{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:FTKJ3KKHG7AXRXIRNAFKN4J2CX","short_pith_number":"pith:FTKJ3KKH","schema_version":"1.0","canonical_sha256":"2cd49da94737c178dd11680aa6f13a15e0ce8f9601fe284f4da8a87b158ca41f","source":{"kind":"arxiv","id":"1511.01877","version":2},"attestation_state":"computed","paper":{"title":"An alternative way to explain how non-commutativity arises in the bosonic string theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"C. Neves, M. A. De Andrade","submitted_at":"2015-11-05T20:04:24Z","abstract_excerpt":"In this work we will investigate how the non-commutativity arises into the string theory, \\textit{i.e.}, how the bosonic string theory attaches to a D3-brane in the presence of magnetic fields. In order to accomplish the proposal, we departure from the commutative two-dimensional harmonic oscillator, which after the application of the general Bopp's shifts Matrix Method, the non-commutative version of the two-dimensional harmonic oscillator is obtained. After that, this non-commutative harmonic oscillator will be mapped into the bosonic string theory in the light cone frame, which it now appea"},"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":"1511.01877","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-11-05T20:04:24Z","cross_cats_sorted":[],"title_canon_sha256":"4a29dac11259913b5fc1db6bef818ca83c8d827d43cd5b61ccb05cc77e096188","abstract_canon_sha256":"c3fc2d1b9a20697936329567d7f2f9a79b109601d772688844fc42cedb736f3d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:25:33.361893Z","signature_b64":"A8MZxnShPpkhCFHtGUeKJJU1y10pimzUogS38UmO8BjUcODGO0aJbhuHFGvJRp5b9RF5dcKook8/H9mwfapWCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2cd49da94737c178dd11680aa6f13a15e0ce8f9601fe284f4da8a87b158ca41f","last_reissued_at":"2026-05-18T01:25:33.361402Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:25:33.361402Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"An alternative way to explain how non-commutativity arises in the bosonic string theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"C. Neves, M. A. De Andrade","submitted_at":"2015-11-05T20:04:24Z","abstract_excerpt":"In this work we will investigate how the non-commutativity arises into the string theory, \\textit{i.e.}, how the bosonic string theory attaches to a D3-brane in the presence of magnetic fields. In order to accomplish the proposal, we departure from the commutative two-dimensional harmonic oscillator, which after the application of the general Bopp's shifts Matrix Method, the non-commutative version of the two-dimensional harmonic oscillator is obtained. After that, this non-commutative harmonic oscillator will be mapped into the bosonic string theory in the light cone frame, which it now appea"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.01877","kind":"arxiv","version":2},"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":"1511.01877","created_at":"2026-05-18T01:25:33.361477+00:00"},{"alias_kind":"arxiv_version","alias_value":"1511.01877v2","created_at":"2026-05-18T01:25:33.361477+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.01877","created_at":"2026-05-18T01:25:33.361477+00:00"},{"alias_kind":"pith_short_12","alias_value":"FTKJ3KKHG7AX","created_at":"2026-05-18T12:29:22.688609+00:00"},{"alias_kind":"pith_short_16","alias_value":"FTKJ3KKHG7AXRXIR","created_at":"2026-05-18T12:29:22.688609+00:00"},{"alias_kind":"pith_short_8","alias_value":"FTKJ3KKH","created_at":"2026-05-18T12:29:22.688609+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/FTKJ3KKHG7AXRXIRNAFKN4J2CX","json":"https://pith.science/pith/FTKJ3KKHG7AXRXIRNAFKN4J2CX.json","graph_json":"https://pith.science/api/pith-number/FTKJ3KKHG7AXRXIRNAFKN4J2CX/graph.json","events_json":"https://pith.science/api/pith-number/FTKJ3KKHG7AXRXIRNAFKN4J2CX/events.json","paper":"https://pith.science/paper/FTKJ3KKH"},"agent_actions":{"view_html":"https://pith.science/pith/FTKJ3KKHG7AXRXIRNAFKN4J2CX","download_json":"https://pith.science/pith/FTKJ3KKHG7AXRXIRNAFKN4J2CX.json","view_paper":"https://pith.science/paper/FTKJ3KKH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1511.01877&json=true","fetch_graph":"https://pith.science/api/pith-number/FTKJ3KKHG7AXRXIRNAFKN4J2CX/graph.json","fetch_events":"https://pith.science/api/pith-number/FTKJ3KKHG7AXRXIRNAFKN4J2CX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FTKJ3KKHG7AXRXIRNAFKN4J2CX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FTKJ3KKHG7AXRXIRNAFKN4J2CX/action/storage_attestation","attest_author":"https://pith.science/pith/FTKJ3KKHG7AXRXIRNAFKN4J2CX/action/author_attestation","sign_citation":"https://pith.science/pith/FTKJ3KKHG7AXRXIRNAFKN4J2CX/action/citation_signature","submit_replication":"https://pith.science/pith/FTKJ3KKHG7AXRXIRNAFKN4J2CX/action/replication_record"}},"created_at":"2026-05-18T01:25:33.361477+00:00","updated_at":"2026-05-18T01:25:33.361477+00:00"}