-05-18T00:15:13.650883+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.01356","created_at":"2026-05-18T00:15:13.650883+00:00"},{"alias_kind":"pith_short_12","alias_value":"NTOBSSKI3LUT","created_at":"2026-05-18T12:32:40.477152+00:00"},{"alias_kind":"pith_short_16","alias_value":"NTOBSSKI3LUTZRO6","created_at":"2026-05-18T12:32:40.477152+00:00"},{"alias_kind":"pith_short_8","alias_value":"NTOBSSKI","created_at":"2026-05-18T12:32:40.477152+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/NTOBSSKI3LUTZRO6XJGCDR3KV3","json":"https://pith.science/pith/NTOBSSKI3LUTZRO6XJGCDR3KV3.json","graph_json":"https://pith.science/api/pith-number/NTOBSSKI3LUTZRO6XJGCDR3KV3/graph.json","events_json":"https://pith.science/api/pith-number/NTOBSSKI3LUTZRO6XJGCDR3KV3/events.json","paper":"https://pith.science/paper/NTOBSSKI"},"agent_actions":{"view_html":"https://pith.science/pith/NTOBSSKI3LUTZRO6XJGCDR3KV3","download_json":"https://pith.science/pith/NTOBSSKI3LUTZRO6XJGCDR3KV3.json","view_paper":"https://pith.science/paper/NTOBSSKI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1805.01356&json=true","fetch_graph":"https://pith.science/api/pith-number/NTOBSSKI3LUTZRO6XJGCDR3KV3/graph.json","fetch_events":"https://pith.science/api/pith-number/NTOBSSKI3LUTZRO6XJGCDR3KV3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NTOBSSKI3LUTZRO6XJGCDR3KV3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NTOBSSKI3LUTZRO6XJGCDR3KV3/action/storage_attestation","attest_author":"https://pith.science/pith/NTOBSSKI3LUTZRO6XJGCDR3KV3/action/author_attestation","sign_citation":"https://pith.science/pith/NTOBSSKI3LUTZRO6XJGCDR3KV3/action/citation_signature","submit_replication":"https://pith.science/pith/NTOBSSKI3LUTZRO6XJGCDR3KV3/action/replication_record"}},"created_at":"2026-05-18T00:15:13.650883+00:00","updated_at":"2026-05-18T00:15:13.650883+00:00"}