{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:R2A2CKVHFHR6FB7VJIPILFJ7R7","short_pith_number":"pith:R2A2CKVH","schema_version":"1.0","canonical_sha256":"8e81a12aa729e3e287f54a1e85953f8fc7414068c15ed3fb90d2a1f002f89159","source":{"kind":"arxiv","id":"1109.6298","version":2},"attestation_state":"computed","paper":{"title":"Supersonic Velocities in Noncommutative Acoustic Black Holes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-ph"],"primary_cat":"hep-th","authors_text":"E. Passos, F.A. Brito, M. A. Anacleto","submitted_at":"2011-09-28T19:04:00Z","abstract_excerpt":"In this paper we derive Schwarzschild and Kerr - like noncommutative acoustic black hole metrics in the (3+1)-dimensional noncommutative Abelian Higgs model. We have found that the changing in the Hawking temperature T_H due to spacetime noncommutativity account for supersonic velocities and analogously may also account for superluminal particles in the general form (v-c)/c=\\Delta T_H/8T_H. Assuming this form is also valid for gravitational black holes and particle physics, we have found that for \\Delta T_H about the heaviest muon neutrino mass and T_H about proton mass gives 2.12\\times 10-5 w"},"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":"1109.6298","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-09-28T19:04:00Z","cross_cats_sorted":["gr-qc","hep-ph"],"title_canon_sha256":"e11d1293d89cbac56e7a8f9d923b69e2a47a17af3538ed849f72c91af4dedda4","abstract_canon_sha256":"68104abeb2d95f38e2f755a479777c6b58b5e37c0732e99ba8ac194d9854de5f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:03:56.814674Z","signature_b64":"7+6yW796WTWci9AM16n19oatRl2UWzJqV4PeWElZphZUWA+zh3zPbOp9btpKR2CHMmqmw6IscU4ujQMx0Y3iDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8e81a12aa729e3e287f54a1e85953f8fc7414068c15ed3fb90d2a1f002f89159","last_reissued_at":"2026-05-18T04:03:56.814141Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:03:56.814141Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Supersonic Velocities in Noncommutative Acoustic Black Holes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-ph"],"primary_cat":"hep-th","authors_text":"E. Passos, F.A. Brito, M. A. Anacleto","submitted_at":"2011-09-28T19:04:00Z","abstract_excerpt":"In this paper we derive Schwarzschild and Kerr - like noncommutative acoustic black hole metrics in the (3+1)-dimensional noncommutative Abelian Higgs model. We have found that the changing in the Hawking temperature T_H due to spacetime noncommutativity account for supersonic velocities and analogously may also account for superluminal particles in the general form (v-c)/c=\\Delta T_H/8T_H. Assuming this form is also valid for gravitational black holes and particle physics, we have found that for \\Delta T_H about the heaviest muon neutrino mass and T_H about proton mass gives 2.12\\times 10-5 w"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1109.6298","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":"1109.6298","created_at":"2026-05-18T04:03:56.814228+00:00"},{"alias_kind":"arxiv_version","alias_value":"1109.6298v2","created_at":"2026-05-18T04:03:56.814228+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1109.6298","created_at":"2026-05-18T04:03:56.814228+00:00"},{"alias_kind":"pith_short_12","alias_value":"R2A2CKVHFHR6","created_at":"2026-05-18T12:26:39.201973+00:00"},{"alias_kind":"pith_short_16","alias_value":"R2A2CKVHFHR6FB7V","created_at":"2026-05-18T12:26:39.201973+00:00"},{"alias_kind":"pith_short_8","alias_value":"R2A2CKVH","created_at":"2026-05-18T12:26:39.201973+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/R2A2CKVHFHR6FB7VJIPILFJ7R7","json":"https://pith.science/pith/R2A2CKVHFHR6FB7VJIPILFJ7R7.json","graph_json":"https://pith.science/api/pith-number/R2A2CKVHFHR6FB7VJIPILFJ7R7/graph.json","events_json":"https://pith.science/api/pith-number/R2A2CKVHFHR6FB7VJIPILFJ7R7/events.json","paper":"https://pith.science/paper/R2A2CKVH"},"agent_actions":{"view_html":"https://pith.science/pith/R2A2CKVHFHR6FB7VJIPILFJ7R7","download_json":"https://pith.science/pith/R2A2CKVHFHR6FB7VJIPILFJ7R7.json","view_paper":"https://pith.science/paper/R2A2CKVH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1109.6298&json=true","fetch_graph":"https://pith.science/api/pith-number/R2A2CKVHFHR6FB7VJIPILFJ7R7/graph.json","fetch_events":"https://pith.science/api/pith-number/R2A2CKVHFHR6FB7VJIPILFJ7R7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/R2A2CKVHFHR6FB7VJIPILFJ7R7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/R2A2CKVHFHR6FB7VJIPILFJ7R7/action/storage_attestation","attest_author":"https://pith.science/pith/R2A2CKVHFHR6FB7VJIPILFJ7R7/action/author_attestation","sign_citation":"https://pith.science/pith/R2A2CKVHFHR6FB7VJIPILFJ7R7/action/citation_signature","submit_replication":"https://pith.science/pith/R2A2CKVHFHR6FB7VJIPILFJ7R7/action/replication_record"}},"created_at":"2026-05-18T04:03:56.814228+00:00","updated_at":"2026-05-18T04:03:56.814228+00:00"}