{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:DNHEOUBM7XUQKJBHF5O7EBOF2Z","short_pith_number":"pith:DNHEOUBM","schema_version":"1.0","canonical_sha256":"1b4e47502cfde90524272f5df205c5d65a4ad74fee31853ae68df29fbd4010e6","source":{"kind":"arxiv","id":"1809.01681","version":1},"attestation_state":"computed","paper":{"title":"Cooling arbitrary near-critical systems using hyperbolic quenches","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.stat-mech","authors_text":"Kartiek Agarwal, Matteo Ippoliti, Prahar Mitra, R. N. Bhatt, S. L. Sondhi","submitted_at":"2018-09-05T18:15:45Z","abstract_excerpt":"We describe a quench protocol that allows the rapid preparation of ground states of arbitrary interacting conformal field theories in $1+1$ dimensions. We start from the ground state of a related gapped relativistic quantum field theory and consider sudden quenches along the space-like trajectories $t^2 - x^2 = T^2_0$ (parameterized by $T_0$) to a conformal field theory. Using only arguments of symmetry and conformal invariance, we show that the post-quench stress-energy tensor of the conformal field theory is uniquely constrained up to an overall scaling factor. Crucially, the $\\textit{geomet"},"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":"1809.01681","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-09-05T18:15:45Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"8c746d9826d3bad94249fd67f1dab22d03055f5ee08b6db9a862970ac55e46cb","abstract_canon_sha256":"9787eb21d6bf0721de8b7448af49b8e63d2cf4f8f88ac6ceda56236684123cc2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:49:43.047526Z","signature_b64":"3Jigi9VXSEIaENUVRmMd7hpbY7N0iJioZIWSAyvdlDGegDwIwouZ1/cn4rHEjtpaMzbxQAS16OJnjHXtZdyaDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1b4e47502cfde90524272f5df205c5d65a4ad74fee31853ae68df29fbd4010e6","last_reissued_at":"2026-05-17T23:49:43.047010Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:49:43.047010Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Cooling arbitrary near-critical systems using hyperbolic quenches","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.stat-mech","authors_text":"Kartiek Agarwal, Matteo Ippoliti, Prahar Mitra, R. N. Bhatt, S. L. Sondhi","submitted_at":"2018-09-05T18:15:45Z","abstract_excerpt":"We describe a quench protocol that allows the rapid preparation of ground states of arbitrary interacting conformal field theories in $1+1$ dimensions. We start from the ground state of a related gapped relativistic quantum field theory and consider sudden quenches along the space-like trajectories $t^2 - x^2 = T^2_0$ (parameterized by $T_0$) to a conformal field theory. Using only arguments of symmetry and conformal invariance, we show that the post-quench stress-energy tensor of the conformal field theory is uniquely constrained up to an overall scaling factor. Crucially, the $\\textit{geomet"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1809.01681","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":"1809.01681","created_at":"2026-05-17T23:49:43.047104+00:00"},{"alias_kind":"arxiv_version","alias_value":"1809.01681v1","created_at":"2026-05-17T23:49:43.047104+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1809.01681","created_at":"2026-05-17T23:49:43.047104+00:00"},{"alias_kind":"pith_short_12","alias_value":"DNHEOUBM7XUQ","created_at":"2026-05-18T12:32:19.392346+00:00"},{"alias_kind":"pith_short_16","alias_value":"DNHEOUBM7XUQKJBH","created_at":"2026-05-18T12:32:19.392346+00:00"},{"alias_kind":"pith_short_8","alias_value":"DNHEOUBM","created_at":"2026-05-18T12:32:19.392346+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/DNHEOUBM7XUQKJBHF5O7EBOF2Z","json":"https://pith.science/pith/DNHEOUBM7XUQKJBHF5O7EBOF2Z.json","graph_json":"https://pith.science/api/pith-number/DNHEOUBM7XUQKJBHF5O7EBOF2Z/graph.json","events_json":"https://pith.science/api/pith-number/DNHEOUBM7XUQKJBHF5O7EBOF2Z/events.json","paper":"https://pith.science/paper/DNHEOUBM"},"agent_actions":{"view_html":"https://pith.science/pith/DNHEOUBM7XUQKJBHF5O7EBOF2Z","download_json":"https://pith.science/pith/DNHEOUBM7XUQKJBHF5O7EBOF2Z.json","view_paper":"https://pith.science/paper/DNHEOUBM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1809.01681&json=true","fetch_graph":"https://pith.science/api/pith-number/DNHEOUBM7XUQKJBHF5O7EBOF2Z/graph.json","fetch_events":"https://pith.science/api/pith-number/DNHEOUBM7XUQKJBHF5O7EBOF2Z/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DNHEOUBM7XUQKJBHF5O7EBOF2Z/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DNHEOUBM7XUQKJBHF5O7EBOF2Z/action/storage_attestation","attest_author":"https://pith.science/pith/DNHEOUBM7XUQKJBHF5O7EBOF2Z/action/author_attestation","sign_citation":"https://pith.science/pith/DNHEOUBM7XUQKJBHF5O7EBOF2Z/action/citation_signature","submit_replication":"https://pith.science/pith/DNHEOUBM7XUQKJBHF5O7EBOF2Z/action/replication_record"}},"created_at":"2026-05-17T23:49:43.047104+00:00","updated_at":"2026-05-17T23:49:43.047104+00:00"}