{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:MTQVIVZFBKBDF7SYQIFFCMKG4D","short_pith_number":"pith:MTQVIVZF","schema_version":"1.0","canonical_sha256":"64e15457250a8232fe58820a513146e0c79c2dae81bf662caf9c43f2dfb74879","source":{"kind":"arxiv","id":"2311.09306","version":2},"attestation_state":"computed","paper":{"title":"Pole-Skipping and Chaos in Hot ${\\cal M}$QCD","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["gr-qc","hep-ph"],"primary_cat":"hep-th","authors_text":"Aalok Misra, Gopal Yadav, Shivam Singh Kushwah","submitted_at":"2023-11-15T19:00:46Z","abstract_excerpt":"We address the question of whether thermal QCD at high temperature is chaotic from the ${\\cal M}$ theory dual of QCD-like theories at intermediate coupling as constructed in arXiv: 2004.07259. The equations of motion of the gauge-invariant combination $Z_s(r)$ of scalar metric perturbations is shown to possess an irregular singular point at the horizon radius $r_h$. Very interestingly, at a specific value of the imaginary frequency and momentum used to read off the analogs of the ''Lyapunov exponent'' $\\lambda_L$ and ''butterfly velocity'' $v_b$ not only does $r_h$ become a regular singular po"},"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":"2311.09306","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2023-11-15T19:00:46Z","cross_cats_sorted":["gr-qc","hep-ph"],"title_canon_sha256":"c13b0ab537cee16040a93f89bcc8901ee7051e22915557ffd0e53437d23b1a45","abstract_canon_sha256":"db67c40d91d12229e2665ba33261a208d25f3df438a6e1e419c6aa430f8d9aa0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:05:52.059002Z","signature_b64":"yK+UQGhhyl04fi0mMRlwQCEYmEa6bWOaGfDJGiKi+aiFPDRkU8HKaaizHhlIXQaIdleWKg/pd5NUfnRoBdE5Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"64e15457250a8232fe58820a513146e0c79c2dae81bf662caf9c43f2dfb74879","last_reissued_at":"2026-07-05T08:05:52.058449Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:05:52.058449Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Pole-Skipping and Chaos in Hot ${\\cal M}$QCD","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["gr-qc","hep-ph"],"primary_cat":"hep-th","authors_text":"Aalok Misra, Gopal Yadav, Shivam Singh Kushwah","submitted_at":"2023-11-15T19:00:46Z","abstract_excerpt":"We address the question of whether thermal QCD at high temperature is chaotic from the ${\\cal M}$ theory dual of QCD-like theories at intermediate coupling as constructed in arXiv: 2004.07259. The equations of motion of the gauge-invariant combination $Z_s(r)$ of scalar metric perturbations is shown to possess an irregular singular point at the horizon radius $r_h$. Very interestingly, at a specific value of the imaginary frequency and momentum used to read off the analogs of the ''Lyapunov exponent'' $\\lambda_L$ and ''butterfly velocity'' $v_b$ not only does $r_h$ become a regular singular po"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2311.09306","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2311.09306/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2311.09306","created_at":"2026-07-05T08:05:52.058520+00:00"},{"alias_kind":"arxiv_version","alias_value":"2311.09306v2","created_at":"2026-07-05T08:05:52.058520+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2311.09306","created_at":"2026-07-05T08:05:52.058520+00:00"},{"alias_kind":"pith_short_12","alias_value":"MTQVIVZFBKBD","created_at":"2026-07-05T08:05:52.058520+00:00"},{"alias_kind":"pith_short_16","alias_value":"MTQVIVZFBKBDF7SY","created_at":"2026-07-05T08:05:52.058520+00:00"},{"alias_kind":"pith_short_8","alias_value":"MTQVIVZF","created_at":"2026-07-05T08:05:52.058520+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/MTQVIVZFBKBDF7SYQIFFCMKG4D","json":"https://pith.science/pith/MTQVIVZFBKBDF7SYQIFFCMKG4D.json","graph_json":"https://pith.science/api/pith-number/MTQVIVZFBKBDF7SYQIFFCMKG4D/graph.json","events_json":"https://pith.science/api/pith-number/MTQVIVZFBKBDF7SYQIFFCMKG4D/events.json","paper":"https://pith.science/paper/MTQVIVZF"},"agent_actions":{"view_html":"https://pith.science/pith/MTQVIVZFBKBDF7SYQIFFCMKG4D","download_json":"https://pith.science/pith/MTQVIVZFBKBDF7SYQIFFCMKG4D.json","view_paper":"https://pith.science/paper/MTQVIVZF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2311.09306&json=true","fetch_graph":"https://pith.science/api/pith-number/MTQVIVZFBKBDF7SYQIFFCMKG4D/graph.json","fetch_events":"https://pith.science/api/pith-number/MTQVIVZFBKBDF7SYQIFFCMKG4D/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MTQVIVZFBKBDF7SYQIFFCMKG4D/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MTQVIVZFBKBDF7SYQIFFCMKG4D/action/storage_attestation","attest_author":"https://pith.science/pith/MTQVIVZFBKBDF7SYQIFFCMKG4D/action/author_attestation","sign_citation":"https://pith.science/pith/MTQVIVZFBKBDF7SYQIFFCMKG4D/action/citation_signature","submit_replication":"https://pith.science/pith/MTQVIVZFBKBDF7SYQIFFCMKG4D/action/replication_record"}},"created_at":"2026-07-05T08:05:52.058520+00:00","updated_at":"2026-07-05T08:05:52.058520+00:00"}