{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:FXM5U3ZTC7NLLHURQRMGEFYAWV","short_pith_number":"pith:FXM5U3ZT","schema_version":"1.0","canonical_sha256":"2dd9da6f3317dab59e918458621700b57978b5608319e28aa68f9d6ca314bf38","source":{"kind":"arxiv","id":"1408.5067","version":1},"attestation_state":"computed","paper":{"title":"Simulations of an ultracold, neutral plasma with equal masses","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph"],"primary_cat":"physics.plasm-ph","authors_text":"B. J. Bender, F. Robicheaux, M. A. Phillips","submitted_at":"2014-08-21T17:00:33Z","abstract_excerpt":"The results of a theoretical investigation of an ultracold, neutral plasma composed of equal mass positive and negative charges are reported. In our simulations, the plasma is created by the fast dissociation of a neutral particle. The temperature of the plasma is controlled by the relative energy of the dissociation. We studied the early time evolution of this system where the initial energy was tuned so that the plasma is formed in the strongly coupled regime. In particular, we present results on the temperature evolution and three body recombination. In the weakly coupled regime, we studied"},"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":"1408.5067","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2014-08-21T17:00:33Z","cross_cats_sorted":["physics.atom-ph"],"title_canon_sha256":"9b2d274958ce7f3a70171a7eee80ebef9ee50e47ddc33f59a95025ce403941d3","abstract_canon_sha256":"bca671803e84b5e387de75f1a6900e3d5fe931f1fc895d6d0c8a7840723a89f5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:42:15.978677Z","signature_b64":"tC4cMQD+nOlGAHWN7kwpCKqL9wnTUJWDzz+M7EOo9J8cC78362ZoCuzwHVmgr8ALn4mLLBJO5Qn5EN/MnUshCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2dd9da6f3317dab59e918458621700b57978b5608319e28aa68f9d6ca314bf38","last_reissued_at":"2026-05-18T01:42:15.977919Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:42:15.977919Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Simulations of an ultracold, neutral plasma with equal masses","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph"],"primary_cat":"physics.plasm-ph","authors_text":"B. J. Bender, F. Robicheaux, M. A. Phillips","submitted_at":"2014-08-21T17:00:33Z","abstract_excerpt":"The results of a theoretical investigation of an ultracold, neutral plasma composed of equal mass positive and negative charges are reported. In our simulations, the plasma is created by the fast dissociation of a neutral particle. The temperature of the plasma is controlled by the relative energy of the dissociation. We studied the early time evolution of this system where the initial energy was tuned so that the plasma is formed in the strongly coupled regime. In particular, we present results on the temperature evolution and three body recombination. In the weakly coupled regime, we studied"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1408.5067","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":"1408.5067","created_at":"2026-05-18T01:42:15.978032+00:00"},{"alias_kind":"arxiv_version","alias_value":"1408.5067v1","created_at":"2026-05-18T01:42:15.978032+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1408.5067","created_at":"2026-05-18T01:42:15.978032+00:00"},{"alias_kind":"pith_short_12","alias_value":"FXM5U3ZTC7NL","created_at":"2026-05-18T12:28:28.263976+00:00"},{"alias_kind":"pith_short_16","alias_value":"FXM5U3ZTC7NLLHUR","created_at":"2026-05-18T12:28:28.263976+00:00"},{"alias_kind":"pith_short_8","alias_value":"FXM5U3ZT","created_at":"2026-05-18T12:28:28.263976+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/FXM5U3ZTC7NLLHURQRMGEFYAWV","json":"https://pith.science/pith/FXM5U3ZTC7NLLHURQRMGEFYAWV.json","graph_json":"https://pith.science/api/pith-number/FXM5U3ZTC7NLLHURQRMGEFYAWV/graph.json","events_json":"https://pith.science/api/pith-number/FXM5U3ZTC7NLLHURQRMGEFYAWV/events.json","paper":"https://pith.science/paper/FXM5U3ZT"},"agent_actions":{"view_html":"https://pith.science/pith/FXM5U3ZTC7NLLHURQRMGEFYAWV","download_json":"https://pith.science/pith/FXM5U3ZTC7NLLHURQRMGEFYAWV.json","view_paper":"https://pith.science/paper/FXM5U3ZT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1408.5067&json=true","fetch_graph":"https://pith.science/api/pith-number/FXM5U3ZTC7NLLHURQRMGEFYAWV/graph.json","fetch_events":"https://pith.science/api/pith-number/FXM5U3ZTC7NLLHURQRMGEFYAWV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FXM5U3ZTC7NLLHURQRMGEFYAWV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FXM5U3ZTC7NLLHURQRMGEFYAWV/action/storage_attestation","attest_author":"https://pith.science/pith/FXM5U3ZTC7NLLHURQRMGEFYAWV/action/author_attestation","sign_citation":"https://pith.science/pith/FXM5U3ZTC7NLLHURQRMGEFYAWV/action/citation_signature","submit_replication":"https://pith.science/pith/FXM5U3ZTC7NLLHURQRMGEFYAWV/action/replication_record"}},"created_at":"2026-05-18T01:42:15.978032+00:00","updated_at":"2026-05-18T01:42:15.978032+00:00"}