{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:GJ5BEOOXEDCZ7TDD7OVZFMNDTW","short_pith_number":"pith:GJ5BEOOX","schema_version":"1.0","canonical_sha256":"327a1239d720c59fcc63fbab92b1a39db1191946fcc8a6836d58899b58f10d6e","source":{"kind":"arxiv","id":"0912.0826","version":4},"attestation_state":"computed","paper":{"title":"Quantum black holes with charge, colour, and spin at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-th"],"primary_cat":"hep-ph","authors_text":"Douglas M. Gingrich","submitted_at":"2009-12-04T11:52:33Z","abstract_excerpt":"In low-scale gravity scenarios, quantum black holes could be produced at the Large Hadron Collider (LHC) provided the Planck scale is not higher than a few TeV. Based on fundamental principles and a few basic assumptions, we have constructed a model for quantum black hole production and decay in proton-proton collisions. By performing a detailed particle-level simulation at LHC energies, we have estimated cross sections and branching fractions for final-state particle topologies that would uniquely identify quantum black holes in LHC detectors. If the Planck scale is about a TeV, even with the"},"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":"0912.0826","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-12-04T11:52:33Z","cross_cats_sorted":["gr-qc","hep-th"],"title_canon_sha256":"96b7cd6b0db3d134bc737dc0f6210d095379f1326f1d5786c2ff149bb63a8549","abstract_canon_sha256":"91c7ed2f6908b31ba912790e24007e760484625c51d646577751bd631308722e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:34:02.306469Z","signature_b64":"x1ew6mO21lxUWfu7xZv5TzRWsunTiKmjBnL5n4Jv4YL/rgqNSWBxt6qp07eSxBBHWdEiJk+D9kYhNhSgN0DpCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"327a1239d720c59fcc63fbab92b1a39db1191946fcc8a6836d58899b58f10d6e","last_reissued_at":"2026-05-18T02:34:02.306001Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:34:02.306001Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum black holes with charge, colour, and spin at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-th"],"primary_cat":"hep-ph","authors_text":"Douglas M. Gingrich","submitted_at":"2009-12-04T11:52:33Z","abstract_excerpt":"In low-scale gravity scenarios, quantum black holes could be produced at the Large Hadron Collider (LHC) provided the Planck scale is not higher than a few TeV. Based on fundamental principles and a few basic assumptions, we have constructed a model for quantum black hole production and decay in proton-proton collisions. By performing a detailed particle-level simulation at LHC energies, we have estimated cross sections and branching fractions for final-state particle topologies that would uniquely identify quantum black holes in LHC detectors. If the Planck scale is about a TeV, even with the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0912.0826","kind":"arxiv","version":4},"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":"0912.0826","created_at":"2026-05-18T02:34:02.306072+00:00"},{"alias_kind":"arxiv_version","alias_value":"0912.0826v4","created_at":"2026-05-18T02:34:02.306072+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0912.0826","created_at":"2026-05-18T02:34:02.306072+00:00"},{"alias_kind":"pith_short_12","alias_value":"GJ5BEOOXEDCZ","created_at":"2026-05-18T12:25:59.703012+00:00"},{"alias_kind":"pith_short_16","alias_value":"GJ5BEOOXEDCZ7TDD","created_at":"2026-05-18T12:25:59.703012+00:00"},{"alias_kind":"pith_short_8","alias_value":"GJ5BEOOX","created_at":"2026-05-18T12:25:59.703012+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.19495","citing_title":"Search for quantum black holes in lepton+jet final states using proton-proton collisions at $\\sqrt{s}=13.6$ TeV with the ATLAS detector","ref_index":4,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GJ5BEOOXEDCZ7TDD7OVZFMNDTW","json":"https://pith.science/pith/GJ5BEOOXEDCZ7TDD7OVZFMNDTW.json","graph_json":"https://pith.science/api/pith-number/GJ5BEOOXEDCZ7TDD7OVZFMNDTW/graph.json","events_json":"https://pith.science/api/pith-number/GJ5BEOOXEDCZ7TDD7OVZFMNDTW/events.json","paper":"https://pith.science/paper/GJ5BEOOX"},"agent_actions":{"view_html":"https://pith.science/pith/GJ5BEOOXEDCZ7TDD7OVZFMNDTW","download_json":"https://pith.science/pith/GJ5BEOOXEDCZ7TDD7OVZFMNDTW.json","view_paper":"https://pith.science/paper/GJ5BEOOX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0912.0826&json=true","fetch_graph":"https://pith.science/api/pith-number/GJ5BEOOXEDCZ7TDD7OVZFMNDTW/graph.json","fetch_events":"https://pith.science/api/pith-number/GJ5BEOOXEDCZ7TDD7OVZFMNDTW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GJ5BEOOXEDCZ7TDD7OVZFMNDTW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GJ5BEOOXEDCZ7TDD7OVZFMNDTW/action/storage_attestation","attest_author":"https://pith.science/pith/GJ5BEOOXEDCZ7TDD7OVZFMNDTW/action/author_attestation","sign_citation":"https://pith.science/pith/GJ5BEOOXEDCZ7TDD7OVZFMNDTW/action/citation_signature","submit_replication":"https://pith.science/pith/GJ5BEOOXEDCZ7TDD7OVZFMNDTW/action/replication_record"}},"created_at":"2026-05-18T02:34:02.306072+00:00","updated_at":"2026-05-18T02:34:02.306072+00:00"}