{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:I4JQN3BLVPECXIZLKQMWBLXUQ7","short_pith_number":"pith:I4JQN3BL","schema_version":"1.0","canonical_sha256":"471306ec2babc82ba32b541960aef487db41b629fe9c0e347b730db9d8aec459","source":{"kind":"arxiv","id":"hep-ph/0510052","version":2},"attestation_state":"computed","paper":{"title":"Non-Perturbative Quark-Antiquark Production From a Constant Chromo-Electric Field via the Schwinger Mechanism","license":"","headline":"","cross_cats":["hep-lat","hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Gouranga C. Nayak (SUNY, Stony Brook)","submitted_at":"2005-10-05T00:32:01Z","abstract_excerpt":"We obtain an exact result for the non-perturbative quark (antiquark) production rate and its p_T distribution from a constant SU(3) chromo-electric field E^a with arbitary color index $a$ by directly evaluating the path integral. Unlike the WKB tunneling result, which depends only on one gauge invariant quantity |E|, the strength of the chromo-electric field, we find that the exact result for the p_T distribution for quark (antiquark) production rate depends on two independent Casimir (gauge) invariants, E^aE^a and [d_{abc}E^aE^bE^c]^2."},"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":"hep-ph/0510052","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2005-10-05T00:32:01Z","cross_cats_sorted":["hep-lat","hep-th","nucl-th"],"title_canon_sha256":"8f699d1ccbb453a29ab4cd59067079bfccae7aa613b415d9e3260533c8999210","abstract_canon_sha256":"0ed0266c684ce1ba47fccea0cd52e9ad0ee1b7f241010d49ed9f2fe37b108233"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:55:50.951352Z","signature_b64":"cJYU/eRJaIaU+ajA2d5mSPuXN9RmxOFcMP2V6W4Vi6YVDGaxCazyac0mHoaaME3JMGrTBRCgyRDrtpklhBRyDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"471306ec2babc82ba32b541960aef487db41b629fe9c0e347b730db9d8aec459","last_reissued_at":"2026-07-04T16:55:50.950991Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:55:50.950991Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-Perturbative Quark-Antiquark Production From a Constant Chromo-Electric Field via the Schwinger Mechanism","license":"","headline":"","cross_cats":["hep-lat","hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Gouranga C. Nayak (SUNY, Stony Brook)","submitted_at":"2005-10-05T00:32:01Z","abstract_excerpt":"We obtain an exact result for the non-perturbative quark (antiquark) production rate and its p_T distribution from a constant SU(3) chromo-electric field E^a with arbitary color index $a$ by directly evaluating the path integral. Unlike the WKB tunneling result, which depends only on one gauge invariant quantity |E|, the strength of the chromo-electric field, we find that the exact result for the p_T distribution for quark (antiquark) production rate depends on two independent Casimir (gauge) invariants, E^aE^a and [d_{abc}E^aE^bE^c]^2."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0510052","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/hep-ph/0510052/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":"hep-ph/0510052","created_at":"2026-07-04T16:55:50.951054+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0510052v2","created_at":"2026-07-04T16:55:50.951054+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0510052","created_at":"2026-07-04T16:55:50.951054+00:00"},{"alias_kind":"pith_short_12","alias_value":"I4JQN3BLVPEC","created_at":"2026-07-04T16:55:50.951054+00:00"},{"alias_kind":"pith_short_16","alias_value":"I4JQN3BLVPECXIZL","created_at":"2026-07-04T16:55:50.951054+00:00"},{"alias_kind":"pith_short_8","alias_value":"I4JQN3BL","created_at":"2026-07-04T16:55:50.951054+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2608.13393","citing_title":"Non-perturbative quark production and transport in the evolving glasma: the WAGASHI event generator","ref_index":42,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/I4JQN3BLVPECXIZLKQMWBLXUQ7","json":"https://pith.science/pith/I4JQN3BLVPECXIZLKQMWBLXUQ7.json","graph_json":"https://pith.science/api/pith-number/I4JQN3BLVPECXIZLKQMWBLXUQ7/graph.json","events_json":"https://pith.science/api/pith-number/I4JQN3BLVPECXIZLKQMWBLXUQ7/events.json","paper":"https://pith.science/paper/I4JQN3BL"},"agent_actions":{"view_html":"https://pith.science/pith/I4JQN3BLVPECXIZLKQMWBLXUQ7","download_json":"https://pith.science/pith/I4JQN3BLVPECXIZLKQMWBLXUQ7.json","view_paper":"https://pith.science/paper/I4JQN3BL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0510052&json=true","fetch_graph":"https://pith.science/api/pith-number/I4JQN3BLVPECXIZLKQMWBLXUQ7/graph.json","fetch_events":"https://pith.science/api/pith-number/I4JQN3BLVPECXIZLKQMWBLXUQ7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/I4JQN3BLVPECXIZLKQMWBLXUQ7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/I4JQN3BLVPECXIZLKQMWBLXUQ7/action/storage_attestation","attest_author":"https://pith.science/pith/I4JQN3BLVPECXIZLKQMWBLXUQ7/action/author_attestation","sign_citation":"https://pith.science/pith/I4JQN3BLVPECXIZLKQMWBLXUQ7/action/citation_signature","submit_replication":"https://pith.science/pith/I4JQN3BLVPECXIZLKQMWBLXUQ7/action/replication_record"}},"created_at":"2026-07-04T16:55:50.951054+00:00","updated_at":"2026-07-04T16:55:50.951054+00:00"}