{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:QG7XP64JR6RFV4D3XW723PRAK5","short_pith_number":"pith:QG7XP64J","schema_version":"1.0","canonical_sha256":"81bf77fb898fa25af07bbdbfadbe205779d6be3528eb005efed9efea7185e34e","source":{"kind":"arxiv","id":"1601.04420","version":1},"attestation_state":"computed","paper":{"title":"Non-Relativistic Anti-Snyder Model and Some Applications","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Chee Leong Ching, Cheng Xun Yeo, Wei Khim Ng","submitted_at":"2016-01-18T07:48:41Z","abstract_excerpt":"We examine the (2+1)-dimensional Dirac equation in a homogeneous magnetic field under the non-relativistic anti-Snyder model which is relevant to deformed special relativity (DSR) since it exhibits an intrinsic upper bound of the momentum of free particles. After setting up the formalism, exact eigen solutions are derived in momentum space representation and they are expressed in terms of finite orthogonal Romanovski polynomials. There is a finite maximum number of allowable bound states due to the orthogonality of the polynomials and the maximum energy is truncated at the maximum n. Similar t"},"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":"1601.04420","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2016-01-18T07:48:41Z","cross_cats_sorted":[],"title_canon_sha256":"86d6f8af480c8def4a70f9f49d76acac6bddf17f7ef5e47ebbb638a7f1615c3c","abstract_canon_sha256":"ef1dd21ee3401151797bb317e27d6c39f615ded4e7560c22c80cb3b828f54642"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:53:17.700436Z","signature_b64":"K97NKvp/uoXz5rAl2j/Ohjpb2SlpZgfeN1xFrBYLZBf8BpBXkUuJtcdOLBfITCuI7xtSEU7fBKSXJs0x5fdcAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"81bf77fb898fa25af07bbdbfadbe205779d6be3528eb005efed9efea7185e34e","last_reissued_at":"2026-05-18T00:53:17.699837Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:53:17.699837Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-Relativistic Anti-Snyder Model and Some Applications","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Chee Leong Ching, Cheng Xun Yeo, Wei Khim Ng","submitted_at":"2016-01-18T07:48:41Z","abstract_excerpt":"We examine the (2+1)-dimensional Dirac equation in a homogeneous magnetic field under the non-relativistic anti-Snyder model which is relevant to deformed special relativity (DSR) since it exhibits an intrinsic upper bound of the momentum of free particles. After setting up the formalism, exact eigen solutions are derived in momentum space representation and they are expressed in terms of finite orthogonal Romanovski polynomials. There is a finite maximum number of allowable bound states due to the orthogonality of the polynomials and the maximum energy is truncated at the maximum n. Similar t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1601.04420","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":"1601.04420","created_at":"2026-05-18T00:53:17.699922+00:00"},{"alias_kind":"arxiv_version","alias_value":"1601.04420v1","created_at":"2026-05-18T00:53:17.699922+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1601.04420","created_at":"2026-05-18T00:53:17.699922+00:00"},{"alias_kind":"pith_short_12","alias_value":"QG7XP64JR6RF","created_at":"2026-05-18T12:30:39.010887+00:00"},{"alias_kind":"pith_short_16","alias_value":"QG7XP64JR6RFV4D3","created_at":"2026-05-18T12:30:39.010887+00:00"},{"alias_kind":"pith_short_8","alias_value":"QG7XP64J","created_at":"2026-05-18T12:30:39.010887+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/QG7XP64JR6RFV4D3XW723PRAK5","json":"https://pith.science/pith/QG7XP64JR6RFV4D3XW723PRAK5.json","graph_json":"https://pith.science/api/pith-number/QG7XP64JR6RFV4D3XW723PRAK5/graph.json","events_json":"https://pith.science/api/pith-number/QG7XP64JR6RFV4D3XW723PRAK5/events.json","paper":"https://pith.science/paper/QG7XP64J"},"agent_actions":{"view_html":"https://pith.science/pith/QG7XP64JR6RFV4D3XW723PRAK5","download_json":"https://pith.science/pith/QG7XP64JR6RFV4D3XW723PRAK5.json","view_paper":"https://pith.science/paper/QG7XP64J","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1601.04420&json=true","fetch_graph":"https://pith.science/api/pith-number/QG7XP64JR6RFV4D3XW723PRAK5/graph.json","fetch_events":"https://pith.science/api/pith-number/QG7XP64JR6RFV4D3XW723PRAK5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QG7XP64JR6RFV4D3XW723PRAK5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QG7XP64JR6RFV4D3XW723PRAK5/action/storage_attestation","attest_author":"https://pith.science/pith/QG7XP64JR6RFV4D3XW723PRAK5/action/author_attestation","sign_citation":"https://pith.science/pith/QG7XP64JR6RFV4D3XW723PRAK5/action/citation_signature","submit_replication":"https://pith.science/pith/QG7XP64JR6RFV4D3XW723PRAK5/action/replication_record"}},"created_at":"2026-05-18T00:53:17.699922+00:00","updated_at":"2026-05-18T00:53:17.699922+00:00"}