{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:C5CJBEVXV62GVMJMCGK5XZTQ3P","short_pith_number":"pith:C5CJBEVX","schema_version":"1.0","canonical_sha256":"17449092b7afb46ab12c1195dbe670dbc44f77d89c5ac1558970b17bf68affac","source":{"kind":"arxiv","id":"1505.05224","version":2},"attestation_state":"computed","paper":{"title":"Smooth and fast versus instantaneous quenches in quantum field theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","cond-mat.str-el"],"primary_cat":"hep-th","authors_text":"Dami\\'an A. Galante, Robert C. Myers, Sumit R. Das","submitted_at":"2015-05-20T02:03:20Z","abstract_excerpt":"We examine in detail the relationship between smooth fast quantum quenches, characterized by a time scale $\\delta t$, and {\\em instantaneous quenches}, within the framework of exactly solvable mass quenches in free scalar field theory. Our earlier studies \\cite{dgm1,dgm2} highlighted that the two protocols remain distinct in the limit $\\delta t \\rightarrow 0$ because of the relation of the quench rate to the UV cut-off, i.e., $1/\\delta t\\ll\\Lambda$ always holds in the fast smooth quenches while $1/\\delta t\\sim\\Lambda$ for instantaneous quenches. Here we study UV finite quantities like correlat"},"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":"1505.05224","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-05-20T02:03:20Z","cross_cats_sorted":["cond-mat.stat-mech","cond-mat.str-el"],"title_canon_sha256":"d89aaf52ec89544d78e4075cc8a468408ab837cfc479161c1a4ad46fc35555a7","abstract_canon_sha256":"9a51191e89b088b394ac203c2a369e5ac0d8f861b5c2746ef7b7728b4e0f4454"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:31:38.971462Z","signature_b64":"a2pLUmXpVGRnQggDMbbzgUgr2SNUWOecGIAQt8WvZ6gS0E0Aw0ajixnr5uXJ3GhrtSWL/0uiiyCCVIdILw+vCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"17449092b7afb46ab12c1195dbe670dbc44f77d89c5ac1558970b17bf68affac","last_reissued_at":"2026-05-18T01:31:38.970842Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:31:38.970842Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Smooth and fast versus instantaneous quenches in quantum field theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","cond-mat.str-el"],"primary_cat":"hep-th","authors_text":"Dami\\'an A. Galante, Robert C. Myers, Sumit R. Das","submitted_at":"2015-05-20T02:03:20Z","abstract_excerpt":"We examine in detail the relationship between smooth fast quantum quenches, characterized by a time scale $\\delta t$, and {\\em instantaneous quenches}, within the framework of exactly solvable mass quenches in free scalar field theory. Our earlier studies \\cite{dgm1,dgm2} highlighted that the two protocols remain distinct in the limit $\\delta t \\rightarrow 0$ because of the relation of the quench rate to the UV cut-off, i.e., $1/\\delta t\\ll\\Lambda$ always holds in the fast smooth quenches while $1/\\delta t\\sim\\Lambda$ for instantaneous quenches. Here we study UV finite quantities like correlat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1505.05224","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":"1505.05224","created_at":"2026-05-18T01:31:38.970937+00:00"},{"alias_kind":"arxiv_version","alias_value":"1505.05224v2","created_at":"2026-05-18T01:31:38.970937+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1505.05224","created_at":"2026-05-18T01:31:38.970937+00:00"},{"alias_kind":"pith_short_12","alias_value":"C5CJBEVXV62G","created_at":"2026-05-18T12:29:14.074870+00:00"},{"alias_kind":"pith_short_16","alias_value":"C5CJBEVXV62GVMJM","created_at":"2026-05-18T12:29:14.074870+00:00"},{"alias_kind":"pith_short_8","alias_value":"C5CJBEVX","created_at":"2026-05-18T12:29:14.074870+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/C5CJBEVXV62GVMJMCGK5XZTQ3P","json":"https://pith.science/pith/C5CJBEVXV62GVMJMCGK5XZTQ3P.json","graph_json":"https://pith.science/api/pith-number/C5CJBEVXV62GVMJMCGK5XZTQ3P/graph.json","events_json":"https://pith.science/api/pith-number/C5CJBEVXV62GVMJMCGK5XZTQ3P/events.json","paper":"https://pith.science/paper/C5CJBEVX"},"agent_actions":{"view_html":"https://pith.science/pith/C5CJBEVXV62GVMJMCGK5XZTQ3P","download_json":"https://pith.science/pith/C5CJBEVXV62GVMJMCGK5XZTQ3P.json","view_paper":"https://pith.science/paper/C5CJBEVX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1505.05224&json=true","fetch_graph":"https://pith.science/api/pith-number/C5CJBEVXV62GVMJMCGK5XZTQ3P/graph.json","fetch_events":"https://pith.science/api/pith-number/C5CJBEVXV62GVMJMCGK5XZTQ3P/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/C5CJBEVXV62GVMJMCGK5XZTQ3P/action/timestamp_anchor","attest_storage":"https://pith.science/pith/C5CJBEVXV62GVMJMCGK5XZTQ3P/action/storage_attestation","attest_author":"https://pith.science/pith/C5CJBEVXV62GVMJMCGK5XZTQ3P/action/author_attestation","sign_citation":"https://pith.science/pith/C5CJBEVXV62GVMJMCGK5XZTQ3P/action/citation_signature","submit_replication":"https://pith.science/pith/C5CJBEVXV62GVMJMCGK5XZTQ3P/action/replication_record"}},"created_at":"2026-05-18T01:31:38.970937+00:00","updated_at":"2026-05-18T01:31:38.970937+00:00"}