{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2000:OAFHHIU7NFUI253CRTAI5CZK3A","short_pith_number":"pith:OAFHHIU7","schema_version":"1.0","canonical_sha256":"700a73a29f69688d77628cc08e8b2ad83b06773f7dbe2896b4cb176aee07cf46","source":{"kind":"arxiv","id":"hep-th/0008096","version":2},"attestation_state":"computed","paper":{"title":"Light-Cone Quantization: Foundations and Applications","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"T. Heinzl (FSU Jena)","submitted_at":"2000-08-11T14:52:56Z","abstract_excerpt":"These lecture notes review the foundations and some applications of light-cone quantization. First I explain how to choose a time in special relativity. Inclusion of Poincare invariance naturally leads to Dirac's forms of relativistic dynamics. Among these, the front form, being the basis for light-cone quantization, is my main focus. I explain a few of its peculiar features such as boost and Galilei invariance or separation of relative and center-of-mass motion. Combining light-cone dynamics and field quantization results in light-cone quantum field theory. As the latter represents a first-or"},"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-th/0008096","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2000-08-11T14:52:56Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"e59d5f3299aa9b7b600c6d850253aa511dc7f1132d81da7c975d9bb9ad0a943b","abstract_canon_sha256":"ed88cc7e87914ac8dec71990e5c57d7925b839ca30263227196e2da5101e18a3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:31:23.910172Z","signature_b64":"xDDEm4hPQ7qb+g8BEM+iPGKeTptt1w0V33dlv2CKjBg5BWhdzvkijBTOp0I6NvKDGy1ogVLZ0EWwj1MWpNm9Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"700a73a29f69688d77628cc08e8b2ad83b06773f7dbe2896b4cb176aee07cf46","last_reissued_at":"2026-07-04T14:31:23.909810Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:31:23.909810Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Light-Cone Quantization: Foundations and Applications","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"T. Heinzl (FSU Jena)","submitted_at":"2000-08-11T14:52:56Z","abstract_excerpt":"These lecture notes review the foundations and some applications of light-cone quantization. First I explain how to choose a time in special relativity. Inclusion of Poincare invariance naturally leads to Dirac's forms of relativistic dynamics. Among these, the front form, being the basis for light-cone quantization, is my main focus. I explain a few of its peculiar features such as boost and Galilei invariance or separation of relative and center-of-mass motion. Combining light-cone dynamics and field quantization results in light-cone quantum field theory. As the latter represents a first-or"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0008096","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-th/0008096/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-th/0008096","created_at":"2026-07-04T14:31:23.909864+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0008096v2","created_at":"2026-07-04T14:31:23.909864+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0008096","created_at":"2026-07-04T14:31:23.909864+00:00"},{"alias_kind":"pith_short_12","alias_value":"OAFHHIU7NFUI","created_at":"2026-07-04T14:31:23.909864+00:00"},{"alias_kind":"pith_short_16","alias_value":"OAFHHIU7NFUI253C","created_at":"2026-07-04T14:31:23.909864+00:00"},{"alias_kind":"pith_short_8","alias_value":"OAFHHIU7","created_at":"2026-07-04T14:31:23.909864+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2605.13804","citing_title":"An algebra of proper observables at null infinity: Dirac brackets, Memory and Goldstone probes","ref_index":15,"is_internal_anchor":true},{"citing_arxiv_id":"2512.21228","citing_title":"Quantum entanglement between partons in a strongly coupled quantum field theory","ref_index":63,"is_internal_anchor":true},{"citing_arxiv_id":"2605.13804","citing_title":"An algebra of proper observables at null infinity: Dirac brackets, Memory and Goldstone probes","ref_index":12,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/OAFHHIU7NFUI253CRTAI5CZK3A","json":"https://pith.science/pith/OAFHHIU7NFUI253CRTAI5CZK3A.json","graph_json":"https://pith.science/api/pith-number/OAFHHIU7NFUI253CRTAI5CZK3A/graph.json","events_json":"https://pith.science/api/pith-number/OAFHHIU7NFUI253CRTAI5CZK3A/events.json","paper":"https://pith.science/paper/OAFHHIU7"},"agent_actions":{"view_html":"https://pith.science/pith/OAFHHIU7NFUI253CRTAI5CZK3A","download_json":"https://pith.science/pith/OAFHHIU7NFUI253CRTAI5CZK3A.json","view_paper":"https://pith.science/paper/OAFHHIU7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0008096&json=true","fetch_graph":"https://pith.science/api/pith-number/OAFHHIU7NFUI253CRTAI5CZK3A/graph.json","fetch_events":"https://pith.science/api/pith-number/OAFHHIU7NFUI253CRTAI5CZK3A/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OAFHHIU7NFUI253CRTAI5CZK3A/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OAFHHIU7NFUI253CRTAI5CZK3A/action/storage_attestation","attest_author":"https://pith.science/pith/OAFHHIU7NFUI253CRTAI5CZK3A/action/author_attestation","sign_citation":"https://pith.science/pith/OAFHHIU7NFUI253CRTAI5CZK3A/action/citation_signature","submit_replication":"https://pith.science/pith/OAFHHIU7NFUI253CRTAI5CZK3A/action/replication_record"}},"created_at":"2026-07-04T14:31:23.909864+00:00","updated_at":"2026-07-04T14:31:23.909864+00:00"}